,....,.:... . _ j , .a...;.,. .. . mat-,4: 3 300l URI? Mt»! Micniuuii mate University This is to certify that the dissertation entitled CLUSTERS AND EXTENDED ARRAYS WITH METAL IONS AND NITROGEN DONOR LIGANDS presented by Cristian Saul Campos Fernandez has been accepted towards fulfillment of the requirements for Ph . D . degree in Chemis t ry ! ‘ 335” I Major professor Date glaji 0/ MS U is an Affirmative Action/Equal Opportunity Institution 0-12771 ._.k* ..._. .- .'_ PLACE IN RETURN BOX to remove this checkout from your record. To AVOID FINE return on or before date due. MAY BE RECALLED with earlier due date if requested. DATE DUE DATE DUE DATE DUE 6/01 c:/CIRCIDataDuep65—n15 CLL'STERS A IONS A in pa: CLUSTERS AND EXTENDED ARRAYS WITH METAL IONS AND NITROGEN DONOR LIGANDS By Cristian Saul Campos Fernandez AN ABSTRACT OF A DISSERTATION Submitted to Michigan State University in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSPHY Department of Chemistry 2001 Professor Kim R. Dunbar CUQSTERS A“ Q‘- \ N ' -, ~-6 rem-Wm . r.‘ M p; -IC Chem-5t. ‘ iv» . ~43 ABSTRACT CLUSTERS AND EXTENDED ARRAYS WITH METAL IONS AND NITROGEN DONOR LIGANDS By Cristian Saul Campos Fernandez The study of nitrogen heterocyclic ligands in coordination chemistry has experienced a steady increase in the last thirty years. The increasing versatility of synthetic methods used in the preparation of ligands has permitted increasingly more complex molecules to be assembled. The work reported in this thesis involves the systematic study of the chemistry of five diimine ligands that have not been investigated thoroughly to date. These are 2-2—pyridyl-l,8-naphthyridine (pynp), 3,6-bis-pyridyl- tetrazine (bptz), 2,2’-bis-bipyridyl-azo (abpy), 1,3,6-trispyridyl-triazine (tptaz), and 2,3,5,6 tetrapyridyl pyrazine (tppz). The chemistry of the bptz ligand was explored with a variety of first row transition metals, with the result being the high yield syntheses of cyclic coordination compounds (metallocyclophanes). The formation of these cyclic entities rather than polymeric materials or dinuclear complexes is attributed, in great degree, to the choice of the anion which functions as a template in the self-assembly of the cationic metallocyclophanes. Anions that are similar in size and geometry, e.g. [BF4]' and [C104]', yield molecular squares, whereas the larger anion, [SbF6]', leads to the assembly of a molecular pentagon. The existence of these species in solution was demonstrated by l9F L 5 .0. o - Q I \’ ‘0 . .’ I ‘ x has -;\ .5-x4~4. - .. " ,. _I ‘ . r» n 2'.- \ b t u..- a , x u, __ y .T‘ ‘ OI‘... “' “it 3“ .. 1'5" a.’ 1" ‘Wqfi ‘E. T." o A ‘ ~55 | 4' .v- I ' L‘H‘ but- A}; Elev-v4“ l ig-ie Orle ' l NMR studies conducted on the diamagnetic metallocyclophane, [Zn4(bptz)4(CH3CN)g][BF4]3), the results of which indicate that the encapsulated anion is present in the solution form of the compound. Electrospray mass spectrometry revealed that the formation of these metallocyclophanes with other transition metals such as Mn", Fe", Coll and Cu" is feasible, but that they are not as stable as the Ni" and Zn11 analogs. The chemistry of tppz has languished for almost two decades, most likely due to reports that coordination of more than one metal center was not possible. We embarked on the synthesis and characterization of a series of mononuclear tppz compounds [M(tppz)2]n+ that can potentially be used as building blocks for the synthesis of higher nuclearity species. In addition, a new application for this ligand was discovered in our laboratory, namely as a linker for metal-metal compounds to give molecular rectangles. In this vein, the compound [Rh4(02CCH3)2(tppz)2(CH3OH)4][PF6]6 was prepared which is the first of its kind in the M-M bond field. Naphthyridine based ligands have been used relatively infrequently compared to phosphine, halide or carboxylate derivatives in metal-metal bond chemistry. The presence of two pynp ligands in the dimetal units [M2]“ (M = M0", Ru" and Rh") allows for a rich electrochemistry that is not observed for most metal-metal compounds with more electronically “innocent” ligands. In the case of two of the new compounds in this study, four reversible one electron ligand based reductions, are observed. The compound [Ru2(02CCH3)2(pynp)2][PR]; shows Class HI Robin-Day behavior with all four electrons being fully delocalized throughout the molecule, whereas in the [M02]4+ derivative, Class II behavior is found. In memory of my grandmother Estelia Alpz’zar Arguedas This tori u I: D1531. v.35. . yawn-u 'atf'u. :m. L'buku x ‘h‘ " ‘ . ah ‘ ".4 I} V '- ap.. . "fl. 0 .> h L'h)..\ “.lk Lin-IL - s 122C Cliff. SUCK}; at " ’ M. the Imp-.3? its" ~‘ ' 'h 5h. 'l‘rl'l'iir‘.‘ me ,; 1 “ O. . ACKNOWLEDGEMENTS This work would not have been possible without the support of my advisor Dr. Kim Dunbar, whose constant support, understanding and patience allowed me to overcome several obstacles during my graduate student years. I also wish to thank all the staff members and Dunbar students at Michigan State University as well as Texas A&M University who taught me laboratory skills and the use of many techniques. I would also like to extend special thanks to Lisa Thompson and John Koomen who greatly helped me with theoretical and mass spectrometry studies at the latter stages of my career at Texas A&M. In addition, I will like to extend special thanks to the members of my research group, Rodolphe Clerac and Jose Ramon Galan Mascaros for their invaluable help with magnetic measurements and Brad Smucker, Kemal Catalan and Elizabeth Lozada for the good moments that we spent in the lab. In general, I would like to thank to all of the Dunbar group members who I met throughout the last six years. I would also like to acknowledge a very special person in my life, someone who influenced my life greatly and taught me the importance of education; my grandmother. She cannot be with me at this important moment of my life, but all the times that we talked about the importance of education really encouraged me to pursue post graduate studies in chemistry. Finally, I will like to give thanks to my family who supported me even though they never quite understand what I was doing here. Without their support and encouragement I would have never had the will power to finish this difficult task. LIST OFTSABLE stoma E5 ,1") SET OF SYMBOL Chapter I... L: hie» 10!}. ..._ 1‘s . ‘ :wx. '-" b '15,? 5“ Q ........ Vi“: “if“ 'w‘tr'l “i ‘I' L. 11‘5“ AW“ :; .~-, 35:17", ‘ \. .5, . . “I?" it ‘. I: \4 :‘H' v.‘ ,7" ‘shfi‘és a “I6 L; GI8pm n_ 9.42": ”1.15.“ ' CHEC\ 1‘.‘ «LHQE‘CH3Cx ‘\= ”This... I D \. “C ‘ ‘s. t... .' H Cs. Ki" 1:. tilt-f ‘1‘?in {C _ \_ \4'ILSD', I“ HTC .v‘ NZJ‘I’C " Q I H x TABLE OF CONTENTS LIST OF TABLES ................................................................................. X LIST OF FIGURES .............................................................................. XIII LIST OF SYMBOLS AND ABBREVIATIONS ........................................................ XXIII Chapter I ............................................................................................................................ 1 Introduction ......................................................................................................................... l I. Background ..................................................................................................................... 2 Nitrogen Heterocylic Ligand Chemistry ............................................................................. 2 Mixed Valency in Ligand-Bridged Metal Assemblies ......................................................... 4 II. New Applications of Bipyridine and Terpyridine Chemistry ........................................ 5 Specific Supramolecular Interactions: Anions as Templates ............................................ 11 III. Naphthyridine Ligands in Metal-Metal Bonded Compounds ...................................... 19 References ......................................................................................................................... 25 Chapter II ......................................................................................................................... 30 I. Introduction ................................................................................................................... 31 11. Experimental Section .................................................................................................... 33 Methods and Starting Materials. ....................................................................................... 33 Physical Measurements. .................................................................................................... 34 [Ni4(bptz)4(CH3CN)3][BF4]g (l). ...................................................................................... 34 [Zn4(bptz)4(CH3CN)g][BF4]3 (2) ....................................................................................... 35 [Ni4(bpt1)4(CH3CN)g][ClO4Is (3) ...................................................................................... 35 [Zn4(bptz)4(CH3CN)g][C1043 (4). .................................................................................... 36 [Ni5(bptz)5(CH3CN)lo][SbFG]lo (6). .................................................................................. 36 {[Mn(bptz)2(CH3CN)2][BF4]2}... (7). ................................................................................ 37 2,2‘ Azo-Bipyridine (abpy). .............................................................................................. 37 [Ni2(abpy)(CH3CN)2][N03]4 (12). .................................................................................... 38 [Cu2(abpy)(CH3CN)g[BF4]4 (13) ....................................................................................... 38 Data Collection and Refinement. ...................................................................................... 39 [Ni4(bptz)4(CH3CN)g][BF4]3'4CH3CN (l). ....................................................................... 39 [Zn4(bptz)4(CH3CN)g][BF4]3'4CH3CN (2) ........................................................................ 43 [Nl4(prZ)4(CH3CN)3][C104]8'2CH3CN'C4H30 (3). ......................................................... 43 [Zn4(bptz)4(CH3CN)g][C104]3-3CH3CN (4). ..................................................................... 44 [Ni2(bptz)(CH3CN)g][C104]4 (5). ...................................................................................... 44 [Ni5(bptz)5(CH3CN);o][SbF6]10'2CH3CN (6) .................................................................... 45 {[Mn(bptz)2(CH3CN)2][BF4]2}.° (7). ................................................................................ 45 [Ni4(bptz)4(CH3CN)g] [BF4] [PF6]3[SbF6]4 (8). .................................................................. 46 [Ni4(bptz)4(CH3CN)3][C104][104]7-2CH3CN (9). ............................................................. 47 vi 1.3%.“: .. HO | 3. NFC" H43- 3: mm CV ::'31‘:‘:::“CFC\ I.» 54'" "F \v‘ .._“. CH C-\ I! v I. .- .‘555 O '7' I U- 1 "1" H ‘t“.L ' 3 p q \.M- rxucss‘lp‘; ‘; x: .233 X=TE -. 3.:X- '3.\C.'\S' I 4....k "Kin-«t u' A. 4 3 “-(P C\ ll .' ' Zr .., m-'£fC34..£r 5.4.4 t 4 . ‘ m “R 52.3.") 5 ”av. 051°“ ' - 3] SH - aux-H. r" -'ulCSSOf lx.f! D.” X'TE“ as. .‘n . nu .\ :- r .. “168 0‘1 N - . cB-ww '- 1. "M .3 ' “.1 S‘jlnhe3 Stol- r\ l 'd X. r“ F m} Cm“ ‘ $11. 3. m. R74“ L‘re “ Ork ‘ u 9.. n ‘u [C0(b0pd)2(H20)2] [PFah (10). .......................................................................................... 47 [Cu(bopd)2(HzO)2][BF4]2 (l 1). ......................................................................................... 48 [Ni2(abpy)(CH3CN)2] [NO3]4 (12). .................................................................................... 48 [Cu2(abpy)(CH3CN)g][BF4]3 (l3) ..................................................................................... 49 {[Cu(abpy)2][BF4] L... (14). ................................................................................................ 49 [Ni4(bptz)4(CH3CN)g][I][SbF6]-, (15). ............................................................................... 49 III. Results and Discussion. ............................................................................................... 50 A. Self-Assembly of Molecular Squares ........................................................................... 50 A1 Syntheses of [M4(bptz)4(CH3CN)g][X]g (M = Ni2+ and Zn”) Compounds .............. 50 MI!) metallocyclophanes .................................................................................................. 5 1 Zn(II) metallocyclophanes ................................................................................................. 51 A2. Spectroscopic and Cyclic Voltammetric Studies of [M4(bptz)4(CH3CN)g][X]g M = Ni(II), Znal); X= [BF4]', [CIOJ ....................................................................................... 52 A3. X-ray Crystallographic Results .................................................................................. 53 Ni(II) molecular squares: [Ni4( bptz)4( CH 3CN)3][X )3; X = [BF4]', [C104]' and [Ni2( bptz)( CH3CN)3][ C104 14 ............................................................................................ 53 Zn(II) molecular squares: [Zn4(bptz)4(CH3CN)3][X]3, X =[ BF41', [C104l' .................... 64 AA. NMR Studies ............................................................................................................. 68 B. A New Generation of Metallocyclophanes: Molecular Pentagons ............................... 71 B.1. Synthesis of [Ni5(bptz)5(CH3CN).o][SbF6]10 ............................................................. 71 3.2. X-ray Crystallographic Results. ................................................................................. 72 B.3. Spectroscopic and Cyclic Voltammetric Studies. ...................................................... 77 C. Chemistry of Bptz with Other 3d Transition Metals .................................................... 78 X- ray Crystallographic Studies of Bptz Products with Mn“, Coz”, Cu”. ....................... 79 D. Electrospray-MS Studies of Bptz Reactions with Mn“, Fe“, Co“, Ni“, Cu2+ and Zn“. ................................................................................................................... 83 E. Interconversion of the [Nis]10+ and [Ni4]8+ ................................................................... 92 E.S-MS Studies of Interconversion Reactions .................................................................. 97 G. 22’ A20 Bipyridine Chemistry .................................................................................... 99 G1 Synthesis of [Ni2(abpy)(CH3CN)2(N03)4], [Cuz(abpy)(CH3CN)3][BF4]4 and { [Cuz(abpy)] [BF4]2 }.. Compounds .................................................................................... 99 6.2. Spectroscopic and Electrochemical Studies. ........................................................... 100 0.3. X-ray Crystallographic Studies ................................................................................ 101 IV. Future Work .............................................................................................................. 107 Reactions of the metallocyclophanes ............................................................................. 107 V. Conclusions ................................................................................................................ l l 1 VII. References ................................................................................................................ 1 15 Chapter III ..................................................................................................................... 119 I. Introduction: ................................................................................................................. 120 11. Experimental Section .................................................................................................. 123 Preparation of Compounds. Methods and Materials. ...................................................... 123 Physical Measurements. .................................................................................................. 123 Synthesis .......................................................................................................................... 124 2,3,5 ,6-tetrapyridylpyrazine (tppz). ................................................................................. 124 vii Q‘I". '_‘ n “‘8 3:335:30; l 13:22:;"1’1-‘5- 1' :p;:';:: .'C. 0 y; c o _.\:.j:;z~; C30..- - XT;1?;‘3aC“7C\.. A- s v-" ('30.,9‘. "I- \'“F ~ ‘ ‘C "'“ .. 5r- . . u ‘ 7'5 04'1. I . - TC.- OCCH .3 13:. CT :22 ’1 :CC‘:C 35:1. “- ‘ ..«Cll C\'. 1170.; TV. "Vt“ h ... .._..- u': ‘5'- “. "~ ~12." . ”P“. s . a.- X'filuanC'H . ".U-w- C‘..C1' ‘ \"‘qw l'\' w o 11 |l"“~ " .~~.,'Z" PF.‘- 11- .. .‘T ‘4- "' Raw. T'C} . 0 -~ -1 O“ i 4. ' .iii,Cox :\' '1'“ " 2’" HERO): 21 :~\1 :ZHCH 1C\ 3‘}: SUCH C\- “T 3:21:18Fl .13 J‘CCh :‘?7 it”. .32 ':;PF;‘. 'CCH :\g-_l-:‘: _‘:. :C1-Jlsr 1 :‘. .fi.” CH1:C\ ‘ H Em ~12 SIC-o. - .3 ( l :11 A px v ‘. A T "J '3" * 3\:‘ka-; \ é .‘ o “H‘sas u S ‘- l‘ hi3 ‘0‘! A a 3. CW __ C)>Cns“3.t SK -0 ‘k kg- 9d“. 11:13]... “15.. :ECIr """"""" in ‘OxOp . ‘ ~r—~ ar ‘. \ ‘ g h... u Chg. 1| t ‘3‘“, '3‘ d Lq.“r ‘5. “UP-S " ‘5 $242 I O: '\ r ‘. ... g"- I 3 (J 2,4,6-tris(2-pyridyl)-l,3,5-triazine (tptaz). ...................................................................... 124 [Ni(tppz)2][N03]2 (16). ................................................................................................... 125 [Co(tppz)2] [P136]; (17). .................................................................................................... 125 [Fe(tppz)2][ClO4]2 (18). .................................................................................................. 125 [Mn(tppz)2] [C104]; (19). ................................................................................................. 126 [Ni(tppz)2][ClO4]2 (20). .................................................................................................. 126 [Ni2(tppz)(CH3CN)6][BF4]4 (21) ..................................................................................... 127 [Rh(tppz)2][BF4]3 (23) ..................................................................................................... 127 [Rh2(02CCH3)2(tppz)2(CH30H)4][PF6]6'CH30H (24). .................................................. 128 [Coz(tppz’)2][CoZCl7][PF6] (25). ..................................................................................... 128 [Ni(tptaz)(CH3CN)2(H20)][BE]; (27) ............................................................................ 128 [Fe(tptaz)2] [C104]; (28) ................................................................................................... 129 [Mn(tpta2)(phen)(H20)][O3SCF3]2 (29) .......................................................................... 129 X-ray Data Collection and Refinement ........................................................................... 130 [Nl(tpp2)2] [NO3]2 (16). ................................................................................................... 130 [C0(tppZ)2] [PF5]2 (l7). .................................................................................................... 135 [Fe(tppz)2][ClO4]2 (l8). ..................................................................................................................... 135 [Mn(tppz)2][ClO4]2 (19). ................................................................................................. 136 [Ni(tppz)2][ClO4]2 (20). .................................................................................................. 136 [Ni2(tppz)(CH3CN)6][BF4]4-CH3CN (21). ...................................................................... 137 { [Coz(tppz)(CH3CN)2Cl4] [PF6] [BF4] }.., (22). ................................................................. 137 [Rh(tppz)2][BF4]3 (23) ..................................................................................................... 138 [Rh4(02CCH3)2(tppz)2(CH30H)4][PF6]6-CH3CN (24) .................................................... 138 [C02(tppz’)2]PF6] [C02Cl7] (25). ...................................................................................... 139 [Co(tp)’)2Cl2] [313.12 (26). ................................................................................................ 139 [Ni(tptaz)(CH3CN)(H20)][BF4]2 (27). ............................................................................ 140 [Fe(tptaz)2] [C104]; (28) ................................................................................................... 140 [Mn(tptaZ)(phen)][Mn(tptaz)(phen)(H20)][CF3S03]4 (29). ........................................... 140 II. Results and Discussion ............................................................................................... 141 A. [M(tppz)2]2+ Series (M = Ni“, Co“, Fe“, Mn“): ..................................................... 141 A1. Synthesis. .................................................................................................................. 141 A2. Spectroscopic and Cyclic Voltammetric Studies. .................................................... 142 A3. X-ray Crystallographic Results ................................................................................. 146 B. Synthesis of the Dimer [Ni2(tppz)(CH3CN)6][BE]. ................................................. 157 B1. Synthesis ................................................................................................................... 157 BZ. Spectroscopic and Cyclic Voltammetric Studies ...................................................... 158 B3. X-ray Crystallographic Studies. ................................................................................ 158 c. Reactivity Studies of [M(tppz)2]2+ (M = Niz“, Fe”, Co“, Mn“) and [Ni2(tppz)(CH3CN)6]“. ................................................................................................... 160 D. Reactions of CoClz with tppz and tpy Ligands. ........................................................ 161 DJ. Synthesis. ................................................................................................................. 161 D2. Spectroscopic and Cyclic Voltammetric Studies .................................................... 164 D3. X-ray Crystallographic Studies ................................................................................ 164 E. Reactions of cis-[Rh2(02CCH3)2(CH3CN)6][BF4]; and [Rh2(CH3CN).o][BF4]4 with tppz. ................................................................................................................................. 17 1 viii F‘ - “; :LS', 5) 3 {Q Q _ ...-T-~'\'\ ; L.-.ux~-'~'>“' ~ h I '1 '7’ i3 ' r ('7 J I I I v- V I 5%91‘!“‘l"- 1 .0-..» {-4. ~ ..-4' “ '- ahl ‘\--—.~ ' ._.- L41“ . ., .. . r. 5372:1351: ........ r- ~ «Ov---~- .- -- f-.§x»-¢.\df.» .3. FE X-ra} CTN 31;; _' Chapterl\'.........‘.. '. trauma: . :t .._-g ‘- E); afi' ' ink ‘IAOA!'~II.‘J S:\. ‘I \" V !\ A ‘13 -‘ ."~“‘ . ~‘\ufi: "1.1. .k U ...; 1.3V \ ‘I‘He ' ‘ . Cyclic \'-‘ d‘C‘ :6 _ Ulti- N \I" Q; ... N . “gneuc S, . 1v. L; [:Grp‘ . “‘Q‘e “ A \"i’, ‘ \ FIRM “5-0573 ... ‘WuHCCS ..... E.1. Synthesis .................................................................................................................. 171 E2. Spectroscopic Studies. ............................................................................................. 172 E3. X-ray Crystallographic Studies. ............................................................................... 172 F. A Hybrid Ligand of 2,2’ Bypiridine-azo and Tetrapyridyl pyrazine: 2,4,6-Tris(2- pyridyl)-l,3,5-triazine (tptaz) .......................................................................................... 178 El. Synthesis .................................................................................................................. 178 F2. Spectroscopic and Cyclic Voltammetric Studies ..................................................... 180 F3. X-ray Crystallographic Studies. ............................................................................... 183 IV. Conclusions ............................................................................................................... 191 V. References .................................................................................................................. 193 Chapter IV ..................................................................................................................... 195 I. Introduction .................................................................................................................. 196 II. Experimental Section .................................................................................................. 197 Physical Measurements. .................................................................................................. 197 Theoretical Details .......................................................................................................... 198 Synthesis .......................................................................................................................... 198 2-(2-pyridyl)-l,8-Naphthyridine (pynp) Synthesis. ......................................................... 198 Z-aminonicotinaldehyde. ................................................................................................. 198 Preparation of 2-(2-pyridyl)-1,8-Naphthyridine (pynp). ................................................. 199 [Moz(02CCH3)2(pynp)2][BF4]2 (30) ................................................................................ 199 [Ruz(02CCH3)2(pynp)2] [PF6]2 (31). ................................................................................ 200 [Rh2(02CCH3)2(pynp)2] [31:4]; (32). ............................................................................... 200 X-ray Data Collection and Refinement. .......................................................................... 201 [Moz(02CCH3)2(pynp)2] [BF4]2‘3CH3CN (30). ............................................................... 201 [Ruz(OzCCH3)2(pynp)2] [PF6]2'CH3OH (31) ................................................................... 203 [Rh2(OzCCH3)2(pynp)2] [BF4]2'C7H3 (32) ....................................................................... 203 [Rh2(02CCH3)2(pynp)2(CH3CN)2] [BF4] [P136] '2CH3CN (33). ........................................ 203 III. Results and Discusion ................................................................................................ 204 Homologous Series of Redox-Active Dinuclear Compounds ......................................... 204 A.l. Synthesis of Compounds [M2(02CCH3)2(pynp)]2+, M = Mo“, Ru“, Rh“. .......... 204 A2. X-ray Crystallographic Studies ................................................................................ 205 A3. Theoretical Calculations. ......................................................................................... 214 A.4. UV-Visible and NMR Spectroscopic Studies. ........................................................ 214 A5. Cyclic Voltammetric Studies ................................................................................... 216 A.6. Magnetic Studies. .................................................................................................... 220 III. Conclusions ............................................................................................................... 221 IV. References ................................................................................................................. 223 Appendix I. .................................................................................................................... 225 LIST OF TABLES Page 1. Crystallographic Data for Compounds 1-15 .......................................... 4O 2. Selected bond distances (A) and angles (°) for [Ni4(bptz)4(CH3CN)3][BF4]3'4CH3CN (1) 55 3. Selected bond distances (A) and angles (°) for [Ni4(bptz)4(CH3CN)8][ClO4Js'2CH3CN'C4I-130 (3) 55 4. Distortions of the bptz ligand in the molecular squares ......................................... 57 5. Selected bond distances (A) and angles (°) for [N12(bptZ)2(CH3CN)3] [C104]4 (5) ........................................................ 63 6. Selected bond distances (A) and angles (°) for [Zn4(bptz)4(CH3CN)3][BF4]3‘4CH3CN (2) ............................................. 65 7. Selected bond distances (A) and angles (°) for [Zn4(bpt2)4(CH3CN)3][C104]3'3CH3CN (4) ............................................ 65 8. Selected bond distances (A) and angles (°) for [Ni5(bptz)5(CH3CN)5][Sng].o-2CH3CN (6) .......................................... 72 9. Selected bond distances (A) and angles (°) for {[Mn(bptz)2(CH3CN)2][BF4]2}.. (7) .................................................. 80 10. Selected bond distances (A) and angles (°) for [Ni4(bpt2)4(CH3CN)g] [BF4][PF6]3[SbF5]4CH3CN (8). . . . . . . . . . . . . . . . . .. 94 1v." ' . .‘ P‘ 3-3-3 | .1.>\m\»sb 3. .u \- \'r w . CL . 1".5uL-. it ‘ a 1‘ " ""t " ‘ 1.551;» :b \ ‘9 5. 323.1?“ m "CF .. . ‘ \u‘o:":.‘ ‘.. . a. isms..g ‘ --\. b ’C n... ' "Hfi- ' . ., . "L H. 3 9. bar" .. 4‘ .. a -. ' buistfi. .3 L: n. .. ..h Cu;:‘:‘-.l H In A (km- 1 . .'l\~‘ 53...,1” C“r~ \ 1 ‘. 11. Selected bond distances (A) and angles (°) for [Ni4(bptz)4(CH3CN)g][C104][IO4]7'2CH3CN (9) ................................. 94 12. Selected bond distances (A) and angles (°) in [Ni2(abpy)(CH3CN)2(NO3)4]'2CH3CN (12) ....................................... 101 13. Selected bond distances (A) and angles (°) for [Cu2(abpy)(CH3CN)g][BF4]2 (13) .................................................. 102 14. Selected bond distances (A) and angles (°) in { [Cu(abpy)2][BF4]2 }.. (14) ............................................................ 103 15. Selected bonds (A) and angles (°) for [Ni4(bptz)4(CH3CN)g][I][SbF6]7 (15) ................................................ 108 16. Crystallographic Data for Compounds 16-29 ....................................... 131 17. UV—Visible data for compounds (16)-(20) .......................................... 143 18. Values of the distortions exhibited by the tppz ligand by coordination to Co(II) (17), Ni(II) (l6), Mn(II) (19) and Fe(II) (18) ............................................................. 147 19. Selected bond distances (A) and angles (°) for [Ni(tppz)2][N03]2 (16) ............................................................. 149 20. Selected bond distances (A) and angles (°) for [Co(tppz)2][PF5]2'CH3CN (l7) ...................................................... 149 21. Selected bond distances (A) and angles (°) for [Fe(tppz)2][ClO4]2 (18) ............................................................... 152 22. Selected bond distances (A) and angles (°) for [Mn(tppz)2] [C104]2 (19) ............................................................... 152 xi ‘2- \_ db“."‘ " .- as e\:~\-~~ “" ' ' . '.\ ‘fifiV, ta 1 ..D‘ A I l n .. . . FA‘ 3" L‘\" . .9 5 5b a - so} 7 . 7’ ‘ I -.. “'1’“ ~. rr‘ ‘ O o.) '. a. .,'; ' Q " ‘ S: m \ ‘ M I I vs “‘5b 5‘ v- < a. ~~-.\-~.§ :0: '3": MCH' .: 3 am . ‘ M. "m. Dond d~~ .: ‘ ~p'u . '°‘ N any] vhf; toy, I K n c ‘42” L:“ ‘b 23. Selected bond distances (A) and angles (°) for [N i(tppz)2][ClO4]2. (20) ................................................................. 155 24. Selected bonds (A) and angles (°) for [Ni2(tppz)(CH3CN)6][BF4]4-CH3CN (21) .......................................... 160 25. Selected bond distances (A) and angles (°) for [C02C12(tPY)2(CH3CN)2][BF4]2. (26) ................................................ 165 26. Selected bond distances (A) and angles (°) for {[Coz(tppz)(CH3CN)2Cl2][BF4][PF6] - CHzClz }.. (22) .............................. 167 27. Selected bond distances (A) and angles (°) for {[Coz(tppz’)2][PF6][C02Cl7] (25) .................................................... 169 28. Selected bonds distances (A) and angles (°) for [Rh4(02CCH3)2(tppZ)2(CH3OH)4] [PF6]6'CH3OH (24) ......................... 173 29. Selected bond distances (A) and angles (°) for [Rh(tppz)2][BF4]3-2CH3CN'C4H30 (23) ........................................... 176 30. UV-Visible spectroscopic data for compounds (27)-(29) .......................... 181 31. Selected bond distances (A) and angles (°) for [Ni(tptaz)(CH3CN)2(H20)][BF4]2 (27) ................................................. 184 32. Selected bond distances (A) and angles (°) for [Fe(tptaz)2][C104]2-2CH3CN (28). .................................................. 186 33. Selected bond distances (A) and angles (°) for {[Mn(tPtaZ)(phen)(H20)][CF330312 } {[Mn(tptaz)(phen)(H20)][CF3803]; }°H20 (29) ................................... 188 34- Crystallographic Data for Compounds 30-33 ........................................ 202 xii c- n . ‘ \ I 5")" ~p4 :. >:It\h§b a who u. )hyECCHv; 1 \n ;\...L g. gOfCH, 3t 3- v5 1 x1"; 8 A 9- n . . . . ' 3 3‘..')“ - '- 4 . r 5\xb\ “U :‘Julk \- 'R‘H. O:CCH ': ‘ n. q Q) 6.03.41' 'v-J . .v «Li 3““ ‘ I”h y AQCCH; .: 35. Selected bond distances (A) and angles (°) for [Moz(OzCCH3)2(pynp)2] [BF412'3CH3CN (30) .................................... 207 36. Selected bond distances (A) and angles (°) for [Ruz(02CCH3)2(pynp)2][PF6]2°2CH3OH (31) ..................................... 209 37. Selected bond distances (A) and angles (°) for [Rh2(02CCH3)2(pynp)2][BF4]2-C7Hg (32) ............................................ 21 l 38. Selected bond distances (A) and angles (°) for [Rh2(OzCCH3)2(pynp)2(CH3CN )2] [BF4[PF6]'2CH3CN (33) ..................... 21 1 39. UV-Visible data for compounds (30)-(32) .......................................... 214 40. Ratio of Metal to Ligand (MIL) and Ligand to Metal (UM) character of the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO) as calculated at the B3LYP level of theory for the dication [M2(OZCCH3)2(pynp)2]2+ (M = M0“, Ru2+ and Rh“) of (30), (31), and (32) ................................... 230 41. Orbital Energies (hartrees) and Ratios for Important Molecular Orbitals in singlet (S = 0) dinuclear complex Mo(II) (30) and dinuclear complex Rh(II) (32), dication, neutral and dianion species ....... 231 42. Molecular Orbital Energies for the Pertinent Molecular Orbitals in triplet (s = 1) [RU2(02CCH3)2(PYHP)2]2+ (31). doublet (s = 1/2) (2)<'*"‘> and singlet (s = 0) 31m" .................................... 232 xiii - F . “pn- M - ‘.. . L >Lu‘5us‘o L his“. LIST OF FIGURES Page 1. Schematic drawing of the ligands (a) 2,2’-bipyridine, (b) l, lO-phenanthroline, (c) 2,2’:6’,2”-terpy1idine and (d) l,3,5-tris[4’-2,2’:6,2”-terpyridinyl]benzene ......................................................... 3 2. Schematic drawing of the ligands (a) 2-2-pyridyl-1,8 naphthyridine (pynp), (b) 3,5-bis-pyridyl- 1,2,4,6-tetrazine (bptz), (c) 2-azo-bis pyridyl (abpy), (d) l,3,6-trispyridyl-triazine (tptaz) and (e) 2,3,5,6 tetrapyridyl pyrazine (tppz) ................................................................ 6 3. Some examples of metallodendrimers ....................................................................... 9 4. Supramolecular chemistry hierarchy ....................................................................... 10 5. Schematic drawing of the molecule [(tpy)Ru(tppz)Ru(tpy)]4+ ............................... l3 6. Schematic drawings of metal tppz building blocks ................................................. 15 7. Schematic drawing of the molecule [Rh4(OzCCH3)2(tppz)2(CH3OH)4][PF6]6 ,,,,,,,,,,,, 16 8. Different functionalities in the ligands (a) l,3,6-t1ispyfidyl-triazine (tptaz) and (b) 2-azo-bis pyridyl (abpy) .................................................................. 17 9. Compounds with the radical form of the ligand abpy .............................................. 19 10. Molecular orbitals for the M-M species ................................................................ 20 xiv ‘I I. -I A Q, \.J~I‘ | '1 1‘. Jinan-o U-u' n . F. ‘ Rum-1.191" . ”.....- .', u» 55”,...“ u_.:t‘ 1' n . 1.. \-“"‘~' L " ‘7 "t'fiA-ohs.\ QIQIK '3"‘vq-ao . ‘ Kh“;b|-Q;1.Lk \‘ . ., ‘ kl.‘ _ 3‘..- H 13. n i _:fl ‘1. ‘n- O ‘ i] \\ \ ...” ‘ Spa.“ 0'". “811112 4. ’_ 5 Uig- ll. 12. l3. 14. 15. l6. 17. 18. Schematic drawing of the series [M2(02CCH3)2(pynp)2]2+ (M = Mo(II), Ru(H) and Rh(II)) .................................................................................................. 21 Possible outcome of linking four cis-[M2(OzCCH3)2(pynp)2]2+ units ................... 23 Schematic drawing of (a) 3,6 bis(2—pyridyl)tetrazine (bptz) and (b) 2,2’ bispyridyl azo (abpy) ................................................................................ 31 Schematic drawing of the distortions experienced by the ligand bptz in the tetrametallocyclophanes ........................................................................................ 56 (3) Thermal ellipsoid representation of the cation in [Ni4(thZ)4(CH3CN)8] [BF418'4CH3CN - (b) Assymetric unit with 50% probability ellipsoids. Hydrogen atoms have omitted for the sake of clarity .......................................... 58 Thermal ellipsoid representation of the cation in [Ni4(bpt2)4(CH3CN)s][C104ls'2CH3CN'C4HsO-(3) (b) Assymetric unit with 50% probability ellipsoids. Hydrogen atoms have been omitted for the sake of clarity ................................ . 59 Space filling diagrams of the cations in (a) [Ni4(bptz)4(CH3CN)g][BF4]3 4CH3CN and (b) [Ni4(bptl)4(CH3CN)s][C104]s.. 2CH3CN C4HsO with the encapsulated anion" Packing diagram of [Ni4(bptz)4(CH3CN)g][BF4]8~4CH3CN ....................... 19. Thermal ellipsoid representation of the cation at the 20. 50% probability level in [Ni2(bptz)(CH3CN)g][C104]2. Hydrogen atoms have been omitted for the sake of (a)Thermal ellipsoid diagram of the cation in [Zn4(bptz)4(CH3CN)g][BF4]3-4CH3CN. (b) Asymmetric unit in [Zn4(bptz)4(CH3CN)g][BF4]3-4CH3CN at the 50% probability level. Hydrogen atoms have been omitted for the sake of clanty . . . . . . . . . . .. XV ...60 61 62 66 21. (a) Thermal ellipsoid di gram of the cation in [Zn4(bptz)4(CH3CN)s][C104]8°CH3CN. (b) Asymmetric unit in [Zn4(bptz)4(CH3CN)g][C104]3°CH3CN. Thermal ellipsoids are drawn at 50% probability level, and hydrogen atoms have been omitted for the sake of clarity ................................. 67 22. Variable temperature "’13 NMR spectra for [Zn4(bptz)4(CH3CN)g][BF4]3 in CD3CN 69 23. (a) Thermal ellipsoid drawing of the molecular cation [Ni5(bptz)5(CH3CN)lo]'°+. Thermal ellipsoids are drawn at the 50% probability level and (b) space-filling diagram of the molecular cation with the encapsulated [SbF6]' ..................................................... 73 24. Thermal Ellipsoid drawing at the 50% level of the asymmetric unit of [Ni5(bptz)5(CH3CN)m]10+ in [Nis(bpt2)s(CH3CN)lo][SbFo]lo'ZCHaCN (6). Hydrogen atoms were omitted for the sake of clarity ...................................... .74 25. A skeletal view of the Ni5(bptz)5 pentagon superimposed on an ideal pentagon to emphasize the distortion of the ligands ........................... 75 26. Packing diagram of [Ni5(bptz)5(CH3CN)lo][SbFo] 10' .................................. 76 27. Possible outcomes for the reaction between of bptz with an octahedral-metal precursor ................................................................................................................ 78 28. (a) Thermal ellipsoid diagram view of a portion of the polymer {[Mn(bptz)2(CH3CN)2]2+}.. at the 50% probability level, (b) asymmetric unit. Hydrogen atoms were omitted for the sake of clarity ................................... , ........................................................................... 81 29. Thermal ellipsoid drawing of the mononuclear complexes (a) [C0(b0pd)2(CH30H)2][PFo]2 and (b) [CU(b0pd)2flizOz)][BF4]2 Thermal ellipsoids are drawn at the 50 % probability level. Hydrogen atoms were omitted for the sake of clarity ........................................ 82 xvi 30. ESI-MS spectra of the 1:1 reaction between [Mn(HzO)6][ClO4]2 and bptz taken after 10 minutes .................................................................. 85 31. ESI- MS spectra of the 1: 1 reaction between [Co(HzO)6][ClO4]2 andbptztaken after lOminutes... .. ... . 86 32. ESI- MS spectra of the 1:1 reaction between [Fe(HZO)6][ClO4]2 andbptztakenafterlOminutes.... 87 33. ESI— MS spectra of the 1:1 reaction between [Cu(HzO)6][ClO4]2 andbptztaken after lOminutes... ...... . 88 34. ESI-MS spectra in acetonitrile of the metallocyclophanes (a) [Ni4(bpt2)4(CH3CN)sl[BF4]s. (b) [Ni4(bpt2)4(CH3CN)a][(310413 and (c) [Zn4(bptz)4(CH3CN)g][C104]3 ................................................................... 89 35. ESI-MS spectra of the pentagon compound [N i 5(bptz)5(CH3CN)lo][SbF6]lo dissolved in acetonitrile ...................................... 90 36. ESI-MS spectra of [Ni4(bptz)4(CH3CN)g][C104]3 in different solvents. The peak being depicted is the parent ................................................................... 91 37. (a) Thermal ellipsoid drawing of the [N 14(bptz)4(CH3CN)g][BFs][SbF(,]6+ unit in [Ni4(bptz)4(CH3CN)g][BF4][PF6]3[SbF6]4 with 50% probability ellipsoids, (b) space filling diagram and (c) asymmetric unit. Hydrogen atoms have been omitted for the sake of clarity..............................95 38. (a) Thermal ellipsoid drawing of the [Ni4(bptz)4(CH3CN)g][C104][104]6+ unit in [Ni4(bptz)4(CH3CN)g] [C104] [104]7 with 50% probability ellipsoids, (b) space filling diagram that emphasizes the molecular volume of the perchlorate versus the periodate and (c) asymmetric unit. Hydrogen atoms have been omitted for the sake of clarity .................................. 96 xvii ...‘ "I l ".T ‘ I. k W \‘QWI'... V.. )‘L““‘§te.l Bali. ... ‘ ‘1 u: ...“w ll“~ o . IV, .5" ‘7“ L. h. “Vt; . .......'. l A I ‘. ‘59,”!‘9 a .1 . . )w.l¥l.1d‘l\ Gordy 39. 40. 41. 42. 43. 45. 46. 47. 48. Conversion of the square into the pentagon by addition of an excess of TBASbF6 to a refluxing solution of [Ni4(bptz)4(CH3CN)g][C104]3. (a) represents the initial sample of the square and (b) represents the final solution ........................................................................... 98 Thermal ellipsoid plot of [Ni2(abpy)(CH3CN)2(NO3)4].2CH3CN (12) at the 50% probability level. Hydrogen atoms have been omitted for the sake of Thermal ellipsoid plot of the cation in [Cuz(abpy)(CH3CN)g][BF4]4 (13) at 50% probability. Hydrogen atoms have been omitted for the sake of clarity ................................. 105 (a) Thermal ellipsoid plot of the basic unit in the polymer {[Cu(abpy)2][BF4] L... (b) an extended portion of the polymeric chain ................. 106 Schematic drawing of the molecular square and pentagon with indicated sites for substitution ................................................................... 109 . (a) Thermal ellipsoid plots of the cation in [Ni4(bptz)4(CH3CN)3][I][SbF6]7 (15) at the 50% probability ellipsoid level, (b) space filling diagram with the iodine anion inside the metallocyclophane and (c) asymmetric unit. Hydrogen atoms have been omitted for the sake of Schematic drawing of the ligand 2,3,5,6-tetrapyridylpyrazine (tppz) ................. 120 The three coordination sites in Tptaz ................................................................... 121 Cyclic voltammogram for [Fe(tppz)2][ClO4]2 in acetonitrile with 0.1 M [n—BusN][PF6] ................................................................ 144 Different types of distortion experienced by tppz upon coordination .................. 148 xviii Ii Th9") .3 '\ .14 it-\u.1-i &.. I. . . . I -.9‘ 4” . aJwb-nh- \u. .4...” .' "b--:~\~ u.. ' . §'-‘..n‘ ‘ \ inst. ......-.. . 1 '- fi , V ‘i.; I; D f H “‘yuflh ~..._ v (7) ’Hfl'u II 11 '4'. ‘ox‘D- . ““U¢ ’ y..., ., ' s I, , \ In .._,4 . a w ~a .1(“‘“‘~I . .Wflw \ ‘ ’&>L I It tn -" ‘1'} m~| ‘l‘la.€ v“ r. ‘1? lxisl‘fifi7 l . w“ 13C} H H ‘ “1.- N111: .. q a \:CI. Jail ‘3' 49. Thermal ellipsoid representation of the [Ni(tppz)2][NO3]2-CH3CN (16) molecular cation with 50% probability ellipsoids. Hydrogen atoms have been omitted for the sake of 50. Thermal ellipsoid representation of cation in [Co(tppz)2][PF6]2-CH3CN (17) with 50% ellipsoids. Hydrogen atoms have been omitted for the sake of clarity ................................ 151 51. Thermal ellipsoid representation of cation in [Fe(tppz)2][ClO4]2 (18) with 50% ellipsoids. Hydrogen atoms have been omitted for the sake of 52. Thermal ellipsoid representation of cation in [Mn(tppz)2][ClO4]2-CH3CN (19) with 50% ellipsoids. Hydrogen atoms were omitted for the sake of clarity ....................................... 154 53. Thermal ellipsoid representation of cation in [Ni(tppz)2][ClO4]2-CH3CN (20) with 50% ellipsoids. Hydrogen atoms have been omitted for the sake of clarity ................................. 156 54. Thermal ellipsoid diagram of the molecular cation in [N12(tppz)(CH3CN )6][BF4]4 CH3CN (21) with 50% probability ellipsoids. Hydrogen atoms are omitted for the sake of clarity... . 159 55. Schematic drawing of the proposed synthesis of [C03(tpy)2(tppz)2]6+ from the reaction of [Co(tppz)2][PF5]2 with two equivalents of [Co(tpy)(CH3CN)3][BF4]2 .............................................................................. 162 56. Rearrangement of the tppz ligand in the presence of CoClz .............................. 163 57. Drawing of the cation in [C02Clz(tpy)2(CH3CN)2][BF4]2 (26) with 50% probability ellipsoids. Hydrogen atoms were omitted for the sake of xix ll , . tr. 9 ”4“ “Li. 5 7.05.1 t F~ *p s}- 0 1‘8. - :u-i -l - b ' 9 ’r h’ ' "aw .1 l; 111;, n.1, ., 9 1R; 03CCr LI 1 -' Ci‘:;‘ ' ”'0 H . L l “54.. , £31.”! "a' PK“ 9 l I \ 58. 59. 60. 61. 62. 63. 65. (a) Thermal ellipsoid representation of the 1-D polymer {[C02C12(tppz)2(CH3CN)2][BF4][PF6]}... (22) with 50% probability ellipsoids. (b) Asymmetric unit diagram with 50% probability ellipsoids ........................... 168 Thermal ellipsoid diagram of [Coz(tppz’)2][C02Cl7][PF6] (25) (a) ligand unit, (b) and (c) metallocyclophane, (d) asymmetric unit and (e) packing diagram with 50% probability ellipsoids. Hydrogen atoms have been omitted for clarity 170 Thermal ellipsoid diagram of the asymmetric unit in [Rh4(02CCH3)2(tPPZ)2(CH30H)4][PFolo'CH30H (24) at the 50% probability level ................................................................................ 174 (a) Thermal ellipsoid representation of the full molecular cation in [Rh4(02CCH3)2(tPPZ)2(CH30H)4][PFoIo'CflsOH (24) at the 50% probability level, (b) space filling diagram of the cation. Hydrogen atoms have been omitted for the sake of clarity 175 Representation of the cation in [Rh(tppz)2][BF4]3-C4HgO-2CH3CN (23) with 50% probability thermal ellipsoids. Hydrogen atoms have been omitted for the sake of clarity ................................ 177 Cyclic voltammogram of [Fe(tptaz)2][ClO4]2 in 0.1M TBAPF6 acetonitrile at a Pt disk electrode versus Ag/AgCl ............................................ 182 Thermal ellipsoid plot of the cation in [Ni(tptaz)(CH3CN)2(HzO)][BF4]2 (27) at the 50% probability level. Hydrogen atoms have been omitted for the sake of clarity........... . . . . . ............l85 Thermal ellipsoid plot of the cation [Fe(tptaz)2]2+ at the 50% probability level. Hydrogen atoms have been omitted for the sake of XX \' .0. s‘.‘ ‘\- fin ‘ u a"? ('1 l/ I a ‘ ! 1| 4 I‘». P\“ 1 t. ‘I»‘ 'v ’- 4.- 1“U-L o ". him. ,0 §I~I T ‘ n- . ,2” 1.. i-L. _ 4‘, “-:~ 'Hl\:\ m a .D .. 4.5;,”141 D 54 ’1 66. 67. 68. 69. 70. 71. 72. 73. Thermal ellipsoid plot of the six coordinate Mn" ion in 1[Mn(tptaZ)(phen)(H20)l[CF380312 l 1[Mn(tpta2)(phen)(H20)][CF380312 }'H20 (29) at the 50% probability level. Hydrogen atoms have been omitted for the sake of Thermal ellipsoid plot of the heptacoordinate Mn" ion in 1[MDOPtaZXphenXHzOH[CF380312 } { [Mn(tPtaZ)(Phen)(H20)l [CF330312 l'HzO (29) at the 50% probability level. Hydrogen atoms have been omitted for the sake of Schematic drawings of the bpnp and pynp ligands ............................................ 196 Thermal ellipsoid plot at the 50% level of the cation in [M02(02CCH3)2(P)’HP)2][BF412'CH3CN (30)- Hydrogen atoms have been omitted for the sake of Thermal ellipsoid plot of the cation in [Ruz(OzCCH3)2(pynp)2][PF6]2-CH3OH (31) at the 50% probability level. Hydrogen atoms have been omitted for the sake of clarity ......................... 210 Thermal ellipsoid plot of the cation in [Rh2(02CCH3)2(pynp)2][BF4]2-C7H,3 (32) at the 50% probability level. Hydrogen atoms have been omitted for the sake of clarity 212 Thermal ellipsoid plot of the cation in [Rh2(02CCH3)2(pynp)2(CH3CN)2][BF4][PF6]2~CH3CN (32) at the 50% probability level. Hydrogen atoms have been omitted for the sake of Cyclic voltammograms for compounds (30)-(32) in acetonitrile with 0.1 M [n-BuaN][PF6] at 3 Pt disk electrode versus Ag/AgCl ....................................... 218 xxi ll 74. 75. 76. Diferential pulse voltammogram of [Rh2(OzCCH3)2(pynp)2][BF4]2 in 0.1 M TBAPF6 acetonitrile at a Pt disk electrode versus Ag/AgCl ................... 219 Plot of xT versus T (red) and 1 versus T (blue) for [RU2(02CCH3)2(P)’HP)2][PFoiz at an applied field of 1000 G .............................................................................................. 220 B3LYP calculated 0.05 isodensity surface of the HOMO and LUMO for [M2(02CCH3)2(pynp)2]2+, where AE(B3LYP) is the calculated difference between the energy of the HOMO and LUMO, and AE(EXP) is the experimentally determined excitation energy ........................................................................................... 234 xxii i ... . r . (‘1 to R r. phi. .4 . 1. i. u... .... ... 1.. 2 .s..- - r. 131. 59 Rule 5.5m an... 5.. m... -l. - .. 3 HRH kin . MIN ‘nm Vi. ..AN . k T s...» ...l.‘ ..tU ...Ali. PL. Lust nuns»: howl New} . .. . . .. . . . .. . . . ,vhi...).8€..2.....uvl! ...... on..o...L......E..q...,..r J Abpy Ag/AgCl BarF4' Bopd Bptz Bpnp pr prm br em CV °C Ep,a Ep,c emu ESI LIST OF SYMBOLS AND ABBREVIATIONS xxiii Angstrom 2-azo-bis-pyn'dyl Silver-silver chloride reference electrode Boltzmann constant Tetrakis(3,5-bis(triflouromethyl)phenyl) borate 2,5-(2-pyridyl)—1,3,4-oxadiazole 3,5-bis-py1idyl— 1,2,4,6-tetrazine 2-7 bis-(2-pyridyl)-l,8 naphthyridine 2,2’-bipyridine 2,2’ bipyrimidine broad centimeter cyclic voltammetry degree centi grade doublet (NMR) parts per million (ppm) half-wave potential anodic peak potential cathodic peak potential electromagnetic unit electrospray ionization '0‘: ’4’}! 4553‘“ v us ‘Cfl 51 ‘Ju_l .._II’UI - 410' HOMO (M)Hz mg min mL mmol nm “P xxiv molar extinction coefficcient Lande factor Gauss hour Hamiltonian Highest Occupied Molecular Orbital (mega)hertz infrared Exchange parameter Kelvin Lowest Unoccupied Molecular Orbital medium moles per liter milligram minute metal-to-ligand charge transfer milliliter millimole mass-to-charge ratio bridging ligand Avodagro’s constant nanometer naphthyridine ‘a I“\ .\.‘ 1n .5. -D;F , b mllw but a s. L hD ml. 1. L 1.. a e. .t. u\w .quv\ by ...... Ln in uu otf phen PPm pynp sh SQUID TBABF4 TBAPF6 TBAI TBAIO4 Tptaz Tppz tP)’ VS XXV nuclear magnetic resonance trifluoromethanesulfonate (triflate, CF3S03') phenanthroline parts per million 2-2’-pyridyl-1,8 naphthyridine singlet (NMR), strong (IR) shoulder Super Quantum Interference Device tetra-n-butylammonium tetraflouroborate tetra—n—butylammonium hexafluorophosphate tetra-n-butylammonium iodide tetra-n-butylammonium periodate tetrah ydrofuran 1,3,6-trispyridyl-triazine 2,3,5,6 tetrapyridyl pyrazine 2,2’;6’,2”-terpyridine ultraviolet Volt frequency VCI‘SUS, very strong ll w weak ZFS Zero-field splitting xxvi Chapter I Introduction ll . DI . (J . ... A. - , ' '5 ., “.... h. "‘ ‘ -vv- ." .- ~+ 5'...” Jiltr-Js or z "5"???- a'. for? “-Pw‘fl 1 ”Wu“, \‘i‘l'c 55m 1“, 11“)!" . '1 ~“fiiii '\ 115} I- I. Background Nitrogen Heterocyclic Ligand Chemistry The use of nitrogen heterocyclic ligands in coordination chemistry has witnessed a steady increase in the last four decades. The versatility of synthetic methods used to prepare these molecules has allowed chemists to design increasingly complex derivatives with different applications in mind. Among the ligands that have been investigated are the common diimine ligands such as 2,2’-bipyridyl (Figure 1a), 1,10-phenanthroline (Figure 1b), 2,2’:6’,2”-terpyridine (Figure 1c) as well as more elaborate ones such as 1,3,5-[tris[4’-(2,2’:6’,2”-terpyridinyl)] benzene (Figure 1d).1 One of the most simple and well studied coordination compounds based on diimine ligands is the tris-chelate complex [Ru(bpy)3]2‘i.2 In general, coordination compounds of this type based on the 2,2 bipyridine motif exhibit strong luminescence in solution at room temperature, and have a powerful photosensitization capacity for electron and energy-transfer processes.3 The photoluminescent excited state is a strong reductant as well as an excellent oxidant due to the presence of an electron deficient d5 metal center and an excess electron located in the ligand network in the excited state. Modifications to the 2,2’ bipyridine unit permits one to tune of the redox potentials of the ligands over a significantly wide range.4 Such strategies have allowed for the synthesis of Ru(H) complexes that are either good oxidants or reductants in the excited state.2 “We 1. (bl l (d) l Figure 1. Drawing of the ligands (a) 2,2-bipyridine, (b) 1,10-phenanthroline,(c) 2,2':6',2"-terpyridine and (d) 1,3,5-tris[4'-2,2':6,2"-terpyridinyl]benzene. .Uit‘t‘d i 1;; Mix: One important application of metal polypyridyl chemistry is in solar energy conversion processes.:"5 For example, a major use for the photosensitiser [Ru(bpy)3]22+ is the photodissociation of water by visible light, but a major drawback is that it can only transfer a single electron to a substrate.3 Consequently, much effort has been expended over the last ten years to design polymetallic systems that incorporate numerous [M(bpy)2]2+ moieties within the same molecule.6 Mixed Valency in Ligand-Bridged Metal Assemblies Mixed-valence materials that contain several redox sites in more than one oxidation state have attracted the interest of chemists for many years. Robin and Day7 defined three broad classes of mixed-valence materials that are referred to as Class I, II and HI compounds. Class I mixed-valence species are those in which the interaction between redox centers bridged by a ligand is so weak that the mixed-valence material exhibits the properties observed for isolated mononuclear species. For Class III compounds, the opposite is encountered, namely the interaction between the two centers is so strong that the properties of individual redox centers are not observed, but rather new properties characteristic of the coupled redox units are exhibited, i.e., the system is delocalized. Intermediate between these two categories are Class II materials that exhibit redox characteristics which are slightly altered from the properties of the isolated units; these are referred to as partially delocalized systems. Cyclic voltammetry is an invaluable tool for establishing the placement of any compound within the Robin-Day classification scheme. Based on the precedence of Taube’s work, it is possible to define a comproportionation equilibrium constant, K, for ‘ . I .w- ‘ '31: :;.;::‘::...- 5“ i- a -l 4.“ 'V «:31th r ‘ {xv-"Xi :;.._,.. I. , ~-.-~ u .311} 3L 5‘. 'I, I! '5 ~~~ O -. .‘u .l .116 ix 0: 5 L0“. The lnzcrtticd citlxizziizon. Int; 11. New Appli One of “t LJI 17.22520115 in the . mg to desgr. ‘ :c‘rgemtrilcs 11:1? ”5331 Properties.9 .‘l‘ s..-am!) of m;- h 171: - . . Mi reporter: mint) in arcs 38.1211 mlolles :’ Luce” ll Id) s‘zr-pyrfl- the equilibrium between two valence states; the separation between two successive reversible redox potentials allows for its calculation as shown in equation 1.8 [xwxl + lxwxlz' zlxwxl-,K. (Eq- 1) where anc = eprEl/a (in mV) 25.69 If there is no communication between the redox centers (Class I), the Kc constant is S 102. In the case of complete delocalization between the redox centers, KC is very large, 2 106. The intermediate situation, in which there is electronic coupling but not full delocalization, yield Kc values in the range 102< K¢<105. II. New Applications of Bipyridine and Terpyridine Chemistry One of the current challenges in chemistry is the manipulation of noncovalent interactions in the design of new materials in a manner akin to Nature. Chemists are striving to design building blocks, often called tectons, that self-assemble into larger conglomerates with the ability to store information in the form of electronic, magnetic or redox properties.9 Much of the supramolecular chemistry in recent years has involved the self—assembly of metal containing molecules with the use of polydentate nitrogen ligands. The work reported in this dissertation involves the application of nitrogen heterocyclic chemistry in areas where they have not been traditionally employed. Specifically, the research involves the coordination chemistry of the five ligands in Figure 2. These include (a) 2-2-pyridyl-1,8-naphthyridine (pynp), (b) 3,6-bis-pyridyl-l,2,4,6-tetrazine \/ \_/ \/ bptz Figure 2. Schematic drawing of the ligands (a) 2-2-pyridyl-1,8 naphthyridine (pynp), (b) 3,6-bis-pyridy1- 1,2,4,6-tetrazine (bptz), (c) 2-azo-bis pyridyl (abpy), (d) l,3,6-trispyridyl-triazine (tptaz) and (e) 2,3,5,6 tetrapyridyl pyrazine (tppz). q I '11”: ‘Ci 320'..- ..-L'- . .' a I _ . ‘i‘C- {gjfgf‘tfi.:. ' .. .0 regions H". R- senile arm 0 .w'u p '9‘. 'II‘ n‘r ...;- :10” .‘Heoul 4L‘i| / Z\ / / \ A lit 1:... “547KB haw: ‘5 :‘lglns4 ”M With in. WW Units [ha I W mm the tfiffl . 1, l, (bptz), (c) azo-2,2’-bipyridine (abpy), (d) 1,3,6-trispyridyl-triazine (tptaz), and (e) 2,3,5,6 tetrapyridyl-pyrazine (tppz). In the past, such ligands have been used mainly in reactions with Ru(II) and Os(II) centers,l0 but in the present work, they are used to assemble arrays of paramagnetic first row metal ions and low valent second row transition metal ions that form metal-metal bonds. O Q Q Q N— \/€\/ ._ N N \/\/\/ N. ,N—N \ I Scheme 1. The ligands have been chosen on the basis of their demonstrated ability to produce compounds with interesting electronic and redox properties.ll Ligand a (pynp) bridges dinuclear units through the naphthyridine unit, thereby allowing for the formation of molecules with the dimetal core "[M2(pynp)2]2+". Ligands b-e possess two or more coordinating domains that permit the synthesis of polymetallic arrays in the form of 1U'9 v I. a 4 ... 3’ 3 ..nE“ - fit. ' A ““15 UHALS 0: p‘ I. l 9 ~rr ' fi' kit-‘1“ 88141 x 5 .....x ”in-v]; ‘ Ltioy‘o .xlIEI-~ A o l ..'.' t , ,.,I,.,.. s-...ac .0. pm... .. .3 ‘4 .1 In snL 51—)» fat“: [0 PFC} Idf' ._ ‘ 't 4 ‘1 ‘ L -~-D..iu11.orl 3."; W! ‘I ‘- (fl . '3' #1.. m . :wa' - 110mg..e> lIon- ., -~~~~u:::on. .1. Bipyridine-l | Supramo, Elf dens: t cyclic units or polymers. Ligands b (bptz) and c (abpy) share some common features, i.e., both can be envisioned as bis-pyridyl units joined by either one or two azo (tetrazine) groups (scheme 1).ll The azo group possesses low lying 112* orbitals (LUMO) that are suitable for promoting good electronic communication between metal centers.H In the case of ligands d (tptaz) and e (tppz), the triazine and pyrazine rings are known to provide a good it pathway for electronic or magnetic coupling. Both ligands possess terpyridine coordination sites.‘2 Each chapter in this dissertation describes the chemistry of a specific ligand and its application in the design of tectons (building blocks) and their intended use in building larger molecules. The dissertation is organized into four chapters including the introduction. A. Bipyridine-based ligands in Paramagnetic Arrays Supramolecular Chemistry ofpolytopic bpy ligands The design of arrays with the goal of exploring electronic or magnetic coupling between metal centers has been under intense investigation in the last three decades.'3 The synthesis of large heterocyclic receptors (ligands) with multiple coordination domains (polytopic), has enabled chemists to design large molecules that exhibit new properties as a result of cooperative effects between the constituent building blocks. An excellent example of this approach can be found in the family of materials known as metallodendrimers (Figure 3).” Progress in this field requires the availability of molecular components (building blocks) with well-defined structures and properties. Figure 3. Some examples of metallodendrimers.12 This approach has major drawbacks, namely multistep procedures similar to a typical organic covalent approach, which results in low yields for the synthesis of large molecules. The self-assembly of large organic molecules in living organisms takes place thorough collective weak forces including ion-pairing,'5 hydrophobic or hydrophilic interactions,’6 hydrogen-bonding,l7 host—guest interactions,l8 rt-stacking,l9 and donor- acceptor interactions.20 By manipulating these supramolecular forces, the linkage of small units (molecules) with useful characteristics to form large entities (supramolecular Macroscopic conglomerate Supramolecular assembly Supramolecular , , array = new tecton . Increasrng Superstructural Complexity Supramolecular assembly Building Block (T ecton) = Primary structure Figure 4. Supramolecular chemistry hierarchy18 10 . ‘fh ‘ q may we" 5‘? " 0’ “in; ‘ e ...-o 1 $6.35.“ 01 s..; The (:33 . V “0‘ J .’ n .. “ NJ, lsgloit 0‘ U ‘K 16 "3‘ ~ 5 1" " A‘.»~5 " .3. I H‘IJ"?‘F‘ P.~ a :I.I—b:l ' "' h‘ ' u n I -. 3"".F- Ir ' ‘ .. I‘I. V.) ‘ A&M... ~ U ' . s l’ .._..i- 5’ .. 1" p. 9 ‘ .- ...t,t..l€.d165 lFIE b i, . g“. .petljzt Supra As descnb W ' 1.5.5. I: 31301).“ t...el role 1n 1}..- ,i',“a--9' . ~55».~4th11 IS the ‘. '5”!' I811 ; 1" : 'Ifi-Htln gls one - . \. winw- species) can be more efficiently achieved. Supramolecular chemistry is described as the chemistry of the “intermolecular bond”, as defined by J. M Lehn.” The driving force in supramolecular chemistry is the self-assembly of larger entities from specifically engineered smaller building blocks. Once these smaller entities have been assembled, they may perform complex functions such as light harvesting,22 conversion of light into chemical23 or electrical energy“, or function as memory devices.” Supramolecular systems are often categorized according to different levels of hierarchy. Primary structure corresponds to small building blocks that are referred to as m. In purely organic supramolecular structures, tectons aggregate via noncovalent bonds to generate polymolecular aggregates called superrnolecules. These superrnolecules can, in turn, associate with one another to render gigantic macroscopic conglomerates (Figure 4).263 Specific Supramolecular Interactions: Anions as Templates As described in the previous section, non-covalent interactions (hydrogen bonding, 7t stacking, van der Waals interactions, cation or anion interactions) play an essential role in the assembly of supramolecular structures. Of particular relevance to this dissertation is the use of anions as templates in the assembly of metallocyclophanes. Templating is one of the more efficient procedures for self-assembly at the disposal of the chemist. It involves the use of temporary or permanent ‘helper” species, of organic or inorganic nature, to assist in the process of assembly. The vast majority of the template effect cases reported in the literature are cation related.27 Among these, crown ether chemistry is the most prominent. By comparison, the study of anion templates is much less common, and there are relatively few cases reported in the literature to date.28 11 I r - i ‘ V -" .. -.. .. ._ - ‘.~' .-. .-. ... . . 4 II 1 .I p ... H .-- .-: ..g, ..1 .-~ :2. ’ -. v. --« -.. on. ~. (- ,” I 3" s‘~ __. 9<~ 1.. .... -II .. ,=. -u- F. l ' ; l. .._. \r _’b\ Dilt’f, Hill 5. Bit/21nd) “'3!" Pool“ IuG rim ,0; 1 Il l "t gfumflnc Chapter 11 describes self-assembly processes in which the divergent ligand, 3,6-bis pyridyl-tetrazine (bptz) permits the self-assembly of metallocyCIOphanes of different nuclearities. The bptz ligand is a bis-bipyridine chelate that is capable of assembling metal cations into cyclic olygomers or polymers. The overwhelming factor in dictating the outcome of the reaction was found to be the size and shape of the anion. The results presented in Chapter II constitute an important contribution to the area of metallocyclophane chemistry and underscore the role of the anion choice in forming a specific nuclearity for cationic assemblies. It is important to point out that previous research in the formation of cationic molecular square has not address the role of the anion (scheme 2). I Divergent Bridging Ligand With two trans Divergent Metal Precursor binding sites with six labile positions Scheme 2. B. Temyridine ligands in Paramagnetic Arrays Despite their outstanding photochemical properties, [M(bpy)3]2+ complexes present two major drawbacks as building blocks for polymetallic arrays, namely stereo and/or geometric isomerism. The use of ligands with the tpy (tpy = terpyridine) 12 coordination unit are advantageous from the geometric point of view, namely [M(tpy)2]“+ complexes are achiral.29 Synthetic tailoring of tpy based ligands has allowed chemists to design ligands with multiple tpy binding sites. For example the tris-tpy ligand depicted in Figure 1d forms large polymetallic arrays based solely on coordination bonds.3'4”5'6 The main goal of this chemistry is the construction of nanosized components by a “bottom- up” approach, i.e., beginning with molecular components. The molecules are highly branched tree-like species commonly called dendrimers and are designed with specific properties such as the capability to absorb visible light, to luminesce, or to undergo reversible multielectron redox processes. Extensive research has been carried out in this area30 with Ru(II) and 05(11):“ being incorporated into building blocks called diads (two metal centers) and triads (three metal centers) based on [M(tpy)2]2+ type units that can function as photosensitizers.32 4+ /\/\\/ /\ N/ / \ \ _\\/ / F /\ Figure 5. Schematic drawing of the molecule [(tpy)Ru(tppz)Ru(tpy)]4+. One of the more important characteristics of metallo-tpy arrays is that they exhibit mixed-valence behavior.33 For example, the complex [(tpy)Ru(tppz)Ru(tpy)]4+ with two 13 L 3" ' “A < ‘ V 2" 9“ 3"". ‘ . g'fL’.i Q ~ ."“ ‘- 2.". 311‘ l n. I F 0.: Li. W 0'5" ..‘rliii of Wk" . y.. «r fill-'31,," ., “dull-E 59¢ titles 01ft: m dost: 01751379017 at 11c prise: Tittit literal". equivalent Ru(II) centers (Figure 5)17 exhibits two oxidation couples corresponding to Ru(H)/Ru(III) and Ru(HI)/Ru(III) species. The large AEV, value for the oxidation processes is evidence for strong delocalization through the tppz ligand (Figure 2e) which stabilizes the mixed valence state Ru(H)/Ru(III). In addition to homometallic systems, multibranched ligands can be used to synthesize heterometallic systems, e.g., [(tpy)Ru(tppz)erl3]2+.l7 In this case the ruthenium center is the light absorbing site whereas the Ir(III) center is a catalytic center. These types of mixed-metal systems present the possibility for developing supramolecular complexes with widely varying functions due to the different metal centers. In this manner, compounds with new properties that arise from cooperative effects are being discovered. As previously mentioned, polymetallic arrays often undergo multiple electron redox processes. This versatility in redox chemistry can be envisioned as providing a switching control, namely the possibility of turning a particular intermolecular interaction "on" or "off". Conceivably one could affect the strength of different binding sites by means of redox chemistry, thereby allowing for control over variables such as nuclearity or binding specificity towards a specific analyte (i.e., a sensor).34 Constable and coworkers offer an excellent example of this approach wherein the nuclearity of a complex depends upon the redox state of the chelated metal ion.35 One important aspect of supramolecular compounds based on coordination bonds is that the presence of metal atoms in the building blocks generates new types of molecular interactions, which are characteristic of inorganic systems. The self-assembly approach for the design of metal-based supramolecules offers an alternative to the 14 i .5113 “was 'R“, '-‘ 1V " ' 1E Cum.“ ' l "W . .r . Ailey/5‘, J16) Units be classical organic route, in which one building block is added in each step of the synthesis. This process takes advantage of metal-ligand interactions that are fairly kinetically labile. The resulting supramolecular entities are often obtained in high yields and require fewer steps than equivalent covalent syntheses. The reversibility of the coordination bonds present in the assembly contribute to a defect-free product because the intermediates are in equilibrium with each other as the final, more thermodynamically stable compound is being formed36 Tridentate I | — Tridentate coordination N/ \ *— coordination site site / \ / \ I” H N CCH3 . Iabile 3C0 \ )1 LabrleI . acetonitrile H3CCN—M—N / \ N—M—NCCH3 acetonrtnle molecules N/ \ _ / \ molecules H30C I \ NCCH3 _ \ / J Figure 6. Schematic drawings of metal tppz building blocks. Ligands based on the terpyridine binding motif have not been used extensively to connect first row transition metals. Chapter III is devoted to the self-assembly of paramagnetic metal ions of the 3d elements with the ligand tppz (Figure 2c). The general “hummer. it mm goal is to probe the magnetic behavior of metal-tpy arrays. The tppz molecule, reported in 1959 by Lion and coworkers,37 possesses two tpy coordination domains that allow for the preparation of dimetallic or higher order metal-arrays. Three precursors of the type [M(tppz)2][X]2 (where M = Coz", Fe“, Ni2+ and x = [N03]‘, [c104]; [Pm and [31:41) were synthesized (Figure 6). They exhibit different degrees of electronic coupling between the two tppz units ranging from complete delocalization (Class HI) for [Fe(tppz)2][ClO4]2 to no electronic interaction at all in the case of [Ni(tppz)2][NOg]2. — -_i 6+ A N O O i .~‘\ ,e“ HsCHO—Rh Rl one... NVT ...... N \r NVN N'\ l l» d ‘. N N N'\ \s‘ l/ i N N / H3CHO Rh IRh—OHCHa o \‘ \‘ N\\ i N\\\ i O O -02CCH3 V O __ __.i Figure 7. Schematic drawing of the molecule [Rh4(OzCCH3)2(tppz)2(CH3OH)4][PF6]6. The mononuclear building blocks [M(tppz)2]"+ posses two dangling tpy binding sites for further coordination to other metal ions. In addition to the electrochemical behavior, some of the molecules exhibit interesting magnetic properties, for example 16 .... ...;i p.31. : {f flM/l [Co(tppz)2][PF6]2 exhibits spin crossover behavior. Besides the mononuclear compounds, a dinuclear [Ni2(tppz)(CH3CN)6][BF4]2 and a polymer of the form [Coz(tppz)(CH3CN)2C12][BF4][PF6]... were also synthesized and structurally characterized. An unexpected application for tppz is reported in chapter 111, namely as a bridge between two metal-metal bonded units (M-M). Earlier reports by Pruchnick and coworkers38 indicated that two tpy ligands can bind to one dirhodium unit, viz, in the compound [Rh2(OzCCH3)(tpy)2]Clz. This result prompted us to attempt the use of tppz to link two [ha]4+ units, which we believed could occur to give and open structure. Instead the linkage of two [Rh2(OzCCH3)]3+ units led to the formation of a molecular rectangle composed of short Rh-Rh bonded sides and long Rh-tppz-Rh sides (Figure 7). C. Dual Bipyridine/Temyridine ligands Terpyridine domain Azo group Bipyridine domain Figure 8. Different functionalities in the ligands (a) 1,3,6-trispyridyl-triazine (tptaz) and (b) 2-azo-bispyridyl (abpy). 17 - .9 o' u 2‘ I \ . . .- O-v .- ‘ o w -v- on. I-3 0" . i ~ ~- \ I ‘9 ‘ '1 I l ' 5. 1. uni-h" Iiif ~V.~W" “‘L ht. 11.211.11th ‘4 3.5,. I...‘ 1 . Ju...‘ U1 die 4 U I‘H'I‘Ofl‘to 0.. - o "ring. Juan 3ii‘ $15.le f \. :‘t‘ivd.1it\ 0.1 LUL I D. infirm/1'11 fin I “'43:: Defa' ‘ .1 I“ Chapter IH also contains a brief account of the coordination chemistry of the ligand 2,4,6-tris-pyridyl triazine (tptaz) with first row transition metals. The ligand can be envisioned as being a combination of two different coordination motifs, namely bpy and tpy (Figure 8a). In this part of the chapter, we reported the syntheses of three mononuclear compounds in which the metal is bound to the tpy domain and the bpy site is free to be used to coordinate to other metal ions. Cyclic voltammetric studies reveal a rich electrochemistry for these mononuclear complexes, the most interesting example being the [Fe(tptaz)2]2+ compound which displays four reversible one-electron reductions, and "'. The electrons added to the molecule are an oxidation corresponding to Fe"—>Fe partially delocalized throughout the tptaz molecules as determined from the electrochemical data. A few dinuclear compounds with this ligand have been reported, but minimal characterization was reported.39 The inductive effect on the triazine ring with binding of the first metal center decreases the basicity of the nitrogen atom of the open coordination site, but the possibility of accessing reduced species will increase the probability of coordinating a second metal. This will be explored in future studies. D. Azopyridine based ligands in Paramagnetic Arrays Chapter 11 includes a brief description of the synthesis and characterization of dinuclear compounds with the ligand azo-2,2’-bipyridine (abpy) (Figure 8b) which possesses low lying 1t* orbitals based on high electron density located at the coordinating N centers.40 This characteristic allows the abpy ligand to function as a molecular bridge between metal centers.“ Previous studies with metals such as Ru(II) and Os(II) have 18 ligur [11. 1131111 [011112011115 lit ffli‘.‘ i" .I. I I ,1; alt-'lm’m" , i A revealed that there is strong electronic coupling (a large comproportionation constant, Kc) indicating good stability for the mixed-valence species with these metals. Dinuclear complexes with the abpy spacer have a short distance between metal centers as compared to ligands with similar coordination capabilities such as bptz (chapter 11), bpym and bppz. Another noteworthy aspect to consider is that the abpy can be reduced to a stable radical spacer in coordination compounds e.g. in the compounds [Cu2(u-n‘-abpy--)(Ph2P(CH2)6PPh2)1tam“ and toaabpy'-)(Br)(c0><102 L(mol-em)"; A = 361, e = 1.47 x 104 L(moi-em)"; x = 203, e = 5.29 x 102 L(mol-cm)". 37 0153113." 3:31.25: 8550355. . ., ..., , >L.Uka\‘il. A [Niz(abPY)(CH3CN)2][N0314 (12)- A sample of [Ni(HzO)6][NO3]2 (100 mg, 0.34 mmol) was dissolved in 30 mL of acetonitrile in a beaker. The pale green solution was stirred until the entire solid had dissolved, after which time a quantity of abpy (32 mg, 0.17 mmol) was added. The solution, which immediately changed to an intense green color, was stirred for 4 additional hours and then concentrated to 10 mL. Slow vapor diffusion of diethyl ether into the reaction solution afforded dark green crystals within 6 days; yield, 80 mg (75%). IR (KBr mull) cm": 2724 (w), 1620 (w), 1147 (w), 1039 (w), 1022 (w), 801 (w), 722 (w). UV-Vis (acetonitrile, nm, e = 9.8 x 10'6M): A = 344, e = 1.8 x104 L(moI-cm)". [Cu2(abpy)(CH3CN)5][BF 414 (13)- The salt [Cu(CH3CN)4][BF4]2 (100 mg, 0.25 mmol) was dissolved in 20 mL of acetonitrile and treated with abpy (22 mg, 0.12 mmol) which led to an instantaneous color change from a blue to a pale green color. The reaction mixture was stirred overnight, after which time the solution was concentrated and treated with diethyl ether to the point of saturation. The solution was then placed in the freezer, and within 5 days green crystals were obtained; yield, 82 mg (80%). IR (KBr mull) cm": 2724 (w), 2296 (w), 2323 (w), 1589 (w), 1261 (w), 1229 (w), 1027 (br,s), 805 (w), 722 (w). UV-Vis (acetonitrile, nm, c = 8.0 x 10'6M): x = 351, s = 2.7 x104 L(mor-em)"; 1. = 230, e = 1.98 x 104 L(mol-cm)". 38 0812 C1 Data Collection and Refinement. The X-ray data were collected on a SMART 1K area detector diffractometer equipped with graphite monochromated Mo K01 radiation (ha = 0.71073 A). The frames were integrated in the Siemens SAINT25 software package and the data were corrected for absorption using the SADABS program.26 The structures were solved using the direct-methods program SI-IELXS-97.27 Crystal parameters and basic information pertaining to data collection and refinement are summarized in Table 1 [Ni4(bpt2)4(CH3CN)s][BF 413°4CH3CN (1)- Crystals of [Nia(bptz)4(CH3CN)g][BF4]3-4CH3CN were grown by slow diffusion of toluene into an acetonitrile solution of the title compound. A dark green prism of dimensions 0.05 x 0.12 x 0.25 mm3 was secured on the tip of a glass fiber with Dow Corning silicone grease and cooled to 173(1) K in a cold N2(g) stream. A total of 24786 reflections was collected, 16456 of which were unique. Five out of the eight [BF4]' ions were disordered, therefore restraints for chemically equivalent distances (B-F = 1.37A) were applied. Displacement parameters of related fluorine positions were equated by means of constraints in order to minimize variables since the [BF4]' anions exhibit positional/rotational disorder patterns. The extensive disorder accounts for the slightly higher than usual R factors. The final full-matrix refinement was based on 9444 observed reflections with Fo>40(Fo) that were used to fit 1554 parameters to give R1 = 0.0831 and wR2 = 0.1957. The goodness-of-fit index was 1.026 and the highest peak in the final difference map was 1.182 e'/A'3. 39 .Vau 1- 23:3. .12: e. v .2 ms .~—.~A~ Wizarznw. --:7..At.~. V th .V\-=.~. ”—OO 5.3 mm: 82 B: as; 483 .1. 23 52 u 23 N32 1 23 :35 n 23 ~83 u E; “Hues...” 3251 E 38.7. 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A light orange platelet of dimensions 0.11 x 0.09 x 0.24 mm3 was mounted on the tip of a glass fiber with Dow Corning silicone grease and cooled to 110(1) K in a cold N2(g) stream. A total of 63108 unique reflections was collected of which 24635 were unique. Two of eight of the [BET ions were disordered, therefore restraints on chemically equivalent B-F (1.37 A) bonds were applied. Displacement parameters of related fluorine atoms were constrained to minimize parameters. The final refinement was based on 13131 reflections with Fo>40(Fo) that were used to fit 1394 parameters to give R1 = 0.0695 and wR2 = 0.2017. The goodness-of-fit index was 1.035 with the highest peak being 1.681 e'lA’3. [Ni4(bptz)4(CH3CN)g][C104]3-2CH3CN°C4H30 (3). Crystals of [Ni4(bptz)4(CH3CN)g][C104]3°2CH3CN-C4HgO were grown by slow vapor diffusion of THF into an acetonitrile solution of the compound. A dark green prism of dimensions 0.11 x 0.08 x 0.02 mm3 was secured on the tip of a glass fiber with Dow Corning silicone grease and placed in a cold N2(g) stream at 110(1) K. Of the 79465 reflections that were collected, 25404 were unique. The final refinement was based on 9335 reflections with Fo>40(Fo) that were used to fit 1384 parameters to give R1 = 0°06“ and wR2 = 0.1584. Restraints for the chemically equivalent distances were applied to the one disordered [C104]' (Cl-O = 1.44 A). The displacement parameters of related oxygen positions were equated by means of constraints in order to minimize Variable$.The goodness-of-fit index was 0.9 and the highest peak in the final difference map was 1.541 e'lA'3. 43 ,r...‘ K) 3 o . f If) I‘ A Y‘- u._’) “"5 fl: ‘4. L1 [Zn4(bptZ)4(CH3CN)3][Cl04]3°3CH3CN (4)- Light orange, single crystals of [Zn4(bptz)4(CH3CN)3][C104]g'3CH3CN were grown by slow vapor diffusion of diethyl ether into a solution of the compound in acetonitrile. A platelet crystal of dimensions 0.1 x 0.25 x 0.03 mm3 was placed on the tip of a glass fiber with Dow Corning silicone grease and placed in a cold stream at 110(1) K. A total of 44125 reflections was collected of which 7997 were unique. Atoms C(19), C(20), C(33) and C(34) were heavily disordered, and were, therefore, refined isotropically. In addition, four of the eight [C1041 ions were disordered, and restraints on their distances were applied (Cl-O 1.44 A). The final refinement was based on 4776 reflections with Fo>46(Fo) that were used to fit 731 parameters to give R1 = 0.0764 and wR2 = 0.2218. The goodness-of-fit index was 1.024 and the highest peak in the final difference map was 1.410 e'/A‘3. The extensive disorder accounts for the higher than usual R factors. [Ni2(bptz)(CH3CN)g][C104]4 (5). Single crystals of [Ni2(bptz)(CH3CN)3][C104]4 were obtained by slow evaporation of a filtrate obtained after harvesting a bulk sample of [Ni4(bptz)4(CH3CN)3][ClO4]g. A pale green needle of dimensions 0.25 x 0.03 x 0.05 mm3 was mounted on the tip of a glass fiber with Dow Corning silicone grease and placed in a cold N2(g) stream at 110(1) K. The data set included 4433 reflections of which 3371 were unique. The final refinement was based on 1968 reflections with Fo>40(Fo) that were USCd to fit 313 Parameters to give R1 = 0.0648 and wR2 = 0.1538. The goodness-of-fit index was 0.957 With the highest peak being 0.733 e'lA'3. [Nis(bptz)s(CH3CN)lo][SbF6]lO'ZCHSCN (6). Crystals of (6) were grown by slow diffusion of a acetonitrile solution of [Ni5(bptz)5(CH3CN).0][SbF(,]lo into dichloromethane. A green prism of approximate dimensions 0.13 x 0.2 x 0.05 mm3 was secured on the tip of glass fiber with Dow Corning silicone grease and placed in a cold N2(g) stream at 110(1) K. A total of 36580 reflections was collected of which 12327 were unique. Four of the ten [SbF6]' ions were disordered and therefore required modeling in several orientations. Constraints on the Sb- F distances were applied (1.88 A). Furthermore, the displacement parameters of related fluorine positions were equated by means of constraints in order to reduce parameters. The atoms Sb(1), F(l), F(2), F(3), F(4), F(5) and F(6) were refined isotropically. The final refinement cycle was based on 8016 reflections with F0>40(Fo) that were used to fit 891 parameters which led to R1 = 0.1160 and wR2 = 0.3645 and a goodness-of-fit of 1.069. The highest peak in the final difference map is 4.551 e'lA3 and is associated with a disordered [SbF6]' anion. The extensive disorder accounts for the higher than usual R factors. {[Mn(bpt1)2(CH3CN)2][BF412l-o (7)- Crystals of {[Mn(bptz)2(CH3CN)2][BE];}.. were grown by slow diffusion of a acetonitrile solution of [Mn(CH3CN)4][BF4]2 into a dichloromethane solution of bptz. A liglib-orange platelet of approximate dimensions 0.2 x 0.1 x 0.02 mm3 was secured on the tip Of a glass fiber with Dow Corning silicone grease and placed in a cold N2(g) stream at l 10 (UK. A total of 12882 reflections was collected of which 4480 were unique. The final least-squares refinement of 382 parameters based on 2339 reflections with F">46(Fo) resulted in residuals of R1 = 0.0666 and wR2 = 0.1744 and a goodness-of-fit 45 index of 0.951. The final difference Fourier map revealed the highest peak to be 1.711 e' #13. [Ni4(bpt2)4(CH3CN)s][BF4][PF a]3[SbF 614 (8)- Single crystals of [Ni4(bptz)4(CH3CN)3][BF4][PF6]3[SbF6]4 were grown by slow diffusion of a solution of [Ni5(bptz)5(CH3CN).o][SbF6].0 in acetonitrile into a solution of toluene that contained a mixture of [TBA][BF4] and [TBA]PF6. Single crystals grew over a period of two weeks in a sealed glass tube of 5mm diameter. A crystal of dimensions 0.15 x 0.8 X 0.05 mm3 was secured on the tip of a glass fiber with Dow Corning Silicone grease and placed in a cold N2(g) stream at 100(1) K. A total of 5030 reflections was collected of which 3459 were unique. The highest peak in the final difference map was 1.561 e’lA'3. All of the anions present in the structure are disordered, thus restraints on chemically equivalent distances (B-F 1.40911, Sb-F 1.820A, P-F 1.622 A) were applied. The tetraflouroborate anion displays a two-way positional/rotational disorder for the fluorine atoms. In addition, the B(l) atom is disordered over two different positions. Fluorine atoms F(7), F(8), F(9) coordinated to Sb(2) are involved in a two-way positional disorder; therefore, the displacement parameters of the opposite fluorine positions were ecluated by means of constraints in order to minimize variables. In the case of the [PF6]' anion, the displacement parameters of related fluorine atoms were also constrained. The final refinement cycle was based on 3459 reflections with Fo>40(Fo) that were used to fit 419 Parameters which led to R1 = 0.0765 and wR2 = 0.1075. The goodness-of-fit index Was 1.030, and the highest peak in the final difference map was 1.25 e'lA3. Extensive disorder accounts for the slightly higher than usual R factors. 46 [Ni4(bptz)4(CH3CN)3][C104][IO4]-,-2CH3CN (9)- Crystals of the product were grown by slow diffusion of a acetonitrile solution of [Ni4(bptz)4(CH3CN)g][C10413 into a toluene solution containing a large excess of [Bu4N][IO4]. Crystals grew at the interface of the two solvents within two weeks. A pale- 3 brown rectangular crystal of dimensions 0.3 x 0.1 x 0.06 mm was mounted on the tip of a glass fiber with Dow Corning silicone grease and placed in a cold N2(g) stream at 100(1) K. A total of 35238 reflections was collected of which 8434 were unique. Atoms C(34), C(32), 0(6A) and 0(8A) were heavily disordered, and were therefore refined isotropically. In addition, four of the [104]' anions are involved in a two-way positional/rotational disorder. Restraints on I-0 distances were applied (1.710 A). The displacement parameters of related oxygen atoms were constrained to be equivalent in order to minimize variables. The final refinement cycle was based on 3996 reflections with Fo>40Fo that were used to fit 727 parameters; this produced residuals of R1 = 0.1063 and wR2 = 0.2895. The goodness-of-fit index was 1.161, and the highest peak in the final difference map was 1.25 e'/A3. The extensive disorder accounts for the higher than usual R factors. [C°(b0Pd)2(H20)2][PF612 (10). Crystals of [Co(bopd)2(H20)2][PF6]2 grew as a side-product from the 1:1 reaction between [Co(CH3CN)6][BF4]2 and bptz. Slow diffusion of the reaction mixture into a tOluene solution saturated With [TBA][PF6] afforded crystals of (10) within one week. A brow" Platelet of dimensions 0.06 x 0.1 x 0.09 mm3 was secured on the tip of glass fiber with Dow Corning silicone grease and placed in a cold N2(g) stream at 110(1) K. Full- matrix least-squares refinement of 2950 reflections with Fo>40(Fo) observed reflections 47 .1“? an: - s .7 "9‘ - L.“\¢l:\.\\‘ s {V 1"“ 7 - “.....lg 51 b 3?. . ‘ Ni 9" “ORR: using 727 parameters produced residuals of R1 = 0.0561 and wR2 = 0.1275. The goodness-of-fit index was 1.020, and the highest peak in the final difference map was 0.548 e'/A3. [CU(b0pd)2(H20)2] [BF 412 (11). Crystals of [Cu(bopd)2(H20)2][BF4]2 were obtained by slow diffusion of a 1:1 ratio of [Cu(CH3CN)4][BF4]2 and bptz in acetonitrile with toluene. A single green platelet of dimensions 0.15 x 0.13 x 0.08 mm3 was mounted on the tip of glass fiber with Dow Corning silicone grease and placed in a cold N2(g) stream at 110(1) K. The final refinement cycle was based on 2607 reflections with Fo>46(Fo) that were used to fit 727 parameters. The final R values are R1 = 0.0582 and wR2 = 0.1586. The goodness-of-fit index was 1.092, and the highest peak in the final difference map was 0.595 e'/A3. [Ni2(3bPY)(CH3CN)2][N0314 (12)- Crystals of the product were grown by slow vapor diffusion of diethyl ether into an acetonitrile solution of the title compound. A dark brown prism of dimensions 0.2 x 0.32 x O. 13 mm3 was secured on the tip of a glass fiber with Dow Corning silicone grease and placed in a cold N2(g) stream at 110(1) K. A total of 8160 reflections was collected Of which 3252 were unique. The final refinement cycle was based on 2815 reflections With Fo>40(Fo) that were used to fit 199 parameters which led to R1 = 0.0416 and wR2 = 0.1054. The goodness-of-fit index was 1.087, and the highest peak in the final difference map was 1.337 e'lA3. [Cuzabpyxcnecmsl[Brill (13> I«ight green platelet crystals of [Cu2(abpy)(CH3CN)g][BF4]4 were obtained by placing an acetonitrile solution of the compound in the freezer at —4 °C for a week. A 48 i. (’0') -Q‘.‘ .\\ v “...5 u ‘fi'- 9' . . .' - ---. 1'.‘ \‘i "D;- 3‘,“ 4.x 1. {Cum light green platelet was secured on the tip of a glass fiber with Dow Corning silicone grease and placed in a N2(g) stream at 110(1) K. The data collection involved a total of 7358 reflections of which 3484 were unique. The final refinement cycle was based on 2907 reflections with Fo>40(Fo) that were used to fit 298 parameters which led to R1 = 0.0750 and wR2 = 0.2053. The goodness-of—fit index was 1.058, and the highest peak in the final difference map was 1.121 e'/A3. {[Cu(abpy)2][BF4]}e (14). Crystals of {[Cu(abpy)2][BF4]}.. grew over the period of three weeks from a solution of (13) layered with toluene. The crystals formed as dark green needles on the edges of the glass tube. A green needle of dimensions 0.05 x 0.03 x 0.12 mm3 was covered with Paratone oil, secured on the tip of a glass fiber with Dow Corning silicone grease, and placed under a N2(g) stream at 110 (1)K. A total of 11151 reflections was collected of which 2040 were unique. The final refinement cycle was based on 1096 r(iflections with Fo>40(Fo) that were used to fit 181 parameters which led to R1 = 0.0861 and wR2 = 0.2055. The goodness-of—fit index was 0.987, and the highest peak in the final di fference map was 1.361 e'/A3. [Ni4(bpt2)4(CH3CN)s][1][SbFalv (15). Single crystals of [Ni4(bptz)4(CH3CN)3][I][SBF6]7 grew over the period of one m()nth from a solution of [Ni5(bptz)5(CH3CN).o][SBF6]lo in acetonitrile that had been layered with a toluene solution saturated with [Bu4N]I. A light brown prism of approximate dimensions 0.1 x 0.08 x 0.2 mm3 was mounted on the tip of a glass fiber With Dow Corning silicone grease and placed in a cold N2(g) stream at 110 (1)K. A total of 19922 reflections was collected, of which 5202 were unique. The final refinement 49 cycle was based on 4618 data points with Fo>40(Fo) that were used to fit 396 parameters which led to R1 = 0.0741 and wR2 = 0.2283. The goodness-of—fit index was 1.092, and the highest peak in the final difference map was 2.094 e‘lA3. III. Results and Discussion. A. Self-Assembly of Molecular Squares. A.l. Syntheses of [M4(bptz)4(CH3CN)s][X]s (M = Ni2+ and Zn“) Compounds. acetonitrile [M(CH3CN)6][X]2 + bptz > [M4(bptz)4(CH3CN)s][X]s (Eq. 2) 4-8 hours M = Ni2+ ; x = [BF4]' : 70-80% M = N12+ ; x = [C104]' : 60-65% M = Zn2+ ; X = [BF4]' : 60-67% M = Zn2+ ; x = [C1041 : 36% A major focus of this study was to prepare paramagnetic complexes with nitrogen heterocyclic ligands with the bptz ligand (Figure 13a). Previous studies indicated that bptz showed promise for allowing electronic communication between metal centers of mass III in the Robin-Day scale.28 No reports of magnetic exchange using bptz have been rePorted however. With this goal in mind, we embarked on the study of self-assembly reactions of first row transition metals with bptz. Equation (2) summarizes the main reactions under investigation. 50 A1, a.“ 4 5T! 53 "‘Mr N(II) metallocyclophanes. Studies began with 1:1 reactions of [Ni(CH3CN)6][BF4]2 in acetonitrile under anaerobic conditions (Eq. 2). The reaction is essentially instantaneous as judged by a color change from a blue solution of [Ni(CH3CN)6][BF4]2 to a brown color upon addition of bptz. The Ni(II) products are stable under a variety of conditions. If the reaction is refluxed for a week, the product is obtained, unchanged, in quantitative yields. Furthermore, a 10:1 ratio of bptz to [Ni(CH3CN)6][X]2 (X = [BF4]' or [C104]') still yields the tetrametallocyclophane as indicated by mass spectrometry and X-ray crystallography. Identical reactions performed in acetone or nitromethane also yield the tetramers (vide infra) as corroborated by mass spectroscopy, but alcohols and water appear to limit the formation of metallocyclophanes; instead lower nuclearity species (monomers and dimers) or even polymers are obtained as evidenced again by mass spectrometric studies (Vide infra) and also by insoluble solids. Zn(II) metallocyclophanes. Analogous results are obtained when Zn(II) is used in place of Ni(II) in these reactions. These metallocyclophanes are synthesized from the 1:1 reaction of bptz with [Zn(CH3CN)4][BF4]2 or [Zn(H20)6[ClO4]2 in acetonitrile (Eq. 2). In both cases, the reaction solution changes from colorless to orange of addition of bptz. X-ray studies revealed that these species exist with either a (BET or a [C104]' anion in the cavity of the molecular cation. A main difference in the Ni(II) and Zn(II) chemistry with bptz was noted. There are drastic differences in the stability of these species in solution. Solutions of [Zn4(bptz)4(CH3CN)g]8+ that are allowed to stand for more than three days begin to 51 decompose with deposition of insoluble precipitates (polymers). A possible explanation is the greater lability of the Zn-N bonds, which allows for reversible coordination which could eventually lead to more insoluble oligomers/polymers with high concentrations. Moreover, unlike their Ni(II) analogues, the Zn(II) squares are sensitive to reaction conditions such as temperature, concentration and solvents. Dilute solutions favor the formation of the tetrametallocyclophane whereas highly concentrated solutions lead to insoluble materials presumably which are presumed to be polymers. Mass spectrometric studies (vide infra) indicate that the [Zna]8+ product is not being formed in solvents other than acetonitrile. For example, reactions performed in nitromethane and acetone led to only low nuclearity species by mass spectrometry. It is worth pointing out that if the solutions of [Zn4(bptz)4(CH3CN)g]8+ are stored at low temperature (0°C), the decomposition process is considerable delayed. A-Z. Spectroscopic and cyclic voltammetric studies of [M4(bptz)4(CI-I3CN)3][X]3 M = Ni, zn; x= [1317413100.]: The [Ni4(bptz)4(CH3CN)3]8+ species exhibit two characteristic electronic transitions in their UV-Visible spectra. The first one occurs at 512 nm (8 = 530 M"°cm") a"Cl is similar to a transition in the free bptz ligand, suggesting that this is a n—m’“ ligand baSled transition. The second transition at 680 nm (8 = 540 M"-cm'l) is characteristic of a I«aporte forbidden d-d transition for Ni(II) compounds. The UV-Visible spectra for the [Zn4(bptz)4(CH3CN)g]8+ salts, (2) and (4), exhibit only one transition at 540 nm with e = 270 M"-cm'l which is assigned to a bptz 1t—->7t* transition. The [Ni4(bptz)4(CH3CN)g][BF4]3 compound exhibits two weak stretches in the infrared spectrum at 2321 and 2325 cm" which correspond to the v(C_=.N) modes from 52 ..V Klu- .4L ..\. ..ka D» the bound acetonitriles. In addition, a broad and strong stretch at 1069 cm'1 is observed, which corresponds to the v(B-F) mode of the tetrafluoroborates. The [Zn4(bptz)4(CH3CN)g][X]g compounds display a characteristic v(B-F) stretch at 1054 cm' I for (2) and 1098 cm'l for a v(Cl-O) stretch in the case of (4). The expected v(CEN) stretches were not observed, however, possibly because prolonged pumping led to the loss of the ligands in the solid state, due to the fact that they maybe weak to be observed. Although previous work with dinuclear complexes of bptz28 revealed good electronic communication between metal centers, (Class II or Class 111 Robin Day behavior),29 cyclic voltammetric studies of the [Nis]8+ species do not indicate significant electronic coupling between metal centers. The compounds [Ni4(bptz)4(CH3CN)3][X]8 (X = [BF4]' or [C104]') exhibit a quasi-reversible ligand based reduction at Em = +0.4 V and irreversible waves at EN = -1.95 V and EN = -1.45 V and Ep,a = -0.62 V. In a similar fashion, the Zn(II) squares do not exhibit communication between metal centers; Compounds (2) and (4) display a quasireversible ligand based reduction at Ev. = 0.37 V and irreversible waves at EN; = -0.85 V and EN = -1.4 V followed by decomposition. It is Possible to rationalize the irreversible behavior by the fact that the tetrazine ring is not Planar which interrupts the 1: pathway for electronic communication. AC3). X-ray crystallographic results. Nim) molecular squares: [Ni4(bptz)4(CH3CN)8][X]8; X = [BF4]’, [01041' and I N i2( thZX CHJCNM I C104] 4. The molecular cation in compound (1) is presented in Figure 15 whereas Compound (3) is depicted in Figure 16. [Ni4(bptz)4(CH3CN)3][BF4]3-4CH3CN (2) crystallizes in the triclinic space group P1 and 53 1" ‘1’.- +2-”, llg)‘“ 3112:. [Ni4(bptz)4(CH3CN)g][C104]3-2CH3CN-C4H30 (4) crystallizes in the monoclinic space group P21/n. As expected, X-ray studies reveal that each Ni(II) center is in a distorted octahedral geometry with two bptz units coordinated in a cis fashion and two acetonitrile molecules completing the coordination environment. Typical angles in compound (1) are [Ni(5C)-Nil-N(1C)] = 78.0 (2)° for the bptz binding, and [N(5)-Ni(1)-N(6)] = 89.4 (5)° for the acetonitrile interactions (Figure 15b). In terms of the Ni-N distances the Ni-N(tetrazine) is the longest bond, followed by the Ni-N(pyridyl) and finally Ni-N(acetonitrile); these distances are Ni(1)-N(5C), 2.098 (5) A, Ni(1)-N(1C) 2.084 (6) A, and Ni(l)-N(5) 2.035 (6) A respectively (Figure 15b). The dimensions of the square are 6.87 A on the edge and 9.69 A along the diagonal (Figure 1 5a). The average vertex angle (0) for the compound [N i4(bptz)4(CH3CN)3][BF4]3'4CH3CN (1) is 923° which represents a deviation of 23° from the ideal angle for a square (Figure 14). It is worth mentioning that each bptz unit is distorted in order to satisfy the coordination requirements. In compound (1), for example, the tetrazine ring shows distortions ranging from 186° to 11.70° ((1)) (Figure 14). The tetirazine ring and the pyridyl are distorted from planarity as well, with angles ranging from the almost negligible 0.38o (almost coplanar) to 761° ((1)) (Figure 14). One of the most important aspects of the structure of (1) is the presence of a tetrafluoroborate anion inside the cavity. This anion has the correct surface area and Volume to fit inside the cavity, which suggests its possible role as a template in the formation of this cyclic tetramer (Figure 15a and Figure 17a).'9 A similar anion in size and shape such as [C1041 renders similar results, namely the assembly of a molecular square with an encapsulated anion (Figure 17). 54 Table 2. bond distances (A) and angles (°) for [Ni4(bpt2)4(CH3CN)3][BF413'4CH3CN (1)- Ni 1-N5 2.035(6) Ni2-N4 2.038(7) Ni 1-N6 2.045(6) N i2-N3 2.052(6) Nil-N 1 B 2.067(6) N i2-N2C 2.057(6) Ni 1-N1 C 2.084(6) N i2-N2D 2.069(6) Ni 1-N5B 2.094(5) N 12-N 3C 2.089(5) Ni 1-N5C 2.098(5) Ni2-N6D 2.107(6) N 5-Ni l-N6 89.4(2) NIB-Ni 1-N5B 77.6(2) N5-Nil-N1B 96.4(2) NlC-Ni l-NSB 88.6(2) N6-Ni1-N1B 92.5(2) N5-Ni 1-N5C 86.1(2) N5-Ni1-N1C 97.5(2) N6-Ni1-N5C 172.6(2) N6-Nil-N1C 96.9(2) N lB-Ni l -N5C 93.8(2) N lB-Nil-NlC 163.2(2) N1C-Ni1-N5C 78.0(2) N5-Ni1-N5B 173.8(2) N5B-Ni1-N5C 95.8(2) N6-Ni1-NSB 89.3(2) Table 3. bond distances (A) and angles (°) for [N i4(bptz)4(CH3CN)g][C104]g'2CH3CN'C4HgO (3). N 4B-N i 1 2.083(5) N2A-Ni2 2.089(5) N l4-Nil 2.040(6) N2B-Ni2 2.082(5) N6-Ni1 2.077(5) N12-Ni2 2.040(6) N 5B-N i 1 2.083(5) N6A-N 12 2.057(5) N13-Nil 2.029(6) N6B-Ni2 2.073(5) N2-Ni1 2.078(5) N1 1-N12 2.037(6) N 13-Nil-N14 90.5(2) N3B-N4B-Ni1 125.4(4) N 13-Ni 1-N6 97 .2(2) N6-Ni1-N4B 89.4(2) N 14-Ni1—N6 96.1(2) N2-Ni1-N4B 92.7(2) N13-Ni1-N2 174.5(2) N13-Ni1-NSB 91 .5(2) N14-Ni 1-N2 87.2(2) N14-Ni l-NSB 96.3(2) N6-Ni1-N2 78.1(2) N6-Ni l-N SB 164.7(2) N13-Ni1-N4B 90.1(2) N2-Ni1-N5B 93.7(2) N14-Ni l—N4B 174.4(2) .mocwnmo_o>oo_§oEabB 05 E San 95w: 2: 3 eoocotoaxo 209036 05 Co wEBSe ouufiozom .3 y....ME Ewan E3“ wet 655308 U 2am 325 23E panacea . xx 56 o 099' owe c Emvli mm; o ood— lthg o 05.: low.— 8 o 3.0— lvmfi o mmfill mm; o cw.olo_._ L681: wmd e . v.8 . Memo . 3e 0 2o c :56...Azuamuzaeeafi .._..emizoazuiaeeaa .._.Quizuamoiaeeaé ......aizoezoezaeeaz. Aegean—Ema Co mcercoe e8 2 oSwE 83 853?. 3.3205 05 E 92%: was 05 mo £85535 .v mink. 57 $3 53» :5 oEoEExm< 3v .ZUmIUv .556 «o 9.3 2: M8 3580 coon u>as WES“ cowoeexm .manEo b=E~noE .EaEzoamoiaeeaa E 5:8 one up 8.535.2ro 2833 afiofi 3 .2 p.53..— 58 sate—o mo 8.3 05 Sm @0388 soon 023 283 53.6sz @3082? 38.55 bagged .x. cm a? was guessed. so did .._.oaizamovaaecvaz. 5 aces as do eecaeoaoaoe 28%; afisfi E .3 25E 59 A 5:5 833885 2: as. 0:32.06.129515522. Be as zuamuvaia:Azonmuvxaeeaza 3 E 22:3 65 cc ”sedge mafia scam .: edema zoamoe.._.dm=.azo .N. :uofiaeez. co Eamae messed .2 as»: 61 .353 we 81$ 05 How eoEEo soon 96: megs comes? smogHazUamoxaeeaZ a :52 afiecca :3 us a 8:8 2: cc eceaeomoaa Eeaao aeeofi .2 can...“ 290 “up... EE' 2% «in/W 1 fit, a; I/ a 232 «la / =9 l, i . amafi. wwvoasz VA“!sz Q s s. $90 58 muz ...,an I. 71% .‘s '.. I»? it @v 532 "new =5 go 58 «Pp ago .1001 62 Table 5. Selected bond distances (A) and angles (°) for [Ni2(bptz)2(CH3CN)3][C104]4 (5). Nil-N4A 2.044 (7) Nil-N4D 2.072 (7) Nil-N1 2.069 (7) Nil-N2 2.073 (7) Nil-N4C 2.073 (7) Ni 1-N4B 2.079 (7) N4A-Ni1-N1 92.2 (3) N4C-NiI-N2 95.0 (3) N4A-Ni1—N4C 92.0 (3) N4D-Nil-N2 90.4 (2) Nl-Nil-N4C 171.8 (3) N4A-Nil-N4B 90.3 (3) N4A-Nil-N4D 177.9 (3) Nl-Ni 1-N4B 92.1 (3) N1-Nil-N4D 89.8 (2) N4C-Ni1-N4B 94.8 (3) N4C-Ni1-N4D 86.1 (3) N4D-Nil-N4B 88.9 (3) N4A-Nil-N2 90.8 (3) N2-Nil-N4B 170.1 (3) N1-Ni1-N2 78.0 (3) The cation in compound (3) exhibits an octahedral geometry about each Ni(II) center, with two bptz units and two acetonitrile molecules coordinated in a cis fashion (Figure 16). The presence of an encapsulated perchlorate anion (47 A3)'9" (Figure 17b) instead of a tetraflouroborate anion (38 A3) results in larger distortions of the ligand units as compared to the previous Ni(II) tetramer (1). Complex (3) exhibits an average vertex aF‘Igle (0) of 94.05°, which is a 405° deviation from the ideal value for a square; this is Compared to the 92.3° found in (1). The tetrazine ring also shows a larger distortion from Planarity [12.66° (m)], compared to the [BF4]° salt which is 11.67° (Figure 14). The di hedral angle between the planes of the pyridyl and tetrazine ring increases to 686° ((1)). The Ni-N distances follow the same trend as the tetraflouroborate. It was possible to isolate crystals of a minor product, namely [Ni2(bptz)(CH3CN)3][ClO4]4 (5) (Figure 19) from a filtrate after isolation of (3). In this Case, each Ni(II) center exhibits a distorted octahedral geometry with the bptz unit co()rdinated in bidentate fashion and four acetonitrile molecules. The angle for the bptz 63 binding is 78.0 (3)° [N(1)-Ni(1)-N(2)], and the average angle between the acetonitrile ligands is 90.4 [3]°. As in the case of (1) and (2), the tetrazine moiety and the pyridyl ring do not lie in the same plane. In this case there is an angle of 526° between planes of the two rings. The Ni-N distances follow the same trend as before with the longest Ni-N distance being the tetrazine ring Ni(l)-N(2) 2.073 (7) A followed by the pyridyl nitrogen Ni(1)-N(l) 2.069 (7) A; the shortest distance is to an acetonitrile ligand Ni(1)-N(4A) 2.044 (7) A (Figure 19). Zn(II) molecular squares: [Zn4(bptz)4(CH3CN)g][X]8, X = [BF4]', [C104]'. Both of the Zn(II) molecular squares exhibit a distorted octahedral geometry. Crystals of [Zn4(bptz)4(CH3CN)3][BF4]g-4CH3CN (2) are triclinic, P1 and those of [Zn4(bptz)4(CH3CN)3][C104]3-2CH3CN (4) are monoclinic, C2/c. The metric parameters Within (2) exhibit the same bonding trends as its Ni(II) counterpart, namely the tetrazine Nitrogen exhibits the longest bond followed by the pyridyl and acetonitrile; the distances are; Zn(1)-N(1A) = 2.266(5)A, Zn(1)-(5A) = 2.091(4) A, and Zn(1)-N(10) = 2.077 A (Pi gure 20b) respectively. The corresponding distances in (4) are Zn(l)-N(3) = 2.234 (4)/A, Zn(1)-N(1) = 2.144 (5) A, and Zn(1)-N(11) = 2.045 (5)A (Figure 21b). There is an inCrease in the M-N distances as compared to the Ni(II) species, as expected due to the 131‘ ger radius of Zn(II). Both [Zn4]8+ cations contain an encapsulated anion. The distances b'E=t\Jl/een the Zn(II) centers in the two squares are 7.2 A for (2) and (4) respectively (Fi gure 20 and Figure 21). The tetrazine rings in (2) exhibit a twist angle as large as 4.74° ((1)) and a torsion angle of 535° ((1)) between the tetrazine and pyridyl rings (Figure 14). In (4), the tetrazine exhibits a torsion angle of 11.92° ((0) and an angle between the planes of the tetrazine and pyridyl ring of 10.140 ((1)), which is the largest distortion among the four structurally characterized squares (Figure 14). Table 6. Selected bond distances (A) and angles (°) for [Zn4(thZ)4(CH3CN)81[BF413’4CH3CN (2)- an-N9 2.070(5) Zn2-N12 2.072(4) an-NIO 2.077(5) Zn2-Nl 1 2.082(4) an-NSA 2.092(5) Zn2-N6A 2.094(4) an-N6 2.131(5) Zn2-N4B 2.293(4) an-N4 2.248(4) Zn2-N5B 2.116(4) an-NlA 2.262(4) Zn2-N3A 2.255(4) N9-Zn1-N10 92.95(18) N10-Zn1-N4 172.5309) N9-Zn1-N5A 98.2908) N5A-an-N4 90.82(17) NIO-an-NSA 96.58(19) N6-an-N4 74.64(16) N9-an-N6 102.6708) N9-Zn1-N1A 172.9208) N10-an-N6 98.91(18) N10-Zn1-N1A 89.1606) N5A-an-N6 153.1306) N6-an-N1A 83.6506) N9-an-N4 84.9506) N4-an-N1A 93.7905) Table 7. Selected bond distances (A) and angles (°) for [Zn4(bptl)4(CH3CN)sl[C10413'3CH3CN (4)- Zn 1 -N11 1.957(8) Zn2-N10 2.01100) Zn 1 -N13 2.088(9) Zn2-N9 2.06000) Zn 1 -le 2.125(8) Zn2-N6 2.094(10) Zn 1 -N1 2.139(8) Zn2-N8 2.107(9) Zn 1 -N3 2.237(8) Zn2-N7 2.246(8) Zn 1 -N14 2.240(8) Zn2-N2 2.29900) N l l-an-N13 88.8(4) N12-an-N3 92.6(3) l l-an-N12 98.0(3) Nl-an-N3 74.4(3) N 1 3-Zn1—N12 94.7(3) N1 l-an-Nl4 90.2(3) N 1 l-an-Nl 97.1(3) Nl3-Zn1-N14 169.5(3) N 1 3-an-N1 102.7(3) N12-Zn1-N14 75.1(3) N 1 2-Zn1-Nl 157.1(3) N1-Zn1-Nl4 87.8(3) 1 l-an-N3 168.2(3) N3-Zn1-N14 97.5(3) 1 3-an-N3 85.2(3) 65 5.5.0 Co 8.3. on. 58 @0280 Son 0%; 8.8:." 5&8ng ._o>o_ bzfianoa eeow 05 as ZUmmUvaHEEEZUEUEEAEVEE E ES ocuoEEm< 3v .Zommovufimm:EZUMEUVASQDVENH E 5:8 2.: c6 ESwEe ESE—.0 Echo—rig .8 95$..— 3V 3 SE30 .8 0x8 05 c8 39:8 :03 ca; ease Emcee? as .35 £5365 a on a :38 pa 368:3 assoc... 20.52.9825.535585 a as seepage. 3v 20.5.11198 122538885 a 8:8 2: .6 same 289.... 3:55. 3 .R 2:5 2: A5 “11. “ll 50 , 27 léo Geo 1% $0 1 fix n! :6 WV 80 so Eu ' a' AC—vu |’ A," ..._. V on.“ ’ \ t/I.:NvU II\A V o! o! \o 1 “26:2 60 .4, A... S u 3 EU s82 1‘ ,1 sec ‘5 . K‘ .1. . e5. GeolIIVlMls . 3.00 t. I. 7.0. 9:... eh 1‘82 “858:0 .r 52.. a: a. ‘ I ‘.:. .1 2:04» 4% 88 .1... c o \ ”v Am—vU n AoCU AwNvU(w ._ ll. mN U ’M l _. 36 Sue «to £5 so... see A NH 830 67 Compound (2) displays an average vertex angle (0) of 93.80 (Figure 14). In the perchlorate salt (4), this angle is 974°, which is the largest deviation in the tetrametallocyclophane series, namely 7.4°. A.4. NMR studies Thus far, support for an anion template effect in this chemistry is based solely in X-ray crystallography. The question that comes to mind is do these species exist in solution with an anion inside the cavity? The diamagnetic molecular square [Zn4(bptz)4(CH3CN)3][BF4]3 is an ideal species for studying the solution behavior of these metallocyclophanes. In order to check for the presence of encapsulated anions in solution, '9F and HB NMR studies were first performed on [Ni4(bptz)4(CH3CN)3][BF4]8, but it exhibited only one broad peak in both the HB and 19F NMR spectra due to the paramagnetism of the compound. On the other hand, the [Zn4(bptz)4(CH3CN)3][BF4]3 derivative, being a diamagnetic species, is an ideal candidate for probing the behavior of these entities in solution by 19P NMR and HB NMR techniques. If the anion resides in the cavity of the cation in solution, one would expect to observe two peaks for the two distinctive type of [BET anions: a major one, that corresponds to the 7 [BF4]' anions outside the cavity and a minor one, that corresponds to the encapsulated one. The llB NMR spectrum of [Zn4(bptz)4(CH3CN)g][BF4]3 contains resonances at —l.60 ppm and —0.20 ppm. Similarly, the I9F NMR spectrum displays two resonances, a major one at -151.2 ppm and the minor one at -151.0 ppm. The relative 68 1 ll 60 °C l l N 0 °C 2‘ A"... -40 °C 1 l l 1 $ -150 -151 -152 Figure 22. Variable temperature l9F NMR spectra for [Zn.,(bptz),,(CH:,CN),,][BF,,]8 in CD3CN. 69 (I) (9 f8 1’81: 50:) integration of the peaks corresponding to the encapsulated and the free [BF4]' anions in the ”B and I9F NMR spectra are not exactly in the expected 7:1 ratio, but differences in relaxation times can account for this phenomenon. A variable temperature ”P NMR experiment was performed from —44.0 up to 80.0 °C. (Figure 22). As the spectra in Figure 22 show, there are two resonances in the temperature of ~0 °C-60 °C. Broadening occurs at higher temperature due to faster exchange of the [BET inside the cavity and the “outer-sphere” anions. At lower temperature the broadening is attributed to solubility problems. Coalescence was not reached due to limitations of the solvent temperature range. The chemical shifts that occur over the temperature range are most likely due to differences in ion-pairing interactions with temperature. The aforementioned NMR experiments provide evidence that the anions are retained in the cavity of the molecular squares in solution. With this evidence in hand, we conclude that the anion plays a role in the assembly of the molecular squares. If so, we argued, it should be possible to tune the size and shape of the metallocyclophane by the choice of the anion. In this vein, numerous anions with different sizes and shapes were attempted in this chemistry; among these are [CF3803]', [PF6]', [AlCl4]', [104]} [Barfl', X' (X = Cl', Br', 1’). None of the previously mentioned anions led to a stable metallocyclophane as corroborated by ES-MS and the lack of crystalline materials suitable for X-ray analysis. By using the anion [SbF6]', however, our goal of tuning the ring size of the oligomer was accomplished. 7O B. A New Generation of Metallocyclophanes: Molecular Pentagons. Both the [C104]' and [BF4]' anions promote the formation of molecular squares, presumably because of similarities in their sizes and shapes. Polygons of different nuclearities should be possible to obtain if the appropriate anion is used. As previously mentioned, different anions were used without success in terms of isolating a tractable product. The larger anion [SbF6]', however, allowed for the assembly of a larger polygon, namely an unprecedented pentagon. 8.1. Synthesis of [Ni5(bptz)5(CH3CN)m][Snglm [Ni(CH3CN)6][SbF6]2 was treated with bptz in a 1:1 ratio in acetonitrile which led to a color change from pale blue to dark orange within minutes. After two hours, a brownish green color persisted (Eq. 3). X-ray studies revealed the compound to be the unprecedented, partially solvated, molecular pentagon [N i5(bptZ)5(CH3CN)10][SbF6] 10'2CH3CN (6)- acetonitrile , [Ni(CH3CN)6][SbF6]2 + bptz > [le(bptz)s(CH3CN)io][SbFs]io (Eq. 3) 4 hours 80-85% yield As in the case of the [N14]8+ compounds, the [Nis]10+ pentagon is stable in solution and, in fact, the compound is obtained in good yields even after one week of refluxing conditions. Different ratios of bptz to [Ni(CH3CN)6][SbF6]2 other than 1:1 do not affect the identity of the product, but they do lead to lower yields. The results were confirmed by mass spectrometry (viole Win) and X-ray crystallography. 7l Table 8. bond distances (A) (°) for [Ni5(thZ)5(CH3CN)5][SbF6]10' 2CH3CN (6)- NiI-N16 2.035 (12) Ni2-Nl9 2.057 (14) Nil-N17 2.039 (14) Ni2-Nl8 2.054 (11) Nil-N3 2.058 (12) Ni2-N6 2.060 (11) Nil-N4 2.062 (10) Ni2-N13 2.056 (11) Nil-N7 2.068 (10) Ni2-N1 2.077 (10) Nil-N11 2.093 (12) Ni2-N14 2.066 (12) N16-Ni1—N17 91.8 (5) Nl9-Ni2-Nl3 176.2(5) N 16-Ni1-N3 96.5 (5) Nl8-N12-N13 87.0 (4) N17—Ni1-N3 92.4 (5) N6-Ni2—N 13 89.0 (4) N16-Nil-N4 174.9 (5) N19-Ni2-N1 89.8 (4) N17-Ni1-N4 89.5 (5) N18-N12-N1 176.1 (4) N3-Ni1-N4 78.5 (4) N6-Ni2-Nl 78.2 (4) N16—Ni1-N7 86.7 (4) N 18-Ni2—N 14 93.5 (4) Nl7-Ni1-N7 177.8 (5) N6-Ni2-N14 162.4 (4) N3-Ni1-N7 89.5 (4) N13-Ni2-N14 78.5 (4) N4-Ni1-N7 92.1 (4) Nl-Ni2-N14 89.7 (4) N16-Ni1-N11 93.9 (5) N20#-Ni3-N20 90.8 (10) N17-Ni1-N11 99.4 (5) N20#1-Ni3—N9 176.5 (6) N3-Ni1-N11 164.0 (4) N 20#1-Ni3-N9#1 88.9 (6) N4-Ni1-N11 90.7 (4) N20#1-Ni3-N9 176.5 (6) N7-Ni1-N1 1 79.0 (4) N9-Ni3-N9#1 91.6 (6) Nl9-Ni2-N18 92.1 (5) Symmetry transformations used to generate equivalent atoms: #1 -x+l,y,-z+1/2,#2 - x+2,y,-z+1/2 B.2. X-ray crystallographic results. As in the case of the tetranuclear metallocyclophanes, the pentagon has an anion residing in the central cavity, in this case [Sde' (Figure 23b), the presence of which is essential for the formation of the pentagonal unit. The six-coordinate Ni“ ions are coordinated to two cis bptz ligands and two CH3CN molecules in a distorted octahedral geometry. The M-N distances follow the same trend observed in the Ni(II) tetramers. The coordinated nitrogen atom of the tetrazine ring exhibits the longest Ni-N distance Ni(l)- 72 . 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It is worth mentioning that, although an ideal pentagon requires 108° vertices, the angles subtended by N-Ni-Ni edges are much smaller e.g. N(4)-Ni1)-N(7) = 92.1(4)° (Figure 25). In order to solve the problem created by using 90° disposed L-M-L building blocks to form a pentagon, the flexible bptz edges adopt 8.4° dihedral angles between the pyridyl and the tetrazine rings. In this way the overall angles between the Ni vertices of 921° + (2 x 8.4°) = 108.9° which is nearly ideal for a five-membered ring (Figure 25). B.3. Spectroscopic and cyclic voltammetric studies. The UV-Visible spectra exhibit two electronic transitions; the first one located at 510 nm (8 = 270 M"-cm") is attributed to a 1t—-> 1t* transition and a second at 690 nm (e = 260 M"-cm") is a forbidden d-d transition for Ni“. Infrared spectroscopy revealed two weak stretches at 2350 and 2354 cm'I which correspond to the v(CEN) modes for the bound acetonitrile, and weak v(C-H) stretches below 900 cm'1 from the aromatic pyridyl hydrogens. Cyclic voltammetric studies in acetonitrile revealed a quasireversible ligand-based reduction at E”: 0.28 V and an irreversible reduction at Ev,c = -l.26 V. The lack of reversibility is attributed to the distortion from planarity of the tetrazine ring. There is an average distortion of 251° out of planarity for the tetrazine ring. 77 C. Chemistry of bptz with other 3d transition metals. F 4 ‘ 2+ \ \ I // + M I, x * DIVERGENT - .4 BRIDGING DIVERGENT METAL PRECURSOR LIGAND 11+ Figure 27. Possible outcomes for the reaction between bptz with an octahedral-metal precursor. 78 In addition to Ni(II) and Zn(II), reactions of bptz with other first row transition metals were investigated. In contrast to the previously discussed metals (Ni2+ and Zn“), Mn(II), Fe(II), Co(II) and Cu(II) reactions tend to favor lower nuclearity species (monomers, dimers) as judged by mass spectroscopy or insoluble materials, although the tetranuclear product is formed to some degree as evidenced by mass spectroscopy. For example Mn(II) forms a zig-zig polymer as determined by X-ray crystallography as well as a lower nuclearity species according to mass spectroscopy studies (vide infra). The ES-MS data show evidence of the presence of the “[Mn4(bptz)4]8+” unit in the first hour of the reaction, but, with time, an insoluble product begins to be deposited at the bottom of the reaction flask. Furthermore, the ES-MS data show evidence for higher concentration of dimers and monomers in marked contrast to the solutions of Ni(II) and Zn(II), in which the molecular squares are the main species even days after the reaction has been performed. X- ray crystallographic studies of bptz products with Mn(II), Co(II), Cu(II). Reactions of Mn(II) with bptz led to the isolation of the zig-zag polymeric material { [Mn(bptz)2(CH3CN)2][BF4]2}°° (7) (Figure 28). In this compound, each Mn(II) center exhibits a distorted octahedral geometry with two bptz units coordinated in a cis fashion along with two acetonitrile ligands. As noted earlier in the case of the cyclic oligomers, the tetrazine and the pyridyl rings are not coplanar (dihedral angle = 532°) (Figure 28a) and the M-N distances follow the same trend as the metallocyclophanes with the shortest bond being to the acetonitrile ligand Mn(l)-N(4B) = 2.143 (6) A, followed by the pyridyl interaction Mn(l)-N(l) = 2.230 (5) A and finally the tetrazine interaction Mn(l)-N(2) = 2.320 (5)/31. The formation of the an+ polymer (7) points out the fact that 79 both Open and closed structures are formed in the reaction and that subtle factors such as identity of the metal, solvent and anion choice can promote one or the other of the two structures (Figure 27). Table 9. Selected bond distances (3.) and angles (°) for {[Mn(bptz)2(CH3CN)2][BF4]2}.... (7)- Mnl-N4B 2.142 (6) Mnl-Nl 2.230(5) Mnl-N4A 2.167 (6) Mnl-N2A 2.309 (5) Mnl-NlA 2.229 (6) Mnl-N2 2.320 (5) N4B-Mnl-N4A 93.7 (2) N1-Mn1-N2A 88.19 (18) N4B-Mnl-N1A 108.7 (2) N4B-Mnl-N2 168.3 (2) N4A-Mnl-N1A 101.4 (2) N4A-Mnl-N2 86.0 (2) N4B-Mnl-Nl 97.2 (2) N1A-Mnl-N2 82.77 (19) N4A—Mnl—Nl 99.2 (2) N1-Mn1-N2 71.36 (19) NlA-Mnl-Nl 145.5(2) N2A-Mn1-N2 94.77 (18) N4B-Mnl-N2A 87.1 (2) N1A-Mnl-N2A 172.4(2) N4A- Mnl-NZA 71.24 (19) It is worth mentioning another factor that should be taken into consideration in this chemistry, namely the tendency for bptz to undergo rearrangements in the presence of metal ions. For example, reactions of [Cu(CH3CN)4][BF4]2 and [Co(CHgCN)6][PF6]2 with bptz yield mononuclear complexes that contain the transformed ligand 2,5-(2— pyridyl)-l,3,4-oxadiazole (bopd) (Figure 29). The combination of an active metal and traces of water apparently promotes this rearrangement. Crystals of the compounds [Cu(bopd)2(H20)2]2+ and [Co(bopd)2(CH30H)2]2+ were obtained from layering the reaction mixtures in acetonitrile with toluene. The thermal ellipsoids plots for these compounds are depicted in Figure 29. 80 ‘ I "“3; ...) If...‘ '73 I1, 4' AMnu) N(3A) N(lA) (b) Figure 28. (a) Thermal ellipsoid diagram of a portion of the polymer {[Mn(bptz)2(CH3CN)2]2+}.. at the 50% probability level, (b) asymmetric unit. Hydrogen atoms were omitted for the sake of clarity. 81 ‘6’; (7: C(13) 5:. (a) 2 C(3) CU. C(l) I 9 ,A’ w ‘- ' ' C(4) \: ,”a - (3‘5) rm f- - 1’ ‘\ .‘1. ‘ é ‘\\\ 2 .3. \C - I ‘ ,9. (211(1) N(z) \ (’9 0(1) (b) Figure 29. Thermal ellipsoid drawing of the mononuclear complexes (a) [C0(b0pd)2(CH3OH)2][PF6]2 and [Cu(bopd)2(H20)][BF4]2 (b). Thermal ellipsoids are drawn at the 50 % probability level. Hydrogen atoms were omitted for the sake of clarity. 82 D. Electrospray-MS studies of bptz reactions with Mn“, Fe“, Co“, Ni“, Cu2+ and Zn“. The metal/bptz products for Mn(II), Fe(II), Co(II) and Cu(II) were studied by the Electrospray mass spectroscopy technique. The following reactions were studied (Eq. 4). acetonitrile . [M(CH3CN)6][CIO4]2 + bptz > [M4(bptl)4(CH3CN)3][(310413 (EQ- 4) (M = Mn2+, Co“, Cu”, Fe“) As mentioned earlier, the polymeric material {[Mn(bptz)2(CH3CN)2][BF4]2}.. (Figure 28) was isolated in low yield (30%), but we were not able to isolate a cyclic oligomer (Figure 24). Mass-spectral studies of aged solutions of Mn(II) ions and bptz do not indicate the presence of tetranuclear products, but instead reveal the presence of monomers and dimmers. If MS data are collected immediately after the reaction has been performed, however there is evidence for the presence of [Mn4(bptz)4][ClO4]77+ (m/z = 1856.66) (Figure 30). One hour later, the same solution does not exhibit any signs of the molecular square. The yield of the insoluble materials (polymer) is low (30 %), after several hours, but afterseveral days, the yield increases to 50 %. These observations point to a lack of stability of the square [Mn4(bptz)4(CH3CN)g]8+ which evidently decomposes into the polymeric form. The Co(II), Fe(II) and Cu(II) analogues follow the same trend as Mn(II), as noted in Figures 31, 32 and 33. There is an indication of the formation of [M4(bptz)4][ClO4]7+ (M = C0“, Fez“, Cu“) species, immediately after the reaction has been performed (Figure 31, 32, 33). An hour later, the signal for the parent ion has disappeared and only lower nuclearity species are observed. 83 The solution data are compelling evidence that a major factor in controlling the outcome of these reactions is the metal identity. One could attribute this behavior to ion size. For example a large cation such as Mn(II) may not form a stable cyclic entity because the cavity inside the molecular square is too large for the [BET or [C104]' to have the same stabilizing effect as they have with Ni(II) and Zn(II). In the case of Cu(II), the Jahn-Teller distortion could play a predominant role in the instability of the metallocyclophanes because of the weak interactions along the axial sites of the metal center. Finally, cations such as Co(II), Fe(II) may exhibit lower lability to their M-N bonds than Ni(II) or Zn(II); consequently, the self-healing mechanism that takes place in the high-yield assembly of the cyclic species may not be occurring. In these cases the kinetic product (polymeric form) would be favored instead. Electrospray mass spectroscopy studies performed on solutions of [Nl4(bp[Z)4(CH3CN)3][X]3 and [Zn4(bptz)4(CH3CN)g][X]g, where X = [BF4]' or [C104]', in acetonitrile revealed the parent ion [l\/I4(bptz)4(CH3CN)g][X]7+ (M = Ni2+ or Zn”) and several fragmentation peaks (Figure 34). These species were detected in a solution that had been standing for more than a week, which is good evidence for the stability of these metallocyclophnes in solution. The MS data in Figure 34 indicate that the products of the perchlorate salts are more stable in the gas phase than the [BET salts in that less fragmentation is observed for the perchlorate derivatives (3 and 4) (Figure 34 b and c), than for the tetrafluoroborate compounds (Figure 31a). Compound (2) is not stable enough in the gas phase to allow for the observation of the parent peak ([Zn4(bptz)4][BF4]7+). 84 ; 10th 3 a 8 0 8= 3. _ n_1 '6 O = 5 50‘ 8 ea c a ... a 3 8 ‘g '2 3' " 2. a 8 “J A 3 0 9 E —> g l ' ' 1 ‘ r c .1“: 1855 1865 1875 1856 1860 1864 3 O a 5 Mass (mlz) Mass (mlz) v L. “+ [Mna(bpt2)21[C|04ls:(*)[MndbpmsllClOJr' 11111409184100.»1 [antbptzlaltmoae 1") , * ‘ r v 4 [MndbplzlsllClodv l * *4! It 4. - ~ - ~1L__.___“- -* —— A .L 800 1000 1200 1400 1600 1800 Mass (mlz) 1873.38 [MmtbptZMIClOJf 1856.6. (saunas) leufits net 1 809.47 1700 1750 1800 1850 1900 Mass (mlz) Figure 30. ESI-MS spectra of the 1:1 reaction between [Mn(H20)6] [C104]; and bptz taken after 10 minutes 85 8 9 (munoo) IBUB!S u0| (%) eauepunqv Icogeioeql 01 ¢ 11 W ' V 18175 1,885 1872 1876 1880 Mass (mlz) Mass (mlz) 0.. [004(bptzl4][C|0d7+(*l .. , 1:..‘7 600 800 1000 1200 1400 1600 1800 Mass (mlz) ‘51 § [Coxbptziatcmr = m 3 _. E8 2 1760 1780 1800 1820 1840 1860 1880 1900 Mass (mlz) Figure 31. ESI-MS spectra of the 1:1 reaction between [Co(H20)6] [C104]; and bptz taken after 10 minutes. 86 100 (%) aauepunqv [80119109111 U! o (siunog) [eufigs uoI L 1.1111 11 1,860 iL87O 1860 1870 Mass (mlz) [Fe4(bptz)4] [(310417+ (swung) [eufigs HO] O 1.- ll L AA _ A ... A J A L *A 600 800 1000 1200 1400 1600 1800 Mass (m/z) [Fe4(bptz)4] [C104]; 1852.72 * 1000 1400 1800 2000 Figure 32. ESI-MS spectra of the 1:1 reaction between [Fe(H20)6] [C104]; and bptz taken afier 10 minutes. 87 100 A 1. 9 S e _, s .9 s1 5 e 9 8 ‘5 8' S: 50 E - 2 8. P. 89 1 H a 011'.“ lili.. 3 ‘ 1,890 1,900 1890 1900 5. Mass (mlz) L’L [C “4(thZ)4l [C104]? .214 J... _._M__--- --_; .._ _.\_: 600 800 1000 1200 1400 1600 1800 Mass (mlz) 7 391 .77 ICII4(bptZ)4] [C104]7+ [CII'.1(bptZ)11[00415+ 1888.68 * [Cus(bpt2)2] 1010.1: + * [Cu4(bptz)3]|ClO4]-; 1652.60 1 1000 1200 1400 1600 1800 2000 Figure 33. ES] spectra of the reaction between [Cu(H20)6][ClO4]2 and bptz taken after 10 minutes. 88 3" 100' Simulated Experimental 8 e- 3 3 § 8 i 501 '3 E ’5 a a i a - ’03 0 . r 1,780 1,790 1,800 1780 1790 1795 M Mass (mlz) Mass (mlz) 600 800 1000 1200 1400 1600 1800 a 511 00 ‘ Simulated 3 Experimental :1 g = (g — 2 3 1 5 5° ‘6 m s 8 — a. : ... 3 E I ll 0 , 8 0. - w , g 4 § 1,8701,8801,890 1870 18801885 5. L ,_ - H AMass (mlz) Mass (mlz)] .. . , , , . , 800 1000 1200 1400 1600 1800 -1 . g 100 Simulated 13 Experimental 3 ca g- a '1 , i- ? 5° ‘8 1 .1. . 5 0 . 0.4. .v - 3 1,780 1,790 1,800 1780 1790 1795 M H" “m" Mass (mlz) Mass (mlz) 600 800 1000 1300 1400 1600 1800 Mass (mlz) Figure 34. ESI-MS spectra in acetonitrile of the metallocyclophanes (a) [Ni4(bptz)4(CH3CN)8][BF4]8: (b) [Ni4(bptz)4(CH3CN)8][ClO4]Sa and (C) [Zm(thZ)4(CH3CN)s][BF4]8. 89 886888 a 82686 e..memzogznoamozaaeaz. 65.888 685:8 as .8 868. 33$ .8 953... :oEoE 6. :m N_ aNEP; m0“: 3} k .2 U .2 J comm ooo_o comm ooom oom... ooow 11‘ 1. l “tit. 11 l «:1. ..._.EEEESV .2. 3:; mass. 3:: mums. ooom oomm omo.m o_.o.m oood oomd oomd - m o n U o w m w m ..m. .1 n S ..._ a m n n om m n .m .6 m w .m T A .m .. Equatooxm noon—2.5m oov 90 62 888 2: a 886% mean .88 9: .8828 8886 5 .298ofofoiaaeazo 8 888. 92$ .8 2:5 3:: 5.82 9mm: 8% es: E: mefi 8M: 0%: ex: at: mom: ON: EONEUmEU lOmflU nflUOnflU mm: owwo ohm: mom: mom: ZUMEU (swung) [eufigs an] 91 Solutions of [Ni5(bptz)5(CH3CN).o][SbF6]to (6) clearly show the signal for the parent ion [Ni5(bptz)5][SbF6]9+ at 3584 mass units (Figure 35). In addition, there are numerous fragmentation peaks corresponding to [Nia], [Ni3] and [Niz] species, as it can be observed in Figure 35. All X-ray structures of the metallocyclophanes were performed on crystals grown in acetonitrile. A question that comes to mind is whether they exist in other solvents besides acetonitrile. Electrospray mass spectroscopy is an excellent technique for probing this question. Since the perchlorate salts were already known to be more stable in the gas phase (as noted earlier), ES-MS studies of these salts in different solvents were performed. Reactions of [Ni(HzO)6][ClO4]2 with bptz in a 1:1 ratio were performed in aprotic solvents such as nitromethane and acetone and evidence for the formation of the tetramers was obtained by mass-spectrometry (Figure 36). On the other hand, protic solvents such as alcohols or water do not promote the formation of the metallocyclophanes, instead only lower nuclearities were observed. F. Interconversion of the [Nis]10+ and [Ni4]°”. With all of the above mentioned data in hand, the evidence for the predominant role of the anion in the assembly of these metallocyclophanes was compelling. Similar anions, in terms of size and geometry such as [BF4]‘ and [ClOJ yield tetramers whereas the larger anion ([SbF6]') produces the pentamer (6). Armed with this knowledge, we asked ourselves if it was possible to transform the pentamer into the tetramer by treating a pure sample of [Nis]10+ with an excess of tetrafluoroborate or perchlorate in order to exchange the [Sng]', or to transform the [Nia]8+ molecule into the [Ni5]'°+ compound by reacting it with an excess of [Sde'. In order to test this hypothesis, two different 92 approaches were taken. In one case, a large excess of tetraflouroborate was added to a solution of [Ni5(bptz)5(CH3CN)lo][SbF6]10 and allowed to stir for several days. In order to obtain crystallographic evidence for the outcome, layering experiments were performed and crystals were obtained. The results showed that the transformation to the tetramer [Ni4(bptz)4(CH3CN)g][BF4]3-4CH3CN (1) had occurred. With the same idea in mind, experiments were performed with a mixture of [TBA][BF4] and [TBA][PF6] which lead to the isolation of the mixed anion salt [Ni4(bptz)(CH3CN)3][BF4][[PF6]3[SbF6]4-CH3CN (8) (Figure 37). In this salt the only [BF4]’ anion that is present is the one inside the cavity of the tetramer. Presumably, the [Sde' and [PF6]' anions are too large to occupy the cavity reside and, therefore, in the interstices between the squares. It was found that the transformation of the molecular squares into the pentagon is not as facile as the reverse reaction. A layering of [Ni4(bptz)4(CH3CN)g][BF4]3 or [Ni4(bptz)4(CH3CN)g][ClOdg in acetonitrile with a saturated solution of [BU4NHSbF6] afforded only crystals of the tetramers. The lack of a transformation was corroborated by mass spectrometry. In order to attempt to force this transformation, a large excess of [Bu4N][SbF6] was added to a solution of [Ni4(bptz)4(CH3CN)g][ClOdg in acetonitrile (> 50:1 ratio) and the solution was refluxed for two days. Mass spectrometric studies revealed the transformation of the tetramer into the pentamer was successful in this case (Figure 39). The fact that the transformation of the pentagon into the square takes place under less forcing conditions is a good indication that the square nuclearity is more stable than its pentagon counterpart. 93 Table 10. Selected bond distances (A) and angles (°) for [Ni4(thZ)4(CH3CN)8][BF4][PF6]3[SbFol4'CH3CN (8)- Nil-N6 199(3) Nil-N3 210(2) Ni l-N5 208(2) Ni 1-N4 2.10(2) Ni l-N2 2.09(2) Ni l-Nl 210(2) N2-Ni1-Nl 76.9(9) N3-Ni1-N4 77.6(8) N2-Ni1-N3 88.7(10) N4-Ni1-Nl 95.1(8) N2-N i 1 -N4 92.6(9) N5-Ni l -N 1 91 .0(9) N3-Ni1-N1 163.7(11) Table 1 1. Selected bond distances (A) and angles (°) for [N i4(thZ)4(CH3CN)8] [C104] [10417'2CH3CN (9)- Nil-N14 2.045(14) Ni2-N 12 204(2) Nil-N13 2.043(13) Ni2-N7 2.061(17) Ni l-Nl 2.065(13) Ni2-N6 2.075(16) Ni 1-N8 2.068(15) Ni2-N9 2.073(14) Nil-N10 2.088(15) Ni2-N11 2.084(16) Ni l-N2 2.096(13) Ni2-N5 2.085(14) N14-Ni 1-N13 86.2(6) Nl2—Ni2-N7 96.5(6) N14-Nil-N1 93.5(6) N12-Ni2-N6 92.6(6) N13-Ni l-Nl 93.6(5) N7-Ni2-N6 162.9(5) N14-Ni1-N8 94.1(6) N12-Ni2-N9 173.2(6) N13-Ni1-N8 92.5(5) N7-Ni2-N9 77.3(6) N1-Nil-N8 170.6(5) N6-Ni2-N9 94. 1(5) Nl- Ni 1 -N10 171.9(5) N12-Ni2-N1 l 90.0(6) N l - Ni l-NlO 92.6(6) N7-Ni2-N1 l 99.9(6) Nl-Ni 1-N10 94.6(5) N6-Ni2-Nl 1 945(6) N8-Ni1-N10 7 8.0(5) N9-Ni2-Nll 88.3(6) Nl4-Ni 1 -N2 87.7(5) N12-Ni2-N5 91.1(6) N13-Ni1-N2 170.0(6) N7-Ni2-N5 87.7(5) N l-Ni l-N2 78.9(5) N6-Ni2-N5 77.7(5) N8-Ni l-N2 95.8(5) N9-Ni2-N5 91.5(5) N 10-Nil-N2 94.6(5) N1 l-Ni2-N5 172.1(7) A good example of demonstrated by the the predominant role of the anions in the self-assembly is addition of 50 equivalents of [Bu4N][IO4] to a solution of 94 I 5"? 9.4 ‘0... 5 ‘ ...-.-. ‘ IA ‘1‘ Figure 37. (a) Thermal ellipsoid drawing of the [Ni4(bptz).4(CH3CN)3][BF4][SbF6]6+ unit in [Ni4(bptz)4(CH3CN)g][BF4][PF6]3[SbF6]4 with 50% probability ellipsoids, (b) space filling diagram and (c) asymmetric unit. Hydrogen atoms have been omitted for the sake of clarity. 95 (a) (b) A‘ c 2 w“?! ” { Co) I»? S // u. 3’ Na)! ”('0’ “ C(26) " N(l3 C(32) {7" ’Q‘ ‘1‘ )C(31) . 5" I : C(13) '1' C(23) C(27) N(ll) lli at) 4': l ' " ‘v ”(12 (é \ C /, N(2) ' v I‘ll; 5 C(29) \ " t", ‘ ‘4 p10) a- " ~“ \/ C(8) / ‘ J ' C(30) '_\ am A a. Na .‘ C(24) A ‘2 ' ’ C(21 c 2 N". (m C) 0(9) r w} ‘5’ C(10) I C(23) C(33) C(22) (C) “34"“ Figure 38. (a) Thermal ellipsoid drawing of the [Ni4(bptz)4(CH3CN)g] [C104] [I04]6+ unit in [Ni4(bptz)4(CH3CN)g][C104][104]7 with 50% probability ellipsoids, (b) space filling diagram that emphasizes the molecular volume of the perchlorate versus the periodate and (c) asymmetric unit. Hydrogen atoms were omitted for the sake of clarity. 96 [Ni4(bptz)4(CH3CN)3][C104]3. The initial goal of the experiment was to obtain metallocyclophanes of nuclearities other than four or five. The outcome of the reaction, however, was the molecular square [Ni4(bptz)4(CH3CN)3][C104][104]7 (9) (Figure 38). Although the solution was saturated with [104]' the compound retains a [ClO4]' inside the cavity and exchanges only the outer anions. E.S-MS studies of interconversion reactions. Another aspect of this chemistry investigated by mass spectrometry is the conversion of [Ni5(bptz)5(CH3CN)1o][SbF6]10 the pentagon into the molecular square in the presence of an excess of either [BF4]‘ or [ClO4]'. This conversion was accomplished easily as previously mentioned and confirmed by X-ray crystallography, but the reverse transformation from the square into the pentagon did not take place under similar mild conditions. A reaction that involved addition of a large excess of [Bu4N][SbF6] to a solution of [Ni4(bptz)4(CH3CN)3][C104]g with two days of reflux was followed by ESI-MS. As indicated by the data in Figure 39, the solution contains only [Ni4(bptz)4(CH3CN)g]8+ in the earlier stages of the reaction (Figure 39a). After two days (under constant refluxing), there are signs of [Ni5,(bptz)5(CH3CN).o]10+ (Figure 39b), but the conversion is not complete. These data suggest that the molecular square is more stable that the molecular pentagon. 97 dos—:8 :25 05 3:829: 3V Ea sass 2: do 23% was 05 message 3 %oazxzvnmoiaaeaa a 8:28 wads—m2 m 9 Homnm= 1t* transitions. The compound [Ni2(abpy)(CH3CN)2(NO3)4] (12) displays only one electronic transition in the UV-Visible range, namely at Am” = 344 nm which is assigned to an MLCT band given the e value of 1.8 x 104 L(mol°cm)". Its counterpart [Cuz(abpy)(CH3CN)3][C104]4 (l3) exhibits a similar transition at 351 nm with e = 1.5 x 104 L(mol-cm)"along with a second electronic transition at higher energy, km,“ = 230 nm, e = 2.0 x 104 L(mol'cm)". The cyclic voltammogram of [Ni2(abpy)(CH3CN)2(N03)]4 (12) in acetonitrile exhibits two oxidation features at Ep,a = +0.62V and Ep,a = +0.4V with no associated return waves. In addition there are three reversible reductions located at EV, = -0.10V, Ev, = -0.4V and E9, = -0.9V. 100 The dinuclear Cu(II) (13) compound also exhibits a rich electrochemistry with an irreversible oxidation at Ep,a = +1.10 V, reversible reductions at E), = 0.65V, En, = +0.40V and a quasireversible reduction at Er), = 0.0V. G.3. X-ray Crystallographic studies. The molecular structure of [Ni2(abpy)(CH3CN)2(N03)4] (12) is based on a distorted octahedral geometry around the metal centers (Figure 40). Each nickel(II) center is coordinated to one bidentate and one monodentate nitrate, an acetonitrile molecule, and an abpy ligand. Table 12. Selected bond distances (A) and angles (°) in [Ni2(abPY)(CH3CN)2(N03)4]'2CH3CN (12). Ni 1-06 1.990(2) Ni 1-03 2.106(2) Ni l-Nl 2.037(2) Ni 1-N2 2.121(2) Ni l-N5 2.044(2) Ni 1-02 2.125(2) N5-Ni1-O3 8669(9) N5-Ni l-N2 170.06(8) O6-N i l-N 2 9556(8) O3-Ni l-N 2 101.99(8) N1-Ni1-N2 7645(9) N 1 -Ni 1-03 l62.44(8) O6-Ni l-Nl 105.01(8) O6-Ni 1-02 153.92(7) O6-Nil-N5 8882(9) N1-Ni1-02 101.0l(8) Nl-N i l-N 5 9380(9) O3-Ni 1-02 61.43(8) O6-Ni 1-03 9255(8) N 2-Ni 1-02 8874(8) N5-Ni1-02 91 .24(9) The Ni-N distance to the acetonitrile ligand is 2.044 (2) A which is essentially the same as the distance in [Ni2(bptz)(CH3CN)3][C104]4; (Ni(l)-N(5), 2.044 (7)A) (Figure 19). The azo nitrogen distance to Ni(II) is the longest of the three Ni-N interactions at Ni(1)-N(2) = 2.121 (2)A. Compared to a similar type of interaction in [Ni2(bptz)(CH3CN)g][C104]4 in which there is a tetrazine ring instead of an azo linkage, this interaction is 0.04 A longer. 101 The angles within the coordination sphere also provide some helpful insight into the distortion of the ligand environment of this compound. The binding angle for the chelating nitrate O(3)-Ni(1)-O(l) is 61.43 (8)°. The angle between the pyridyl and the acetonitrile ligand is close to the ideal value for an octahedron, (N(5)-Ni(1)—N(1) = 93.80 (2)°). The binding angle of abpy, N(1)-Ni(l)-N(2) of 76.45 (9)°, is very close to angles of coordinated bptz in [Ni2(bptz)(CH3CN)3][ClO4]4 78.10 (3)°. The two Ni(II) atoms are 4.942 A apart, which is much shorter than the corresponding distance in [Ni2(bptz)(CH3CN)g][ClO4]4, (6.904A). An important feature to note in the structure of (12) is the elongation of the N=N bond by 0.025%. with (N(2)-N(2#) 1.271 A), compared to the corresponding value in free abpy, (1.246 A)“ This phenomenon indicates n-back donation from the Ni(II) centers into the 1r* (abpy) orbital. This effect has been previously noted for coordination complexes of abpy with Cu(I).32 Table 13. Selected bond distances (A) and angles (°) for [Cu2(abpy)(CH3CN)g][BF4]2 (13). Cul-N4 2.004(5) Cul-N6 2.318(5) Cul—N 3 2.007(5) Cul-N2 2.403(5) Cu 1 -N5 2.029(6) Cu 1 -N1 2.032(5) N6-Cu1-N 2 166.00(18) N3-Cul-N6 94.4(2) N4-Cul-N3 l74.83(l9) N5-Cul-N6 87.0309) N4—Cu1-N 5 91 .6(2) N l-Cu 1 -N6 94.59(19) N3-Cu1-N5 86.9(2) N4-Cul-N2 86.35(18) N4-Cu1-Nl 89.5(2) N3-Cul-N2 89.35(19) N3-Cul-Nl 91 .8(2) N5-Cul-N2 106.66(18) NS-Cul-Nl 178.01(l9) Nl-Cul-N2 71.79(18) N4-Cul-N 6 90.4 1(19) [Cuz(aszy)(CH3CN)g][BF]4 (13) exhibits typical parameters for a Cu(II) metal center in an distorted octahedral environment. It displays a Jahn-Teller distortion which 102 corresponds to the Cu-azo nitrogen interaction, Cu(I)-N(Z) 2.403 (5)A and the Cu-N acetonitrile interaction Cu(I)-N(6) 2.318 (5)A along the z axis (Figure 41). The other four coordination sites are filled by three acetonitrile molecules, which exhibit an average Cu(I)-N distance of 2.013 [5] A, and the pyridyl ring, Cu(l)-N( 1) 2.032 (5) A. The L-Cu- L binding angles are distorted from the ideal 90 or 180 ° expected for an octahedron. The angles N(2)—Cu(1)-N(5) = 106.6 (2)° and N(2)-Cu(1)—N(1) = 71.8 (2)° are typical values. The N-N distance in the azo group N(2)-N(2A), 1.277 (1) A is indicative of it back- donation from the Cu(II) center into the 71* (abpy) orbital. This distance is 0.03 A larger than the one found in free abpy, which is 1.246 (2)A.3 ' The Cu(II) centers are separated by a distance of 5.408A, which is 0.46 A longer that the corresponding separation in the Ni(II) case, as expected for a larger metal radius. Table 14. Selected bond distances (A) and angles (°) in {[Cu(abpy)2][BF4]2}.o (14). Cul-N4 1.934(9) Cul-Nl 2.060(9) Cul-N3 2.009(9) N3-N3A 1.300(16) Cul-N2 2.009(9) N3-C9 1.396(13) N4-Cul-N3 146.5(4) N2-Cu1-N1 135.6(4) N4-Cul-N2 117.1(4) N3-N3A-Cu1 115.7(9) N3-Cu1-N2 79.5(3) C9-N3-Cu1 129.0(7) N4-Cu1-N1 77.8(4) Cl-Nl-Cul 131.2(7) N3-Cu1-Nl 111.9(3) CS-Nl-Cul 113.0(7) Finally, {[Cu(abpy)2][BF4]2}m (14) is a 1-D polymer with Cu(I) ions instead of Cu(II). As expected for Cu(I), the metal center exhibits a distorted tetrahedral geometry (Figure 42). This is illustrated by the angles observed between the pyridyl-azo, N(3)- Cu(1)-N(1) = 111.9 (3)°, and the two pyridyl groups N(1)-Cu(1)-N(2) = 135.6 (4)°, which are far from the ideal 109.5° for a tetrahedron. The distance N(3)-N(3#) = 1.300 A 103 SHE—o go 813 05 88 “82:80 noon 9:2 383 some—i: .65. 5:33th 8% 05 “a a: zummom.Emozfizommovaoesmz co 83 283:... some: .3 2:3..— ad 4“ .\\.. s t ..., 104 .5520 m0 913 05 88 8338 58 2: wage 586% 5:538 soon a a: .Ea..Azunmoxaesso. 5 e88 2.. no 6:. 289% 3:55. .=. 2:3... $5 “a. 85 \M. So ..\ 3 0 mg i 56 $2 N. :8 6o . . . 50 \ x V. .../4 105 .Emno ocoioo 2: ..o 5:8 86:25 5 3v 1 Hemmzfiooseu: 6.58 es 5 as 223 a: do so... 283:». .25.: 3 d. 2:3..— N .52 .. - .- 2:8 «0. 266. .- '. .52 AU 232 , (v. 106 to the azo group is evidently involved in appreciable 7t back-donation from the Cu(I), as expected for an electron rich (1‘0 center. The N=N distance is 0.054 A, which is nearly twice the lengthening observed for the Ni(II) and Cu(II) complexes. IV. Future work Reactions of the metallocyclophanes. In our search for supramolecular compounds with interesting properties, an interesting family of metallocyclophanes was isolated. A close look at the structures reveal the presence of two acetonitrile ligands on each metal center as emphasized in Figure 43. Substitution of these molecules by organic linkers may allow the formation of higher nuclearity species (Figure 43). With this goal in mind, several bridging ligands were reacted; these include 1,4’ phenyldiamine, pyrazine, cyanide, 4,4’-azo-bipyridine, 2,2’-bipyrimidine, 4,4’-bipyridine, 1,4’-benzonitrile and thiocyanide. Reactions of [Ni4(bptz)4(CH3CN)3][BF4]3 with a large excess of either [Bu4N][CN1 or bpym led to the isolation of the compounds [Bu4N]2[Ni(CN)4] and [Ni(bpym)3][BF4]2 as verified by X- ray crystallography. Halides (Cl', Br' and I') react to yield insoluble species in acetonitrile. The reaction is effectively instaneous, and IR/spectral analyses of the precipitates reveal the disappearance of the v(CEN) and v(B-F) modes that are normally observed for [Ni4(bptz)4(CH3CN)3][BF4]3. It is worth mentioning at this point, that reactions of the pentagon with halides are much slower, with eventual precipitation of an insoluble precipitate that lacks CEN stretches. Moreover, in the case of reactions of the pentagon [Ni5(bptz)5(CH3CN)lo][SbFo]lo with I', there is more than one product. After the initial insoluble solid is removed, the remaining light green solution affords crystals when 107 layered with toluene. The crystals are the unexpected compound [Ni4(bptz)4(CH3CN)3][I][SbF6]7 (Figure 44) in which the central cavity is occupied by an iodide atom. The iodide ion is another anion which has the correct size to occupy the cavity of the molecular square. Attempts to synthesize this compound by using NiIz as the source of Ni(II), led to only an insoluble, material which is either a polymer or a neutral square. Other organic linkers that appear to react with the [Ni4]8+ square are isocyanide and oxalate. In both cases, there is a disappearance of the characteristic v(CEN) mode with precipitation of insoluble products. This can be attributed to the formation of either neutral species that are insoluble in acetonitrile or molecular grids, which would not be soluble. Unfortunately, attempts to obtain crystals by layering experiments or by slow vapor diffusion were unsuccessful. Table 15. Selected bonds (A) and angles (°) for [Ni4(bptz)4(CH3CN)g][I][SbF6]7 (15). Ni 1-N6 2.026(10) Ni 1-N4 2.098(10) Nil-N3 2.052(11) Nil-N1 2.100(11) Nil-N2 2.066(9) Nil-N7 2.130(17) N 6-Ni l-N3 96.7(4) N2-Ni1-N l 78.1(4) N6-N i 1-N2 174.2(4) N4-Nil-N1 94.6(4) N 3-Ni l-N 2 89. 1(4) N6-Ni1-N7 90.4(5) N6-Ni l-N4 91 .9(4) N3-Ni1-N7 94.3(4) N3-Ni1-N4 79.0(4) N 2-Ni 1 -N7 88.4(4) N 2-Ni 1-N4 89.9(4) N4-Ni l-N7 173.1(4) N6-Ni l-Nl 96.2(4) N 1 -Ni l-N7 91 .5(4) N3-Ni1-Nl 165.8(4) Symmetry transformations used to generate equivalent atoms: #1 -x+2,-y,z ; #2 x,-y,-z #3 -x+1,-y,z; #4 -x+l,y,-z; #5 -x+1,y,-z+1 Other organic linkers that were used in pursuit of linked metallocyclophanes are 1,4 disubstitued benzenes, such as 1,4 benzonitrile and 1,4 phenyldiamine. These ligands 108 H 3C—CE /\ H/ K... I A=BorCl X=ForO' M = Ni2+ or an+ Each comer of the square has two acetonitrile molecule that can be substituted by an organic linker Each comer of the pentagon has two acetonitrile molecules that can be substituted by an organic linker Figure 43. Schematic drawing of the molecular square and pentagon with indicated sites for substitution. 109 N(6)1\", C(15) p ’1 C(14) \k‘. \\, I 5- 81888 8:588 81' \ / §\\ ‘\\\. :5 \\ \ 3‘. \\\;\\‘ ‘ ‘\\\ .5 § 8} 83358 5,) 88%,1 5- V 1% t: N") Figure 44. (a) Thermal ellipsoid plot of the cation in [Ni4(bptz)4(CH3CN)3][I][SbF6]7 (15) at the 50% probability ellipsoid level, (b) space filling diagram with the iodine anion inside the metallocyclophane and (c) asymmetric unit. Hydrogen atoms have been omitted for the sake of clarity. 110 did not react swiftly as was the case for reactions of halides or cyanide, but, under refluxing conditions for 4 hours, there was a noticeable color change. Layering experiments and slow vapor diffusion have thus far been unsuccessful in leading to single crystals growth. IR data of the products reveal an absence of nitrile stretches, indicating that the substitution of the acetonitrile molecules has occurred. Finally, the use of neutral ligands such as pyrazine, 4,4’-azo-bipyridine and 4,4’- bipyridine do not appear to react with [Ni4(bptz)4(CH3CN)3][BF4]3 in acetonitrile, even with a large excess of the ligands under refluxing conditions. Reaction solutions afforded crystals of only the starting materials [Ni4(bptz)4(CH3CN)3][BF4]3 and the linking ligand. V. Conclusions The metallocyclophanes presented in this work are outstanding examples of how subtle factors such as anion choice, solvent and metal identity can lead to differences in self-assembly reactions. Molecular squares ([Ni4]8+ or [Zn4]8+) and the pentagons ([Ni5]‘°+) are obtained in good yields when the precursor salts that contain tetraflouroborate, perchlorate or hexaflouroantimonate anions are reacted in 1:1 ratio with bptz. In addition to acetonitrile, other solvents such as nitromethane and acetone allow for the formation of these metallocyclophanes as evidenced by ESI-MS (Figure 36). These results are attributed to the match between the size of the cavity formed by the [M4] or [M5] cyclic unit and the anion.19 The tetramers [Ni4(bptz)4(CH3CN)3]8+ and [Zn4(bptz)4(CH3CN)8]8+ have a cavity size that is well-matched with a [BF4]', [CIOJ and [I]'.19a The use of a much larger anion, [Sde' (71 A3),'9a led to the pentagon metallacyclophane, [Ni5(bptz)5(CH3CN)lo][SbFo]10'2CH3CN (6). On the contrary, when anions such as, [CF3803]', B{C6H3(CF3)2}4', [PF6]’, [AlCl4]‘, [N03]' and [SO4]2‘ were 111 used, the formation of [M4]8+ and [M5]'0+ entities is precluded; instead lower nuclearity or polymers are assembled. Molecular pentagons versus squares can be favored, in solution and in the solid- state simply by altering the anion present in solution. Transformations between molecular square [Ni4(bptz)4(CH3CN)g]8+ and the molecular pentagon [Ni5(bptz)5(CH3CN)m]l0+ can be achieved by adding an excess of the anion needed for the assembly; [Sde' for the first case and [BF4]’ or [ClO4]' for the second. The fact that the nuclearity of these macrocyclos can be interchanged is excellent evidence of the predominant role of anion as a template. The conversion of the pentagon into the square takes place under mild conditions whereas the opposite (square —> pentagon) requires refluxing for two days (Figure 39). These results indicate that the squares are more stable than the pentagon. The diamagnetic tetramer [Zn4(bptz)4(CH3CN)g][BF4]3 allows for the study of these entities in solution by means of l9F NMR and 1'B NMR spectroscopy. Both NMR experiments show two peaks, one corresponding to the encapsulated and the other to the exterior [BF4]' anions, thereby proving the existence of these entities in solution. Coalescence could not achieved in a variable l9F NMR experiment, presumably due to the formation of aggregates between the metallocyclophanes in solution when the temperature is varied (Figure 22). Mass spectrometric studies of the products of different Ni(II) salts ([Ni(CH3CN)6][X]2 X = anions) with bptz show that only those reactions that involve the [BF4]', [C104]', [SbF6]' anions yield tetramers or pentamers respectively; all others appear to be leading only to lower nuclearity species or polymer formation. Tetrametallocyclophanes with Co(II), Fe(II), Cu(II) and Mn(II) are formed initially, as 112 verified by ES-MS (Figures 30 through 33), but they are not stable in solution. Decomposition takes within a few minutes to one hour, with entities of lower nuclearity or polymers being formed. It was noted that the bptz ligand is prone to side-reactions in the presence of water and Co(II) or Cu(II) which apparently assist in the tetrazine ring-opening and formation of a five-membered ring (2,5-di(2-pyridyl)-l,3,4-oxadiazole). This is evidenced by the isolation of the mononuclear compound [Cu(bopd)2(H20)2][BF4]2 and [Co(bopd)2(CH3OH)2] [BF4]2 (Figure 29). The new [M.;]8+ and [M5]l0+ molecules are of an unprecedented type of partially solvated molecular metallocyclophanes. The presence of labile CH3CN ligands on the periphery of these molecules allows for their use as building blocks for larger molecules for the elaboration of 2-D square grids (Figure 43). First-row transition metal coordination compounds with abpy do not exhibit as good electronic coupling as their counterparts in the second and third row transition metals. 20 A good approach to improve the capabilities of the abpy as a molecular bridge for first-row transition metals would be the use of the radical form of abpy instead. Previous studies with Cu(II) and Fe(II) have demonstrated that this approach affords mixed-valence species.”33 Dinuclear compounds of Ru(II) and Os(II) with abpy are difficult to obtain and require tedious and lengthy synthesis, but the mononuclear species were obtained in high yields. The large activation barrier to the formation of abpy-bridge dimers from monomeric precursors has previously been attributed to steric interactions between the 6 and 6’ protons of the bridge and the coordinating nitrogen atoms of adjacent ligands.33 In 113 the case of the dimers of Ni(II) and Cu(II), however, they are obtained in large yields just by stirring for a few hours followed by crystallization without any forcing conditions. 114 VI. References 1. (a) Balzani, V.; Scandola, F. Pure Appl. Chem, 1990, 62, 1457. (b) J. M. Lehn, Supramolecular Chemistry: Concepts and Perspectives, VCH, Weinheim, 1995. (c) Baxter, P. N. W. Comprenhensive Supramolecular Chemistry, (Ed. Atwood, J. L.; Davies, J. E. D.; MacNicol, D. D.; Vogtle, F.; Lehn, J. M.) Pergamon, Oxford, 1996; 9, 123; (d) Constable, E. C. Comprenhensive Supramolecular Chemistry, (Ed. Atwood, J. L.; Davies, J. E. D.; MacNicol, D. D.; Vogtle, F.; Lehn, J. M.) Pergamon, Oxford, 1996, 9, 253. (f) Fyfe, M. C. T.; Stoddart, J. F.; Acc. Chem. Res. 1997, 30, 393. 2. H. Taube, Electron Transfer Reactions of Complex Ions in Solution, Academic, New York, 1970. 3. Sinn, E., Coord. Chem. Rev., 1970, 5, 313. 4 Hoffman, B. M.; Ibers, J. A.; Acc. Chem. Res., 1983, I6, 15. 5. Haim, A. Acc. Chem. Res., 1975, 8, 264. 6. (a) Kaim, W.; Angew. Chem. Int. Ed. Engl. 1983, 22, 171. (b) Kahn, O. Angew. Chem. Int. Ed. Engl., 1985, 24, 834. 7. Kurtz, D. M.; Shriver, D.; Klotz, I. M. Coord. Chem. Rev., 1977, 24, 145. 8. (a) Bencini, A.; Benelli, C.; Gatteschi, D.; Zanchini, C.; Inorg. Chem, 1986, 25, 398. (b) Hanack, M.; Seelig, F. F.; Stréhle, J. Z.; Naturforsch, A: Phys.Chem Kosmophys., 1979, 34A, 983. 9. Geldard, J. F.; Lions, F. J. Org. Chem, 1960, 30, 318. 10. Schwach, M., Hausen, H. D., Kaim, W. Inorg. Chem, 1999, 38, 2242. 115 11. (a) Campos-Femandez, C. S.; Clérac, R.; Dunbar, K. R. Angew. Chem. Int. Ed. Engl., 1999, 38, 3477. (b) Bu, X.-H; Morishita, H.; Tanaka, K.; Furusho, S.; Shionoya, M. Chem. Commun., 2000, 971. 12. (a) Benkstein, K. D.; Hupp, J. T.; Stem, C. L.; J. Am. Chem. Soc., 1998, 120, 12982. (b) Cotton, F. A.; Dikarev, E. V.; Petrukhina, M. A. Inorg. Chim. Acta., 1998, 284, 304. (c) Woessner, S. M.; Helms, J. B.; Houlis, J. F.; Sullivan, B. P. Inorg. Chem, 1999, 38, 4380. ((1) Sun, S.; Lees, A. J. Inorg. Chem, 1999, 38, 4181. (e) Be’langer, S.; Hupp, J. T.; Stem, C. L.; Slone, R. V.; Watson, D. F.; Carrel], T, G. J. Am. Chem. Soc., 1999, 121, 557. 13. (a) Henrich, J. L; Berseth, P. A; Long J. R. Chem. Commun., 1998, 1231 (b) Scuiller, A.; Mallah, T.; Verdaguer, M; Nivorozkhim, A.; Tholence, J.-L; Veillet, P. New. J. Chem, 1996, 20, 1 (c) Vernier, N.; Bellessa, G.; Mallah, T; Verdaguer, M. Phys. Rev. B., 1997, 56, 75. (d) Klausmeyer, K. K.; Rauchfuss, T. B.; Wilson, S. R. Angew. Chem. Int. Ed., 1998, 37, 1694. (e) Stang, P. J.; Cao, D. H.; Saito, S.; Arifa, A. M.; J. Am. Chem. Soc., 1995, 117, 6275. (f) Stang, P. J.; Chen, K.; J. Am. Chem. Soc., 1995, 117, 1667. (g) Olenyuk, B.; Whiteford, J. A.; Stang, P. J. J. Am. Chem. Soc., 1996, 118, 8221. (h) Whiteford, J. A.; Stang, P. J .; Huang, S. D. Inorg. Chem, 1998, 37, 5595. (i) Sugiura, K.; Fujimoto, Y.; Sakata, Y.; Chem. Commun., 2000, 1105. 14. (a) Fujita, M.; Yazaki, J .; Ogura, K; J. Am. Chem. Soc., 1990, 112, 5645 (b) Stang, P. J .; Olenyuk, B.; Acc. Chem. Res., 1997, 30, 502; (c) Fujita, M.; Aoyagi, F.; Ibukuro, K.; Yamaguchi, K.; J. Am. Chem. Soc., 1998, 120, 611; ((1) Lee, S. B.; Hwang, S.; Chung, D. S.; Yun, H.; Hong, J. I. Tetrahedron Lett., 1998, 39, 873. 15. (a) Bélanger, S.; Hupp, J. T. Angew. Chem. Int. Ed., 1999, 38, 2222. (b) Slone, R.V.; Hupp, J. T.; Stem, C. L.; Albrecht-Schmitt, T. E. Inorg. Chem, 1996, 35, 4096. (c) Slone, R. V.; Hupp, J. T.; Inorg. Chem, 1997, 36, 5422. (d) Cruse, H. A.; Leadbeater, N. E. Inorg. Chem, 1999, 38, 4149. (e) Sheng—Shih, S.; Lees, A. J Inorg. Chem, 1999, 38, 4181. (f) Rajendran, T.; Manimaran, B.; Lee, F. Y.; Lee, G. H.; Peng, S. M.; Wang, C. M.; Lu, K. L Inorg. Chem, 2000, 39, 2016. (g) Benkstein, K. D; Hupp, J. T.; Stem, C. L. Inorg. Chem, 1998, 37, 5404. (h) Woessner, S. M.; Helms, J. B.; Shen, Y.; Sullivan, B. P. Inorg. Chem, 1998, 37, 5406. (i) Benkstein, K. D.; Hupp, J. T.; Stem, C. L. J. Am. Chem. Soc., 1998, 120, 12982. (h) Slone, R. V.; Benkstein, K. D.; Bélanger, S.; Hupp, J. T.; Guzei, I. A.; Rheingold, A. L. Coord. Chem. Rev., 1998, I71, 221. 16. (a)Yoshida, N.; Ichikawa, K. Chem. Commun., 1997, 1091. (b) Zhao, L.; Matthews, C. J .; Thompson, L. K.; Heath, S. L. Chem. Commun., 2000, 265. (c) Baxter, P. N.; Lehn, J-M.; Fischer, J .; Yoinou, M-T. Angew. Chem. Int. Ed. Engl., 1994, 33, 2284. (d) Tong, M-L.; Chen, X-M.; Yu, X-L.; Mak, T. C. J. Chem. Soc. Dalton Trans, 1998, 5. (e) Rojo, 116 J.; Romero-Salguero, F. J .; Lehn, J-M.; Baum, G.; Fenske, D. Eur. J. Inorg. Chem, 1999, 1421. 17. (a) Hosseine, W.; Ruppert, R.; Schaeffer, P.; Cian, A.; Kyritsakas, N.; Fisher, J.; J. Chem. Soc. Chem. Commun., 1994, 2135 (b) Ohata, N.; Masuda, H.; Yamauchi, O. Angew. Chem. Int. Ed. Engl., 1996, 35, 531 (c) Sessler, J. L.; Andrievsky, A.; Gale, P. A.; Lynch, V. Angew. Chem. Int. Ed. Engl., 1996, 35, 2782. (d) Hosseine, W.; Ruppert, R.; Schaeffer, P.; Cian, A.; Kyritsakas, N.; Fisher, J.; J. Chem. Soc. Chem. Commun., 1994, 2135. (f) Saalfrank R. W.; Low, N.; Hampel, F.; Stachel, H. D. Angew. Chem. Int. Ed. Engl., 1996, 108. 2353. 18. (a) Jones P. L; Byrom; K. J.; Jeffery, J. C.; McCleferty; J. A.;. Ward, M. D. Chem. Commun., 1997, 1361. (b) Man, S.; Huttner, G.; Zsolnai, L.; Heinze, K.; Angew. Chem. Int. Ed. Engl., 1996, 35, 2808. (c) Fleming, J. S.; Mann, K. L.; Carraz, P. B.; Jeffrey, J. C.; McCleverty, J. A.; Ward, M. D.; Angew. Chem. Int. Ed., 1998, 37, 1279. 19. (a) Mingos, M. P.; Rohl, A. L. Inorg. Chem, 1991, 30, 3769. (b) Saalfrank, R. W.; Burak, R.; Breit, A.; Stalke, D.; Herbst-Irmer, R.; Daub, J .; Porsch, M.; Bill, B.; Miither, M.; Trautwein, A. X.; Inorg. Chem, 1994, 106, 1697 and 1994, 33, 1621. (c) Mingos, M. P.; Rohl, A. L. J. Chem. Soc. Dalton. Trans, 1991, 3419. (d) Vilar, R.; Mingos, A.; White, J. P.; Williams, D. J. Angew. Chem. Int. Ed., 1998 37, 1258. (f) Hasenknopf, B.; Lehn, J-M.; Kneisel, B. O.; Baum, G.; Fenske, D. Angew. Chem. Int. Ed. Engl., 1996, 35, 1838. (g) Hasenknopf, B.; Lehn, J-M.; Boumediene, N.; Leize, E.; Dorsselaer, A. D. Angew. Chem. Int. Ed. Engl., 1998, 37, 3265. (h) Hasenknopf, B.; Lehn, J-M.; Boumediene, N.; Dupont-Gervais, A.; Dorsselaer, A. V.; Kneisel, B.; Fenske, D. J. Am. Chem. Soc., 1997, 119, 10956. 20. (a) Kausikisankar, P.; Shivakumar, M.; Ghosh, P.; Chakravorty, A. Inorg. Chem, 2000, 39, 195. (b)Waldhor, B.; Poppe, J.; Kaim, W.; Cutin, B.; Garcia, M.; Katz, N. Inorg. Chem, 1995, 34, 3093. (c) Bellamy, A. J .; MacKirdy, I. S.; Niven, C. E. J. Chem. Soc. Perkin. Trans. 11., 1983, 183. 21. (a) Aumttller, A.; Erk, P.; Klebe, G.; Hiinig, S.; Schi'rtz, J .; Werner, H.; Angew. Chem. Int. Ed. Engl., 1986, 25, 740. (b) Erk, P.; Gross, H. J .; Hilnig, U. L.; Meixner, H.; Von Schlitz, J. U.; Wolf, H. C. Angew Chem. Int. Ed. Eng., 1989, 28, 1245. (c) Naklicki, M. L; Crutchley, R. J. J. Am. Chem. Soc., 1994, 116, 6045. (d) Kato, R.; Kobayashi, H.; Kobayashi, A. J. Am. Chem. Soc., 1989, III, 5224. 22. Hathaway et al. J. Am. Chem. Soc., 1962, 2444. 117 23. Baldwin, A.; Lever, A. B. P.; Parish, R. V. Inorg. Chem, 1969, 8, 107. 24. Theory and Applications of Molecular Paramagnetism, Boudreaux, E.A.; Mulay, L.N., Eds; John Wiley & Sons: New-York, 1976. 25. SAINT, Program for area detector absorption correction, Siemens Analytical X-Ray Instruments Inc., Madison WI 53719, USA 1994-1996. 26. Program in the SI-[ELXTL software. 27. SHELXL-97 — g.m. Sheldrick, SHELXL — 97, Program for refining crystal structures, University of Gottingen,1997. 28. (a) Glockle, M.; Kaim, W.; Katz, N. E.; Garcia-Posse, M.; Cutin, E. H.; Fiedler, J. Inorg. Chem, 1999, 38, 3270 (b) Roche, S.; Yellowlees, L. J.; Thomas, J. A. Chem. Commun., 1998, 1429 (c) Kaim, W.; Reinhardt, R.; Fiedler, J.; Angew. Chem. Int. Ed. Engl., 1997, 36, 2493 (d) Poppe, J; Moscherosch, M.; Kaim, W.; Inorg. Chem, 1993, 32, 2640. 29. Robin, M. B.; Day, P. Adv. Inorg. Chem. Radiochem, 1967, 10, 247. 30. Kelso, L. S.; Reitsma, D. A.; Keene, R. F.; Inorg. Chem, 1996, 35, 5144. 31. Schafer, R.; Kaim, W.; Fiedler, J.; Inorg. Chem, 1993, 32, 3199. 32. Kaim, W.; Kohlmann, J.; Jordanow, D.; Fenske, Z. Anorg. Allg. Chem, 1991, 217, 598. 33. Ernst, S. D.; Kaim, W.; Inorg. Chem, 1989, 28, 1520. 118 Chapter III Reactivity of the Ligands 2,3,5,6 tetrapyridyl pyrazine (tppz) and 2,4,6-Tris(2-pyridyl)-1,3,5-triazine (tptaz) with Paramagnetic First Row Metal Ions 119 I. Introduction In the last thirty years, the scientific community has witnessed a growth of research in the area of supramolecular chemistry. One of the main approaches in this field is to use predesigned “building blocks” to assemble larger structures. In order to build more elaborate molecules, the building blocks must possess reactive sites at which further chemistry can take place. One of the simple ligands that has been used with these goals in mind is 2,3,5,6-tetrapyridylpyrazine (tppz) (Figure 45). The tppz ligand was synthesized in 1959 by Goodwin and Lions, who reported a series of monodentate compounds of the type [M(tppz)2]2+ (M = first row transition metals) with little characterization to verify their nature.I At the time, it was believed that once the ligand tppz was coordinated to one metal, binding to the second site would not occur. This prediction was based on the belief that the four pendant 2-pyn'dyl rings would not be stable in a coplanar arrangement with the central diazine ring. Figure 45. Schematic drawing of the ligand 2,3,5,6-tetrapyridylpyrazine (tppz). 120 For almost thirty years the tppz ligand was largely ignored due to these early predictions, and it was not until 1988 that Thummel and coworkers started using the ligand to prepare compounds such as (tpy)Ru(tppz)Ru(tpy)]4+, work which demonstrated that coordination of a second metal was indeed possible.2 A series of compounds with Ru(II), Os(II), Ir(II), Rh(II) and tppz were synthesized and characterized during the next 15 years, with the ultimate aim being to use them as photosentizers.3 In addition to displaying photoluminescence, some of these species exhibit strong electronic coupling, which is an excellent indication that this bridging ligand permits delocalization of electronic density between metal centers. Within this category, the compound [(NH3)3Ru(tppz)Ru(NH3)]4+ is the best example, with a comproportionation constant Kc Tridentate coordination site A r ‘ / N N/ \ N\ \ \N / N Monodentate coordination site Brdentate coordination srte / [N \ Figure 46. The three coordination sites in Tptaz. 121 of 2.8 x 108 based on cyclic voltammetric studies. This qualifies the compound as class III (completely delocalized) on the Robin-Day scale.4 Concomitant with the research on the reaction of the second and third row transition metal with tppz, Stoeckli-Evans and co-workers undertook reactivity studies with first row metals.5 “Monomers” and “dimers” such as [M2(tppz)2(L)(,]4+, [M(tppz)]2+ (M: Ni“, Cu“; L = H20) were prepared and found to exhibit significant antiferromagnetic coupling.5 There were no reported attempts, however, to use these compounds as building blocks for higher nuclearity species. Work in our laboratories on the tppz ligand focuses on two main areas: (a) the synthesis of paramagnetic building blocks with first row transition metals and (b) the self-assembly of molecular rectangles with metal-metal bonded cores, a novel application for this ligand. In related chemistry, exploratory chemistry with the ligand tptaz (2,4,6- Tris(2-pyridyl)—l,3,5-triazine) is also being conducted. The tptaz ligand possesses three coordination sites (tridentate, bidentate and monodentate) according to the number of donor nitrogen atoms (three, two and one, respectively) as shown in Figure 46. Given the multiple coordination sites on tptaz, it can act simultaneously as a tridentate and a bidentate ligand. Dinuclear compounds of this type have been synthesized with Co(II),6 Hg(I),7 and Ru(II)8 ions. It is worth mentioning, however, that the coordination of the second metal to this ligand is not particularly common due to the deactivation of the triazine ring by the inductive effect of the first metal, and also because of steric interactions between the hydrogen atoms and the metal ion.9 In the chapter, the syntheses of precursors to be used as building blocks for the preparation of multinuclear metal complexes are reported. Three compounds were 122 synthesized in quantitative yields, namely [Ni(tptaz)(CH3CN)2(HzO)][BF4]2 (12), [Fe(tptaz)2][ClO4]2 (13) and [Mn(tptaz)(phen)][CF3SO3]2 (14). A detailed characterization of these compounds including magnetic measurements, cyclic voltammetry, UV-Visible spectroscopy and X-ray crystallography is presented. A description of our attempts to form larger supramolecular entities will be presented along with a rationale for the outcome and possible future approaches to succeed in this goal. 11. Experimental Section Preparation of Compounds. Methods and Materials. All operations were performed under a nitrogen atmosphere using standard Schlenk line techniques unless otherwise indicated. All solvents were pre-dried over 4 A molecular sieves with the exception of acetonitrile, which was pre-dried over 3 A molecular sieves. Diethyl ether and toluene were freshly distilled over Na/K, acetonitrile was distilled over 3 A molecular sieves and methylene chloride was distilled over P205. The starting materials [Ni(HzO)(,[ClO4]2, [Mn(HzO)6[ClO4]2 and [Fe(HzO)6[ClO4]2 were purchased from Aldrich and used without further purification. The solvated compounds [Ni(CH3CN)6][BF4]2 and [Co(CH3CN)6][PF6]2 were synthesized by published methods.10 The tppz ligand was prepared from a literature method and recrystallized from pyridine.2 The tptaz molecule was synthesized by a published method with minor modifications.ll Physical Measurements. IR spectra were performed on a Nicolet 740 FT -IR spectrometer using KBr plates and samples were suspended in Nujol mulls. The magnetic susceptibility measurements were obtained with a Quatum Design SQUID MPMS-XL magnetometer. Measurements were performed on finely ground polycrystalline samples. Data were corrected for the 123 sample holder, and the experimental diamagnetic contribution was calculated from the Pascal constants.12 Electrochemical measurements were carried out by using an EG&G Princeton Applied Research Model 362 scanning potentiostat in conjunction with a BAS Model RXY recorder. Cyclic voltammetry was performed in CH3CN containing 0.1 M tetra-n-butylammonium hexaflourophosphate (TBAPFo) as the supporting electrolyte. The working electrode was a BAS Pt disk electrode. The ferrocene couple occurs at 0.52 V vs. Ag/AgCl under the same experimental conditions. Synthesis 2,3,5,6otetrapyridylpyrazine (tppz). In a 500 mL round-bottomed flask, a 90 g sample of NILOZCCH3 was thoroughly mixed with 20 g of a-pyrodoin (ClzNzOsz). This mixture was slowly heated to 180 °C in an oil bath for two hours. After the first hour of refluxing, yellow crystals began to appear in the brown melt. The thick brown solution was filtered to give a yellow solid which was washed with a large quantity of diethyl ether. The solid was recrystallized from pyridine; yield 4.8g (27 %) mp 284°C. 'H NMR (CDC13): three multiplets centered at 7.30, 7,85 and 8.45 ppm. UV-Visible (acetonitrile, nm, c = 2.47 x 10°5M): Am, = 320, e = 2.62 x 104 L(mol°cm)"; Am, = 274, e = 2.6 x 10‘ L(mol-cm)". IR (KBr mull) cm", 1680 (w), 1288 (w), 1138 (w), 1061 (w), 992 (w), 748 (m), 789 (w), 724 (w). 2,4,6-tris(2-pyridyl)-l,3,5-triazine (tptaz). The tptaz ligand was synthesized from a previously published method with some modifications.'1 The reagent 2-cyano pyridine (6.0 g, 0.058 mol) was loaded in a round- bottomed flask and mixed thoroughly with NaH (0.1g, 0.004 mol) under nitrogen. This mixture was heated at 165 °C until the entire solid had melted and then refluxed at 170 °C 124 for one hour. At this point the melt had turned black. The solid was extracted with hot benzene and recrystallized by slow evaporation; yield 3.0g (50%). [Ni(tPPZ)2JIN03]2 (16)- The salt [Ni(HzO)6][NO3]2 (100 mg, 0.344 mmol) was dissolved in 20 mL of acetonitrile, and two equivalents of tppz were added (270 mg, 0.69 mmol). Within a few minutes a drastic color change from blue to yellow ensued, and a precipitate appeared at the bottom of the vessel. The reaction mixture was stirred overnight after which time the precipitate was removed by suction filtration. The filtrate was layered with toluene to afford crystals of [Ni(tppz)2][NOg]2 within one week; yield, 190 mg (58%). IR (KBr mull) cm", 2723 (w), 1598 (w), 1250 (w), 1204 (w), 1149 (w), 1096 (w), 1015 (w), 743 (w), 722 (w). UV—Vis (acetonitrile, nm, c = 1.9 x 10'5 M): Am, = 355, e = 4.3x 104 L(mol-cm)"; hm, = 298 e = 4.0 x 104 L(mol-cm)"). [C0(tPPZ)2][PF6]2°2CH3CN (17)- The precursor [Co(CH3CN)6][PF6]2 (100 mg, 0.2 mmol) was dissolved in 20 mL of acetonitrile in a 50 mL round-bottomed flask, and the resulting pink solution was treated with tppz (155 mg, 0.4 mmol). The solution immediately changed to a red color. It was stirred under nitrogen overnight, after which time it was layered with toluene to afford red rectangular crystals; yield, 213 mg (90%). IR (KBr mull) cm", 2726 (w), 1317 (W), 1250 (w), 1152 (w), 840 (s,b), 722 (m), 687 (w). UV-Vis (acetonitrile, nm, c = 1.5 x 104M): Am = 520, e = 2.3 x 103 L(mol-cm)"; Am, = 484, e = 2.3 x 103 L(mol-cm)". [Fe(tPPZhJIClodz (18)- The salt [Fe(HzO)6][ClO4]2 100 mg (0.276 mmol) was dissolved in 30 mL of acetonitrile in a beaker. To this clear solution was added 215 mg (0.553 mmol) of tppz 125 which led to an instantaneous color change from a clear solution to a dark blue. The blue solution was stirred for 4h, and the volume was decreased by half. The reaction mixture was layered with diethyl ether and blue crystals were obtained within a week; yield, 230 mg (81%). IR (KBr mull) cm", 2723 (w), 1320 (w), 1220 (w), 1078 (s,b), 722 (m), 619 (w). UV—Vis (acetonitrile, nm, c = 7.4 x 10’6M): Amax = 568, e = 3.7 ><103 L(mol-cm)"; A. = 341, e = 4.0 x 104 L(mol.cm)"; Am, = 242.5, 8 = 4.4 x 104 L(mol-cm)". [Mn(tPchHClOdz (19)- A sample of [Mn(HzO)6][ClO4]2 (100 mg, 0.277 mmol) was placed in a beaker and dissolved in 30 mL of acetonitrile. To this clear solution was added 215 mg (0.55 mmol) of tppz. The solution turned a pale yellow color within a couple of minutes, was stirred for two hours, and finally concentrated to one-half of its original volume. The solution was layered with diethyl ether and a crop of pale yellow crystals was harvested in two days; yield, 215 mg (75%). IR (KBr mull) cm", 2723 (w), 1303 (w), 1155 (w), 1099 (s,b), 1012 (m), 722 (w). UV-Vis (acetonitrile, nm, c = 2.9 x 10M): 2...... = 351, e = 4.1 x 104 L(mol-cm)"; Am, = 290, e = 3.5 x 104 mmol-cm)". [Ni(tPchJIClodz (20). A quantity of [Ni(HzO]6[ClO4]2 (100 mg, 0.275 mmol) was dissolved in 30 mL of acetonitrile in a beaker and treated with two equivalents of tppz (215 mg, 0.549 mmol). The pale blue solution immediately turned yellow. The solution was stirred for four hours, reduced in volume to 15 mL, and layered with toluene to obtain yellow needles; yield, 275 mg (83%). IR (KBr mull) cm", 2723 (w), 1568 (w), 1301 (w), 1246 (w), 1148 (w). 1080 (s,b), 788 (w), 769 (m), 723 (w). UV-Vis (acetonitrile, nm, c = 1.4 x 10‘5M): Am... = 355, e = 4.3x 104 L(mol-cm)"; 2...... = 298 e = 4.0 x 104 L(mol-cm)". 126 [Ni2(tPPZ)(CH3CN)o][BF414 (21). The salt [Ni(CH3CN)6][BF4]2 (100 mg, 0.2 mmol) was placed in a Schlenk flask under nitrogen and dissolved in 20 mL of freshly distilled acetonitrile. The stirring pale blue solution was treated with tppz (39 mg, 0.1 mmol) which led to a color change to brown-yellow. After stirring overnight, the solution was concentrated, diethyl ether was added, and the solution was chilled to -10 °C. Crystals of [Ni2(tppz)2(CH3CN)6][BF4]4 grew over a period of two weeks; yield, 145 mg (66%). IR (KBr mull) cm", 3450 (b,m), 2725 (w), 2316 (m), 1600 (w), 1311 (w), 1301 (w), 1260 (w), 1209 (w), 1018 (s,b), 787 (w), 750 (w), 722 (m). UV-Vis (acetonitrile, nm, c = 1.3 x 10'5M): km = 354, e = 2.5 x 10“ L(mol'cm)"; Am, = 292 e = 2.4 x 104 mmol-cm)“; A = 241, e = 4.2 x104 L(mol-cm)’ I. [Rh(tpPZ)2][BF4]3 (23)- A sample of [Rh2(CH3CN)10][BF4]3 100 mg (0.12 mmol) was loaded into a round- bottomed flask under nitrogen and dissolved in 20 mL of acetonitrile. The orange solution was stirred until the entire solid had dissolved. After which time, 93 mg (0.24 mmol) of tppz were added. This produced a drastic change of color from orange to a dark brown within minutes. The reaction mixture was stirred overnight, and the solution was concentrated and treated with diethyl ether to the point of saturation. The vessel was placed in the freezer, and a microcrystalline compound was collected within five days; yield, 75 mg (48%). IR (KBr mull) cm], 1653 (s), 1565 (s), 1155 (w), 1014 (w), 839 (w), 722 (w). UV-Vis (acetonitrile, mm, c = 1.8 x lO'SM): Am, = 749, 8 = 2.9 X 103 L(mol'cm)' 1 mm, = 517 e = 1.6 x 104 L(mol°cm)"; Am, = 437, e = 1.4 x104 L(mol-cm)", Am, = 405, 8 = 1.4 x104 L(mol-cm)". 127 IRh2(02CCH3)2(tPPZ)2(CH30H)4][PFsk'CnsoH (24)- A quantity of [Rh2(OZCCH3)2(CH3CN)6][BF4]2 (100 mg, 0.13 mmol) was dissolved in 20 mL of CH3OH, and the purple solution was stirred until the entire solid had dissolved. After this time, tppz (52 mg, 0.13 mmol) was added, and the solution was heated to 60 °C to dissolve the tppz. The solution changed to a dark green color within 20 minutes, after which time the heating was ceased and diethyl ether was added to the saturation point. A microcrystalline powder was collected after two days; yield, 65 mg (48%). IR (KBr mull) cm", 2724 (w), 1170 (w), 1034 (w), 1846 (s), 769 (w), 722 (w). [C02(tpp2’)2][C02C1711PF61 (25)- To a sample of CoClz (100 mg, 0.78 mmol) dissolved in 30 ml of acetonitrile was added tppz (301 mg, 0.78 mmol). An immediate color change from intense blue to a dark green color ensued, and after ten minutes an orange insoluble solid began to deposit on the bottom of flask. The solution was stirred overnight under nitrogen, and the solution was separated from the solid by suction filtration. At this point, the solution was concentrated, and green crystals of the product were obtained by slow vapor diffusion of diethyl ether into acetonitrile within three days; yield, 280 mg (52%). IR (KBr mull) cm' I, 2722 (w), 1585 (w), 1298 (w), 1251 (w), 1143 (w), 1060 (w), 1034 (w), 795 (w), 746 (w). UV-Vis (acetonitrile, nm, 0 = 2.74 x 10'4M): Am = 679.5, 8 = 3.77 x 102 L(mol-cm)' ‘; km, = 588.0 a = 3.74 x 102 L(mol'cm)". [Ni(tptaZ)(CH3CN)2(H20)][BF412 (27). A sample of [Ni(CHgCN)6][BF4]2 (100 mg, 0.21 mmol) was dissolved in 20 mL 0f acetonitrile, and tptaz (65 mg, 0.2 mmol) was added to the stirring solution which affected a color change from bright blue to yellow-green. The reaction mixture was 128 stirred overnight under nitrogen and layered with toluene. (Note that the acetonitrile should not be anhydrous, otherwise crystals do not grow.) Crystals grew over the period of a week; yield, 80 mg (62%). IR (KBr mull) cm", 3483 (b,m), 2325 (w), 2298 (w), 1377 (s), 1258 (w), 1060 (w), 1066 (b,s), 773 (w), 722 (w). UV-Vis (acetonitrile, nm, C = 4.96x 10'5M): Am, = 293, e = 5.9 x104 L(mol-cm)", Am, = 253, e = 2.5 x102 L(m01'cm)' 1 [Fe(tptaz)2][ClO4]2 (28)- The salt [Fe(HzO6)][ClO4]2 (100 mg, 0.28 mmol) was dissolved in 30 mL of acetonitrile in a beaker and treated with tptaz (175 mg, 0.56 mmol). The solution, which immediately developed an intense blue color, was stirred for five hours and then concentrated to 15 mL. Blue platelet crystals were obtained by slow diffusion of diethyl ether into the reaction mixture in acetonitrile; yield, 215 mg (82%). IR (KBr mull) cm", 1573 (w), 1356 (w), 1258 (w), 1083 (b,s), 768 (w), 622 (w). UV-Vis (acetonitrile, nm, 0 = 4.6 x lO'SM): Am, = 568, e = 6.1 x102 L(mol'cm)", Am, = 341, e = 6.5 x 103 L(mol-cm)", hm, = 243, 8 = 4.3 x 103 L(mol-cm)". [Mn(tptaz)(phen)(H20)][O3SCF312 (29)- A sample of Mn(phen)2(O3SCF3)2 (100 mg, 0.14 mmol) was loaded into a round- bottomed Schlenk flask under nitrogen and dissolved in 20 mL of freshly distilled acetonitrile. The colorless solution was stirred for a few minutes until the solid had dissolved, and tptaz (44 mg, 0.14 mmol) was added, giving a pale green solution. The reaction mixture was stirred overnight and concentrated. Crystals of the product were Obtained by slow vapor diffusion of diethyl ether into the acetonitrile solution; yield, 110 mg (91%). IR (KBr mull) cm", 1533 (w), 1274 (w), 1222 (w), 1151 (w), 1028 (w), 635 129 (w). UV-Vis (acetonitrile, nm, c = 6.3 x 10‘6M): Am, = 292, e = 5.0 x 10“ L(mol-cm)'l, Am, = 272, e = 7.0 x104 L(mol-cm)", Am, = 227, a = 6.7 x 104 L(mol-cm)". X-ray data collection and Refinement. X-ray structural studies were performed on crystals of (16)-(29) on a SMART 1K area detector diffractometer equipped with graphite monochromated Mo K01 radiation (ha = 0.71073 A). The frames were integrated in the Siemens SAINT software package,'3 and the data were solved using the direct-methods program SHELXS-97.M Crystal data are listed for compounds (16)-(29) in Table 16. [Ni(tPPZ)2][N03]2 (16)- Single crystals of [Ni(tppz)2][N03]2 (16) were grown by slow diffusion of dichloromethane into an acetonitrile solution of the title compound. A light yellow 3 was secured on the tip of a glass rectangular crystal of dimensions 0.01 x 0.04 x 0.2 mm fiber with silicone grease and transferred to the Bruker Smart CCD system. The crystal was cooled to 110 i 2 K during the data collection via a cold stream of nitrogen gas. A total of 22900 reflections was collected of which 4086 were unique. 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A red 3 platelet with dimensions 0.15 x 0.2 x 0.1 mm was mounted on a glass fiber using Dow- Coming silicone grease and cooled down to 173 i 2 K during data collection via a cold stream of nitrogen gas. A total of 11742 reflections was collected, of which 4176 were unique. The final full-matrix least-squares refinement was based on 2916 observed reflections with Fo>40(Fo) that were used to fit 356 parameters to give R1 = 0.0605 and wR2 = 0.1014. The goodness-of—fit index was 1.083 and the highest peak in the final difference map was 0.396 e'/A'3. [F “11113321100412 (13)- Single crystals of [Fe(tppz)2][ClO4]2 were obtained by slow vapor diffusion of diethyl ether into an acetonitrile solution of [Fe(tppz)2] [C104]2. Data were collected on a dark-blue, rectangle shaped crystal with dimensions of 0.3 x 0.05 x 0.25 mm3 which was mounted on the tip of a glass fiber, secured with silicone grease and placed under a stream of N2(g) at 110 i 2 K. A total of 25468 reflections was collected, of which 8599 were unique. Both [C104]' anions exhibit a 2-fold rotational disorder. In order to solve this problem, restraints for chemically equivalent distances (Cl-O 1.415 A) were applied. The final full-matrix least-squares refinement was based on 3312 observed reflections with Fo>40(Fo) which were used to fit 647 parameters to give R1 = 0.0766 and wR2 = 0.1925. The goodness-of-fit index was 0.922 and the highest peak in the final difference map was 1.322 e'lA'3. The extensive disorder accounts for the slightly high R factor. 135 [Mn(tPPZhIIClOdz (19). Crystals of the title compound were obtained by slow diffusion of toluene into an acetonitrile solution of the title compound. A pale yellow crystal of dimensions 0.2 x 0.4 x 0.25 mm3 was mounted on the tip of a glass fiber with silicone grease and placed in a cold N2(g) stream at 110 i 2K. A total of 13232 reflections were collected, of which 2261 were unique. The final full-matrix refinement was based on 2033 observed reflections with Fo>40(Fo) which were used to fit 163 parameters to give R1 = 0.1352 and wR2 = 0.3510. The goodness-of-fit index was 1.29 and the highest peak in the final difference map was 0.898 67.313. [Ni(tPPZ)2][CIO4]2 (20)- X—rays quality crystals of [Ni(tppz)2][ClO4]2 were grown by slow diffusion of toluene into an acetonitrile solution of [Ni(tppz)2] [C104]; in a thin pyrex tube (diameter = 3 mm). A pale yellow needle of dimensions 0.05 x 0.2 x 0.06 mm3 was placed on the tip of a glass fiber, secured with silicone grease, and placed in a N2(g) stream at 298 :l:2 K. A total of 44378 reflections was collected, of which 8270 were unique. One of the [ClOJ anions exhibits a two-fold rotational disorder. In order to solve this problem, restraints for chemically equivalent distances (Cl-O 1.529 A) were adopted. The final full-matrix, least-squares refinement was based on 3735 observed reflections with Fo>40(Fo) which were used to fit 675 parameters to give R1 = 0.0749 and wR2 = 0.1979. The goodness-of-fit index was 0.983 and the highest peak in the final difference map was 0.939 e'/A'3. As the previous cases, this disorder accounts for the slightly higher R factor. 136 [Ni2(tPPZ)(CH3CN)s][BF414'CH3CN (21)- Single crystals of (21) were grown by treating a saturated solution of [Niz(tppz)(CH3CN)6][BF4]4 in acetonitrile with diethyl ether and placing it in the freezer for two weeks at —5 °C. Crystals formed at the bottom of the flask. A dark yellow platelet with dimensions 0.1 x 0.24 x 0.07 mm3 was covered in paratone oil and quickly mounted on the tip of glass fiber due to the rapid solvent loss. It was secured with Dow Corning silicone grease and placed under a N2(g) stream at 173 i 2K. A total of 21891 reflections was collected, of which 6042 were unique. The final full-matrix least-squares refinement was based on 4706 observed reflections with Fo>40(Fo) which were used to fit 343 parameters to give R1 = 0.0531 and wR2 = 0.1123. The goodness-of-fit index was 1.074 and the highest peak in the final difference map was 0.622 e'IA'3. {[C02(tpp2)(CH3CN)2Cl4][PFol[BF 4] 14 (22). Good quality crystals of (22) were obtained by slow diffusion of an acetonitrile solution of the title compound into dichloromethane. A red platelet of dimensions 0.2 x 0.15 x 0.08 mm3 was mounted on the tip of a glass fiber and and placed in a N2(g) cold stream at 110 :l:2 K. A total of 34759 reflections was collected, of which 6762 were unique. The [PF6]' anions are involved in a two-fold rotational disorder, therefore restraints on the chemically equivalent distances (P-F 1.580 A) were applied. The final full-matrix refinement was based on 4538 observed reflections with Fo>40(Fo) which were used to fit 563 parameters to give R1 = 0.0807 and wR2 = 0.245. The goodness-of- fit index was 1.049 and the highest peak in the final difference map was 0.837 e'/A'3. This disorder accounts for the high R factor of the refinement of the structure. 137 [Rh(tPPZ)2][BF4]3 (23). Single crystals of [Rh(tppz)2][BF4]3 were obtained by slow vapor diffusion of diethyl ether into an acetonitrile solution of the title compound. A brown platelet of dimensions 0.02 x 0.01 x 0.05 mm3 was secured on the tip of a glass fiber with silicone grease and placed under a N2(g) stream at 110 i 2 K. At the end of the data collection, a total of 39610 reflections had been collected, of which 14580 were unique. The final full- matrix refinement was based on 7715 observed reflections with Fo>40(Fo) which were used to fit 799 parameters to give R1 = 0.0725 and wR2 = 0.1861. The goodness-of-fit index was 0.942 and the highest peak in the final difference map was 1.169 e'/A'3. IRh(ozCCH3)2(tPPZ)2(CH30H)4][PF616 (24)- Single crystals of [Rh4(OzCCH3)2(tppz)2(CH3OH)4][PF6]6 were obtained by slow diffusion of a toluene solution saturated with [Bu4N][PF6] into a solution of the title compound in methanol in a thin pyrex tube (diameter = 3 mm). Crystals grew over a period of two months. A green rectangular platelet of dimensions 0.06 x 0.03 x 0.1 mm3 was mounted on the tip of a glass fiber with silicone grease and placed in a N2(g) cold stream at 173 3: 2K. At the end of the data collection, a total of 32269 reflections was collected, of which 6137 were unique. Two [PF6]' anions are involved in a three-fold rotational disorder. In order to solve this problem, restraints on chemically equivalent distances (P-F 1.671 A) were applied, and the atoms were refined isotropically. The carbon atoms C(16) and 0(4) were also refined isotropically. The final full-matrix, least- squares refinement was based on 4599 observed reflections with Fo>40(Fo) which were used to fit 493 parameters to give R1 = 0.0786 and wR2 = 0.1906. The goodness—of-fit index was 1.086, and the highest peak in the final difference map was 2.067 e'/A'3, which 138 is not located near any other atoms. The high degree of disorder accounts for the slightly high R factor present in the final refinement. [C02(tpp2’)2]PFs][COzCl7] (25)- X-ray quality crystals of [Coz(tppz’)2][PF6][C02C17] were isolated by slow diffusion of toluene into an acetonitrile solution of the title compound in a thin pyrex tube (diameter = 3 mm). A dark green platelet of dimensions 0.09 x 0.04 x 0.2 mm3 was mounted on a tip of glass fiber, secured with silicone grease, and placed in a N2(g) cold stream at 110 i 2K. A total of 21108 reflections were collected, of which 3754 were unique. The final full-matrix, least-squares refinement was based on 2310 observed reflections with F0>40(F0) which were used to fit 194 parameters to give R1 = 0.0519 and wR2 = 0.1584. The goodness-of—fit index was 1.052 and the highest peak in the final difference map was 0.735 e‘/A°3. [C0(tpy)2Clz][BF4]2 (26). X-ray quality crystals were obtained by slow diffusion of toluene into an acetonitrile solution of (26). A pale-red prism of dimensions 0.08 x 0.23 x 0.075 mm3 was mounted on tip of a glass fiber, secured with silicone grease, and placed in a N2(g) cold stream at 110 i 2 K. During the data collection process, a total of 13051 reflections was collected, of which 4485 were unique. The final full-matrix, least-squares refinement was based on 2999 observed reflections with Fo>40(Fo) which were used to fit 253 parameters to give R1 = 0.0475 and wR2 = 0.1119. The goodness-of-fit index was 0.979 and the highest peak in the final difference map was 0.939 e'lA'3. 139 [Ni(tptaz)(CH3CN)(H20)][BF4]2 (27)- Crystals suitable for X-ray crystallography analysis were obtained by slow diffusion of toluene into an acetonitrile solution of the title compound. A light-green prism of dimensions 0.33 x 0.22 x 0.4 mm3 was secured on a tip of a glass fiber with silicone grease and placed in a stream of cold N2(g) at 110 3: 2K. During the data collection a total of 16965 reflections was collected, of which 6596 were unique. The final full-matrix, least-squares refinement was based on 4144 observed reflections with F0>40(Fo) that were used to fit 379 parameters to give R1 = 0.0532 and wR2 = 0.1389. The goodness-of-fit index was 0.995 and the highest peak in the final difference map was 0.948 e'lA’3. [Fe(tptaz)2][ClO4]2 (28)- In order to obtain crystals suitable for X-ray crystallography, diethyl ether was gently layered over a solution of the title compound in acetonitrile. Crystals grew over a period of 5 days. An intense blue colored needle of dimensions 0.5 x 0.21 x 0.15 mm3 was mounted on a tip of a glass fiber, secured with silicone grease and placed in a N2(g) cold stream at 110 j: 2 K. A total of 25468 reflections was collected, of which 8599 were unique. The final full-matrix, least-squares refinement was based on 7393 observed reflections with Fo>40(Fo) that were used to fit 647 parameters to give R1 = 0.0766 and wR2 = 0.1925. The goodness-of-fit index was 0.891 and the highest peak in the final difference map was 1.322 e'/A’3. [Mn(tptaZXPhenXHzO][Mn(tptaZ)(Phen)(H20)][CF330314 (29). Suitable quality single crystals were obtained by slow vapor diffusion of diethyl ether into an acetonitrile solution of the title compound. A light yellow platelet of 140 dimensions 0.3 x 0.11 x 0.35 mm3 was mounted on the tip of a glass fiber with silicone grease and placed in a N2(g) cold stream at 110 i K. A total of 16569 reflections was collected, of which 8412 were unique. The final full-matrix, least-squares refinement was based on 8412 observed reflections with F0>40(Fo) that were used to fit 991 parameters to give R1 = 0.056 and wR2 = 0.1237. The goodness-of—fit index was 0.983 and the highest peak in the final difference map was 1.427 e'/A'3. II. Results and discussion A. [M(tppz)2]2+ Series (M = Ni“, Co”, Fe“, an”): A.1. Synthesis. A series of compounds of general formula [M(tppz)2]2+ was synthesized by reacting the salts [M(HZO)6][ClO4]2 (M = Ni“, Mn“, Fe“), [Ni(H20)6][N03]2 and [Co(CH3CN)6][PF6]2 with two equivalents of tppz in acetonitrile (Eqs. 7 and 8). The reactions were performed in air with the exception of the Co(II) reaction, which was performed under nitrogen. All reactions proceed with a dramatic color change that occurs within minutes of mixing the reagents. CH3CN [M(H20)6][X]2 + 2 t13131 p [M(tPPZ)2][X]2 (Eq. 7) M = Ni“. Co“. Fe“. Mn“ [Ni(tpp2)2] [N0312 [Mn(tppz)2][ClO4]2 x = [ N031, [(31041 yield: 58% yield: 75% [Fe(tppz)2][ClO4]2 [Ni(tPPZ)2][C|0412 yield: 81% yield: 83% CH CN [C0(CH3CN)611PF612 + 2 tppz 3 4. [C0(tPPZ)21[PFe]2 (Eq. 8) yield: 90% 141 Experimental conditions such as the anion appear to play a major role in the chemistry as judged by the Ni(II) reaction with tppz. The mononuclear complex [Ni(tppz)2]2+ is formed in yields that exceed 80% when perchlorate is used (Eq. 7), but, when [N03]' is used, the yield is only about 58% (Eq. 7) and a significant amount of insoluble, presumably polymeric material is formed. Interesting, when the anion is [BF4]', the dinuclear complex [Niz(tppz)(CH3CN)6][BF4]4 is the main product of the reaction. In a deliberate attempt to prepare the dinuclear compound [Ni2(tppz)(CH3CN)6][C104]4, different ratios of Ni(II): tppz were used, but all attempts were unsuccessful; regardless of changes in temperature or concentration the sole product was still [Ni(tppz)2][ClO4]2. It is apparent that the anion is playing a dominant role in determining whether the nuclearity of the product is monuclear, dinuclear or polymeric. Solvent is another variable that is important in this chemistry. The compound lCo(tppz)2][PF6]2 was obtained in yields greater than 75% (Eq. 8) in acetonitrile, but, if an alcohol or acetone is used instead, the yield drops to less than 50% and insoluble solids are obtained. The same situation is encountered for Fe(II) and Ni(II) as well. It should be emphasized that attempts to synthesize the dinuclear species [M2(tppz)(CH3CN)6][X]4 (M = C0“, Fe”, Mn“; X = [PF6]' , [C104]') were unsuccessful regardless of the ratio of reagents or solvent utilized. A.2. Spectroscopic and cyclic voltammetric studies. As indicated from the data in Table 17, compounds (16) through (20) exhibit characteristic MLCT transitions as expected for polypyridine coordination compounds. The tppz moiety with its low lying 11* orbitals are easily accessible for electron promotion from the metal (1 electrons. The Ni(II) compounds (16) and (20) exhibit two 142 /,—.) /. 7 transitions at 355 nm and 298 run that are assigned to MLCT transitions; the transitions exhibit 8 values of ~ 4.3 x 104 mol(L-cm)". The cobalt derivative (17) displays two MLCT transitions as well located at 520 and 484 nm with 8 values of 2.3 x 103 mol(L-cm)". In the case of [Fe(tppz)2][ClOa]2 (18), there are three MLCT transitions located at 568, 341 and 242 nm; their respective 8 values are 3.7 x 103, 4.0 x 104 and 4.4 x 104 mol(L-cm)". Finally, [Mn(tppz)2][ClOa]2 (19) exhibits two MLCT transitions located at 352 and 290 nm with e values of 4.1 x 104 and 3.5 x 104 mol(L-cm)" respectively. Table 17. UV-Visible data for compounds (16)-(20). Mnm) e mol(L°cm)" [Ni(tPPZ)2][X12 (16) x = [N031 298 4.3 x 104 (20) x = [c1041 355 4.3 x 10‘ (17) [Co(tppz)2][PFs]2 520 2.3 x 103 434 2.3 x 103 568 3.7 x 103 (18) [Fe(tPPZ)ZJ[ClO4]2 341 4.0 x 10‘ 243 4.4 x 104 (19) [Mn(tppz)2][ClO.t]2 352 4.1 x 104 290 3.5 x 10‘ Cyclic voltammetry confirmed the accessibility of the 7t* orbitals in compounds (16)-(19). shows a very rich electrochemistry in the range 0 to —1.8 volts. Compound [Fe(tppz)2][ClO.1]2 (18) exhibits the most impressive electrochemical properties with four 143 reversible reduction couples and a reversible oxidation. The oxidation couple occurs at E11, = +1.37 V and corresponds to the oxidation of Fe(II) to Fe(III). The ligand-based reductions occur in the range —0.4 to —1.8 V at EU)” = -0.77, Ema = -1.04, Ema, = -1.50 and E“’.,, = -l.67 V (Figure 47). These cyclic voltammetry measurements allow for the 5.0x 10 -6 l I l 3.0x 10 ‘6 1.0x 10 ‘6 0.0 -20 x 10 '° 1 1 1 04 -O.8 -1.2 -1.6 -2 V(volts) Figure 47. Cyclic voltammogram for [Fe(tppz)2][ClO4]2 in acetonitrile with 0.1 M [n-BlelPFel. calculation of the comproportionation constant (K) for the stability of the mixed-valence intermediates as each ligand is reduced.4 The comproportionation constant for the first two couples is 3.7 x 104, whereas the second set of reductions gives a value of 7.5 x 102 (scheme 3). These equilibrium constants correspond to class H and class I borderline behavior for the stability of the mixed valence species, respectively. In the first case, the electrons are partially delocalized throughout the system, therefore the mixed valence intermediate is moderately stable. In the latter case, the mixed valence species is rather unstable and corresponds to nearly insulating behavior. 144 [Feappzlzl2+ ‘ . L [13841313421+ -e Kc = 3.7 x 104 [Fettppzlzr 1 +°_ > [Fe(tPPZ)2] -e [Fe(tppz)2] ‘ *8 s1 [Fe(tppz)2]' '9 Kc = 7.5 x 102 [Fe(IPPZ)2l' 1 f: - [Fe(tppzlzlz‘ Scheme 3. The Ni(II) derivative, [Ni(tppz)2][C104]2 (20), exhibits three redox events, namely a reversible reduction at E1), = -0.79 V, follow by a irreversible cathodic wave at 13p,c = - 1.2 V and finally a quasireversible reduction at E1, = -1.61V with subsequent decomposition of the reduced species. These data represent an electrochemical, chemical, electrochemical (ECE) series of processes.15 [Mn(tppz)2][ClO4]2 displays an irreversible couple at E = +1.22 V attributed to the oxidation of Mn(II) to Mn(IH) with the subsequent decomposition of the main species. Two reversible ligand based reductions were observed, the first one being at E1, = -l.1 V which involves one electron, and the second one located at Ev, = -1.7 V that involves two electrons. Finally, [Co(tppz)2][PF6]2 (17) exhibits two reversible ligand based reductions and a reversible oxidation. The oxidation couple occurs at EV, = +0.41 V and corresponds to 145 an oxidation of Co(II) to Co(III). The reduction, at Ema, = -0.28 v and Ema, = -l.18V each correspond to a two electron process. A.3. X-ray crystallographic results. In the mononuclear compounds, the metal centers reside in highly distorted octahedral environments, as indicated by the angle between the pyridyl moiety and the pyrazine unit with the metal center. This value averages ~80° as compared to the expected 90° for an ideal octahedron; the specific angles for the Mn(II), Fe(II), Co(II) and Ni(II) compounds are 723° (2), 81.4° (3), 792° (8) and 78.3°(2) respectively (Figures 49-53). The average M-N distances to the pyrazine moiety for the different compounds are 1.870 [3], 1.892 [4], 1.986 [3] and 2.228 [4] A for Fe(II), Co(II), Ni(II) and Mn(II) respectively. The M-N distances to the pyridyl moiety are 1.952 [4], 2.052 [3], 2.094 [4] and 2.241 A for Fe(II) Co(II), Ni(II) and Mn(II) respectively. The gradual increase in the MN distances is due to an increase in the radii of the metal centers. The ligand unit itself undergoes considerable distortion upon coordination. The pyrazine ring is not planar in any of the compounds, as determined from X-ray structural determinations (11)) (Figure 48). The greatest distortion is found in [Co(tppz)2][PF6]2-CH3CN (17); in this case, there is a torsion angle of 107° (4)). The second largest distortion is exhibited by [Ni(tppz)2][ClO.1]2 (20), with a value of 98° ((11), followed by [Mn(tppz)2][ClOa]2, 55° (0), and finally the smallest distortion is found in [Fe(tppz)2][ClO.1]2 (18) at 48° (0) (Table 18). The planes between the coordinated pyridyl groups are not coplanar in these compounds with the exception of [Fe(tppz)2][C104]2 (18). In the Fe2+ compound, the pyridyls rings are nearly coplanar with a dihedral angle of only 02°. The Mn2+ and Co2+ analogues display the largest deviation 146 from coplanarity with 13.5 and 132° angles respectively (K, Table 18). The compound [Ni(tppz)2][ClO4]2 (20) displays a deviation of 6.120 (K, Table 18). The non-coordinated pyridyl rings exhibit much larger dihedral angles (B) between the planes (Figure 48) These values are 137°, 443°, 582° and 728° for Co", Ni", Mn” and Fe" respectively (B. Table 18) (Figure 48). Table 18. Values of the distortions exhibited by the tppz ligand by coordination to Co(II) (17), Ni(II) (l6), Mn(II) (19) and Fe(II) (18). (1’ (°) 9 (°) [3 (°) K (°) [Co(tppz)2]2+ 10.7 44.9 13.74 13.2 [Ni(tppz)2]2+ 9.8 66.9 44.3 6.1 [Mn(tppz)2]2+ 5.5 63.4 58.2 13.5 [Fe(tppz)2]2+ 4.8 59.6 72.8 0.2 147 downy—6.58 com: 39 .3 305530 5:566 Ho 39: Bogota .5. 95”..— .983 $53.3 on. 2 83mm. 5? 292 .U wmcwi 6;. 65 8958 148 Table 19. Selected bond distances (A) and angles (°) for [Ni(tppz)2][NO3]2 (16). Nil-N(2)#l Nil-N2 Nil-N(6)#l N2-Nil-N(2)#1 N(2)#l-Ni l-N(6)#l N2-Nil-N(6)#l N(2)#l-Ni1-N6 N2-Nil-N6 N6-Nil-N(6)#l N(2)#l-Ni1—Nl 2.002(4) 2.002(4) 2.093(4) 177.7(2) 104.0l(l6) 77.63(l6) 77.63(l6) 104.01(l6) 90.4(2) 100.22(l6) Ni 1-N6 2.093(5) Nil-N1 2.118(4) Nil-N(l)#l 2.118(4) N6—Ni1-Nl 98.37(16) N(6)#l-Ni l-Nl 155.49(16) Nl-Ni l-N(l)#1 83.0(2) N2-Ni 1 -N1 78.05( 16) N6-Ni1-N(1)#l 155.49(16) N(6)#l-Ni 1-N(1)#1 98.37( 16) Symmetry transformations used to generate equivalent atoms: #1 -x+2,y,-z+l/2 Table 20. Selected bond distances (A) and angles (°) for [Co(tppz)2][PF6]2-CH3CN (l7). Col-N2 Col-N5 Col-N1 Nl-Col-N(l)#1 NZ-Co l -N(6)#l N5-Co l -N(6)#1 N 1-Col-N(6)#l N2-Co 1 -N5 N 2-Co 1 -N1 NS-Co 1 -N1 N2-Co l -N( l )#1 1.859(4) 1.925(4) 1.970(3) 164.49(l7) 100.80(8) 7920(8) 88.57(12) 180.02(5) 8225(8) 97.75(8) 8225(8) Col-N6 2.134(3) Col-N( 1) #1 1.970(3) Col-N(6)#1 2.134(3) N(1)#l-Col-N (6)#l 94.33( 12) N2-Col -N(6)#1 100.80(8) N5-Col-N6 7920(8) N1-Col-N6 94.33(12) N l -Col-N(6)#l 88.57(12) N6-Col-N(6)#l 158.3906) NS-Col-Nl 97.75(8) Symmetry transformations used to generate equivalent atoms: #1 -x+l,y,-z+l/2 149 55.6 no 873 05 .5.“ 32:5 coon 022 8.9a smegma 8286:; 35368 saw .23 8:8 33835 G: zommuéozfinacmza 2: 26 8358262 283:6 35.2: .3 2:3... 4‘8 a), 88 .0 -y AIM new \ :8 ‘0 41 150 .558 .3 83m 05 no.“ 359:0 :03 02“: 8.8a 82%: 86356 es 8 as, A5 zummuhemafiaevea 5 :88 me 8.6358282 288:6 3:55. .8 2:3... \‘ \\. s t @z t 8% EU '\ 1 3:0 fix 4 . \ ,\ 3:0 151 Table 21. Selected bond distances (A) and angles (°) for [Fe(tppz)2][ClO4]2 (18). Fel-N2 1.865(6) Fel-N3 1.952(7) Fel-N12 1.876(6) Fel-N7 1.954(6) Fel-Nll 1.945(6) Fel-Nl 1.955(6) N2-Fel-N12 178.6(3) N1 l-Fel-N7 162.3(3) N2-Fe1-N1 l 98.3(3) N3-Fel-N7 88.6(3) N12-Fel-Nll 81.4(3) N2-Fe1 -Nl 81.4(3) N2-Fe 1 -N3 81 .5(3) N12-Fel-Nl 100.0(3) N12-Fel-N3 97.2(3) N1 l-Fel-N l 87.0(3) N11-Fel-N3 942(3) N3-Fel-N1 162.8(3) N2-Fel—N7 99.4(3) N7-Fe1-N1 95.4(3) N12—Fe1-N7 80.9(3) Table 22. Selected bond distances (A) and angles (°) for [Mn(tppz)2][ClO4]2 (l9). Mn(l)—N(2)#1 2.227(8) Mn(1)-N(l)#1 2.241(11) Mn(1)-N(2) 2.227(8) Mn( 1)-N(1)#2 2.241(11) Mn(1)-N(1) 2.241(11) Mn(l)-N(1)#3 2.241(11) N(2)#1-Mn1-N2 180.0 N(1)#1-Mnl-N(1)#2 144.7(4) N(2)#1-Mnl-N(l)#l 72.3(2) N l-Mnl-N(1)#2 9529(12) N2-Mn1-N(1)#1 107.7(2) N(2)#1-Mn1-N(l)#3 107.7(2) N(2)#1-Mnl-N(1) 107.7(2) N2-Mn 1 -N(1 )#3 72.3(2) N2-Mn1-N1 72.3(2) N(1)#l-Mn1-N(l)#3 9529(12) N(l)#1-Mnl-N1 9529(12) N1-Mnl—N(1)#3 144.7(4) N (2)#1-Mn1-N(1)#2 72.3(2) N (l)#2—Mn1—N(l)#3 9529(12) N2-Mn1-N(1)#2 107.7(2) Symmetry transformations used to generate equivalent atoms: #1 y,-x+l,-z ; #2 -y+1,x,-z #3 -x+1,-y+l,z; #4 x+0,-y+1/2,-z+1/4 Another aspect that should be considered is that the nitrogen atoms of the non- coordinated, pyridyls rings are rotated away from each other, and do not form a terpy coordination environment. The final angle to note in these compounds is the one between the coordinated and non-coordinated pyridyl rings. These deviations from coplanarity are quite large (0 in 152 .bta-u go 8.3 05 ..8 85:5 022 macaw comp—gm 868:6 Essen saw .23 3: 606.2886": 5 :88 5829: 65 .6 8:88:62 2833 .852: Am 2:3... Amvvu 14% J.,/:43 830 .. A530 0;. '3 l‘ O l, 6:6 6 r 2 u 88 62 3:06” . . 88 m« l ’/ anU 8va 153 SEE... .6 8.3 05 8.. 68:80 803 383 comets»: 620850 88% es, 382 8666 36: 666: 65 55 a: 2085398389622 5 .666 65 6 6.266 668:6 666:... .Nm 2:5 154 Table 18 and Figure 48). All the values are near 60° with the exception of the Coll analogue. The specific values are 449°, 596°, 634° and 66.90 for Co", Fe", Mn" and Ni'l respectively. This deviation is in response to the steric interaction between the 2’ hydrogen atoms of the pyridyl rings. It is obvious from the X-ray structures of compounds (16)-(20) that the tppz moiety in these complexes experiences a great deal of distortion upon coordination. This observation helps to explain the difficulties encountered in using these as precursors for the self-assembly of larger supramolecular entities and the lack of electronic coupling between the two ligands, as evidenced by spectroscopic methods and cyclic voltammetry as previously discussed. Table 23. Selected bond distances (A) and angles (°) for [Ni(tppz)2] [C104]; (20). Nil-N2 1.981(4) Ni l-N3A 2.091(5) Ni l-N2A 1.990(5) Ni l-N 1A 2.094(5) Ni 1-N3 2.082(5) Ni l-N 1 2.101(5) N2-Ni l-N 2A 176.46(19) N3-Ni1—N1A 94.990 8) N2-Ni1-N3 78.70(l8) N3A-Nil-N1A 157.24(19) N2A-Ni 1-N3 99.59(18) N2-Nil-N1 78.39(18) N2-Ni1-N3A 97.81(18) N2A-Nil-N1 103.3608) N2A-Ni1-N3A 78.9908) N3-Nil-N1 157.0508) N3-Ni1-N3A 88.3008) N3A-Ni l-Nl 96.0909) N2-Ni1-N1A 104.9208) NlA-Ni l-Nl 89.6308) N2A-Ni1-N1A 7826(19) 155 .btflo .0 8.3 05 8.. 68:80 :32 3a... 858 come—u»... 668% E6386 .88 56. Sue Aeofifinaéz. 5 866 66866 65 6 @586 668:6 6:55. .8 2:5 52 .4 330 .y . A» E 156 B. Synthesis of the dinuclear compound [Ni2(tppz)(CH3CN)6][BF4]4. B.l. Synthesis In all previous cases, attempts to synthesize a dinuclear compound of the form [Mz(tppz)(CH3CN)6][X]4 where M = Mn", Fe" and Coll were unsuccessful regardless of the ratio of reagents, solvent, anion or temperature conditions. The exception to this situation is Ni". In this particular case, the choice of anion appears to play an important role in whether the product is mononuclear or dinuclear, as previously discussed. In the presence of [BF.;]', the dinuclear product is formed rather than the mononuclear form. The reaction was performed under anaerobic conditions in acetonitrile in a 2:1 ratio of [Ni(CH3CN)6][BF4]2 and tppz (Eq. 9). CH3CN _ 2[Ni(CH3CN)6] [1312,12 + tppz > [N12(tppz)(CH3CN)s][BF414 (Eq. 9) yield: 66% The reaction proceeds instantaneously, with the solution changing from a pale blue to a dark yellow color within minutes. Solvent is another variable that has to be taken into consideration. Alcohols and water promote the formation of insoluble products. Aprotic solvents, such as acetone or dichloromethane promote the formation of the mononuclear form as indicated by IR and UV-Visible spectroscopies. The only conditions that appear to favor the assembly of the dinuclear complex are the combination of CH3CN and [BF.;]' Crystals of [Ni2(tppz)(CH3CN)6][BF4]4 were obtained by adding diethyl ether to a concentrated solution of the compound in acetonitrile and placing it in the freezer at 157 -10°C for 10 days. The crystals are highly hygroscopic and readily decompose in the presence of moisture. B.2. Spectroscopic and cyclic voltammetric studies. UV-Visible spectroscopic studies of the dinuclear compound [Ni2(tppz)(CH3CN)6][BF4]4 in acetonitrile led to the observation of three electronic transitions. Two of the transitions are nearly identical to the mononuclear species [Ni(tppz)2][C104]2 (20) and appear at 7km, = 354 and 292 nm with e = 2.5 x 104 and 2.4 x 104 L-(mol°cm)'l respectively. In addition to the previous two transitions, there is a third feature at 74m. = 241 nm (8 = 4.2 x 104 (L-(mol°cm)"). As in the previous case, these transitions can be assigned to MLCT transitions between the metal center and low lying 7t* orbitals in tppz. The cyclic voltammogram exhibits one reversible reduction at Er}, = -0.4 V, a quasireversible reduction at Etc = -1.10 V and a reduction wave at Ep,c = —1.5 volts without accompanying wave. These studies indicate that weak electronic coupling between the two Ni" centers is occurring. As will be pointed out in the next section, the weak coupling can be attributed to the disruption of planarity of the pyrazine ring upon coordination of both Ni" centers, with the subsequent disruption of the n-system. B.3. X-ray crystallographic studies. The Ni" center resides in a highly distorted octahedral geometry with the angle between the pyridyl and pyrazine rings and the metal center of N(3)-Ni(l)-N(2) = 78.1 (3)° (Figure 60). The angle between the acetonitrile ligands is close to the ideal value 90° (N(5)-Ni(l)-N(6) = 88.3 (2)°). The shortest M-N distance is to the pyrazine ligand at Ni(l)-N(2) = 2.025 (2) A, followed by the M-N(CH3CN) distances at an average value of 158 5.3.0 h... 8.3 2.. 8.. 68...»... 8.. «:83 Swap»... 662% seen 6.3 .5 208.541.... ...zummuxaécz. 6 6:8 66866 2: 6 6686 286.6 666:... ...m 2:»... 3.2 . < 330 4 / . .97. 6:0 68 62 - .1. m4 4: 4 .. ,\' 1.. :1 .I 9' 5., mm. .1, A: ..._z 9. ll. 44 14,. . ..E ".4 ‘4 So ”..._. Eu 4.“ 830 A! 5. $30 .... 159 2.083 [3] A. The longest M-N distance is to the pyridyl ring (2.104 [3] A). The two coordinated pyridyl rings are not coplanar to each other, posessing a dihedral angle of 9.2 °. The central pyrazine ring is twisted at an angle of 129°. Table 24. Selected bonds (A) and angles (°) for [Ni2(tppz)(CH3CN)6][BF4]4-CH3CN (21). Ni 1-N2 2.025(2) Nil-N1 2.100(2) Ni 1-N5 2.043(2) Ni 1-N3 2.108(2) Ni 1-N6 2.090(3) Ni l-N4 2.115(3) N2-Ni1-N5 177.3100) N5-Nil-N1 100.08(9) N2-N i l-N6 8994(9) N6-Nil-N1 94.64(9) N5-Ni l-N6 8826(10) N2-Ni1-N3 7806(8) N 2-Ni l ~N1 7808(8) NS-Ni l-N 3 103.84(9) C. Reactivity studies of [M(tppz)2]2+ (M = Ni“, Fe", Co", Mn") and [NizttpszCHaCN).l‘*. As stated earlier, the goal of synthesizing and characterizing the mononuclear species [M(tppz)2]2+ and the dinuclear compounds represented by [Ni2(tppz)(CH3CN)6]4+ is to use them in the assembly of extended arrays. Several approaches were undertaken to connect these precursors through their accessible coordination sites, (see Figure 6, Chapter 1). One attempt involved the reaction of [Ni2(tppz)(CH3CN)6]4+ with two equivalents of the mononuclear species [Co(tppz)2]2+, with the aim of synthesizing the tetranuclear species [(tppz)Co(tppz)Ni(tppz)Ni(tppz)Co(tppz)]8+. Various reaction conditions were used, including different solvents such as acetonitrile, acetone, dichloromethane and alcohols, and various temperature conditions. The outcome in every case was the isolation of mononuclear species such as [Ni(tppz)2]2+, [Co(tppz)2]2+ as corroborated by X-ray crystallography. Another approach that was taken is to use 160 FeC13(tpy) as the source of the second coordinating metal. In this particular case, Fe(tpy)Cl3 was reacted with the [M(tppz)2]2+ complexes in a 2:1 ratio. The products that were isolated are [Fe(tppz)2]2+, Fe(tppz)Cl2 and [Fe(tpy)2]2+, which result from ligand redistribution and reduction of Fe(III) to Fe(II). These results indicate the that the [Fe(tppz)2]2+ species is quite stable. Additional attempts to prepare oligomers were performed in which the included reactions of [M(tppz)2]2+ with two equivalents of [M(CH3CN)6][X]2 or [M(H20)6][X]2 (M 2 Ni”, Co", Fe"; X = [BF4]’, [004]"). This reaction is based on the fact that two the dangling coordination sites on [M(tppz)2]2+ cations could allow for a trinuclear product to be assembled. In most cases, an insoluble product was obtained, suggesting that a polymer or higher order oligomer is being formed. On several occasions, crystals were isolated, but these were inevitably the mononuclear species [M(tppz)2][X]2. D. Reactions of C00; with tppz and tpy ligands. D.1. Synthesis. After noting that [Co(tppz)2][PF6]2 (17) exhibits spin-crossover behavior we became interested in adding two additional Co(II) centers at the open coordination sites to produce a trinuclear complex (Figure 55). The presence of three Co" ions instead of one could lead to cooperative spin crossover or even multiple step spin crossover. In pursuit of the proposed trinuclear compound, a Coll starting material that possesses three open coordinating sites, namely [mer-Co(tpy)(CH3CN)3][BF4]2 was used. In an attempt to prepare the unknown compound [Co(tpy)(CH3CN)3][BF4]2, CoClz was treated in a 1:1 ratio with tpy in order to first prepare [Co(tpy)Clz(CH3CN)]. The next step was to 161 abstract the Cl' ions from [Co(tpy)C12(CH3CN)] with AgBFa in acetonitrile so that the compound [Co(tpy)(CH3CN)3][BF4]2 could be obtained. _ _ _2+ 1 / \ 2* / 4 / 4 Q Q CCH3 2 0.0—NCCH3 + . O O CCHa /_\ 69 0 +6 09‘ 4 ,0. <99 Ho 06> Figure 55. Schematic drawing of the proposed synthesis of [C03(tpy)2(tppz)2]6+ from the reaction of [Co(tppz)2][PF6]2 with two equivalents of [Co(tpy)(CH3CN)3][BF4]2. We reasoned that this mononuclear partially solvated species, would be an ideal building block because of the presence of the tpy capping ligand. Instead of the anticipated [Co(tpy)(CH3CN)3][BF4]2 compound however, the dinuclear compound [Coz(tpy)2(CH3CN)2Cl2][BE]; (26) with two bridging Cl' ions was obtained instead. The 162 8.000 n.0 00:30.6. 0... E 05%.. N0... 05 .0 .coEwSEwom 0m 0.5»... m:.::000 we... 003.36 .80.). \_z z_/ / z \ 1v. _/ 3.x 7. \I..\.—0n—v \ 163 reaction of [Coz(tpy)2(CH3CN)2C12][BF4]2 with [Co(tppz)2][BF4]2 in the presence of an excess of [n-BuaN][PF6]afforded the polymer {[C02(tppz)2(CH3CN)2C12][BFa][PF6]}.. (22). The product is a l-D chain with alternating bridging Co(u-Cl)2Co and Co(tppz)Co units. Once the existence of {[Coz(tppz)2(CH3CN)2Cl2][BF4][PF6] }. (22) had been confirmed by X-ray crystallography, a more direct route to its synthesis was attempted. The polymeric material CoClz was used as the source of Co" and reacted in 1:1 ratio with tppz. The outcome of this reaction is an unexpected rearrangement of the tppz moiety, as shown in Figure 63. This ligand rearrangement allows for the coordination of two Co(II) centers in a molecular square (Figure 66). D2. Spectroscopic and cyclic voltammetric studies. The cyclic compound [Coz(tppz’)2][PF6][C02Cl7] (25) displays two electronic transitions in the UV-visible spectrum, at 70m = 680 nm (e = 3.7 x 102 L°(mol-cm)") and Am. = 588 nm (e = 3.7 x 102 L°(mol-cm)"). Both transitions can be assigned to MLCT transitions in which electrons from the d orbitals of the metal are promoted to the low lying 7t* LUMO of the tppz ligand. The cyclic voltammogram displays an irreversible reduction wave at Ep,c = —0.75 V; there is no evidence of an oxidation of the metal up to 2.0 V. D.3. X-ray crystallographic studies. In the tpy derivative [C02Clz(tpy)2(CH3CN)2][BF4]2 (26), the C001) center resides in a highly distorted octahedral environment as illustrated in Figure 57. The pyridyl and the pyrazine interaction with the metal is N(l)—Co(1)-N(2) = 76.15 (3)°, which is a 138° deviation from an ideal 90° angle. The acetonitrile and the pyrazine moieties are 164 separated by N(4)-Co(l)-N(2) = 99.92 (2)°, which is a 99° deviation from ideal octahedral coordination. Finally, the two bridging chlorine angle Cl(1)-Co(l)-Cl(1)* = 86.24 (3)°. The Co—N distances (in increasing order) are N(2)—Co(1) = 2.078 (3) A, N(4)- Co(l) = 2.127 (3)/3., and N(1)-Co(l) = 2.146 (3) A for pyrazine, acetonitrile and pyridyl interactions, respectively. The metal centers are 3.562 A apart. It is worth noting that the midpoint of the dinuclear unit resides on an inversion center; thus, only one-half of the molecule is unique. Table 25. Selected bond distances (A) and angles (°) for [C02C12(IP)')2(CH3CN)2] [BF412- (26)- Col-N2 2.078(3) Col-N1 2.150(3) Col-N4 2.127(3) Col-C11 2.3679(9) Col-N3 2.141(3) Col-C12 2.510(1) N 2-C01-N4 99.9200) N3-C01-Nl 151.3600) N2-Col-N3 75.6400) N2-Col—Cll 172.58(7) N4—Col-N 3 90.6700) N4-Col-Cll 8729(8) N 2-Col-N 1 76.1500) N3-Col-Cll 102.68(7) N 1 -Co 1 -C11 105.93(8) N2-Co 1 -C11 8649(7) N4-Col-N1 89.3800) N4-Col-Cll 173.17(7) The compound {[CozClz(tppz)(CH3CN)2][BF4][PF6] - CHZClz}... (22) was obtained from the reaction of [C02Cl2(tpy)(CH3CN)2][BF4]2 (26) in a 2:1 ratio with [Co(tppz)2][PF6]2 in acetonitrile. This compound is similar to [CozCl2(tpy)(CH3CN)2][BF4]2 (26), but, in this case, the tpy ligands have been substituted by tppz units, which allows for the growth of a l-D polymer (Figure 58). The Co(H) centers are linked on one side by bridging Cl‘ ions and on the other side by a tppz unit. The two Co(II) centers linked by the Cl- ions are 3.509 A apart from each other, which is 0.053 A shorter than in the dinuclear compound [Coz(tpy)Clz(CH3CN)2][BF4]2 165 09.5.0 .0 8.3 2.. ..0. .00....00 0.03 350... comet»... .m...0m.....0 .... em 5.3 GM. ”Tum.1.7.0.306996530. ... 00:3 2.. .0 wEBEn. Sm 0.5»... 0:0 .80 h. .... c A. t 166 (26) (Figure 57). The distance between Co" centers linked by the tppz unit is much larger, namely 6.792 A, which is nearly twice the distance between Coll centers bridged by two Cl' ions. Each metal center is in a very distorted octahedral coordination environment that consists of one tppz, one CH3CN and two Cl' ions. Three of the coordination sites are occupied by the tppz ligand, one by an acetonitrile molecule, and finally two bridging chlorine atoms (Figure 64). Table 26. bond distances (A) (°) for {1C02(IPPZ)(CH3CN)2C12] [BF411PF6] ° CH2C12 }. (22)- Co 1 —N 5 2.085(6) C02-N2 2.081(6) Co 1 -N6 2.102(6) CoZ-Nl 2.1 14(6) Col -N8 2.1 12(7) C02-N7 2.122(7) Co 1 -N4 2.1 13(6) C02-N 3 2.126(6) Co 1 -Cll 2.326(2) Co2-C12 2.319(2) Co 1 -C12 2.563(2) Co2-Cll 2.561(2) NS-Co 1 -N6 75.4(2) N2-C02-Nl 76.7(2) N 5-Co 1 -N8 95.8(2) N2-C02-N7 94.9(2) N6—Co 1 -N8 88.5(2) N l -C02-N 7 91 .9(2) NS-Co 1 -N4 76.0(2) N2-Co2-N3 75.2(2) N 6-Co 1 -N4 151.3(2) N l -C02-N 3 151.7(2) N8-Co 1-N4 922(2) N7 -Co2-N3 87.3(2) N 5-Col-Cl 1 171.7206) N 2-Co2—Cl2 171.6707) N6-Co 1 -Cll 103.63( 16) N1-Co2-Cl2 102.7006) N 8-Co 1 -Cl 1 92.34(19) N7-C02-C12 93 .4609) N4-Col-Cll 105.0106) N3-C02-C12 105.6006) N5-Col-Cl2 83.65(16) N2-Co2-Cll 83.3406) N 6-Col-Cl2 89.66(17) N l -Co2-Cll 90.1006) N8-Col-C12 178.1209) N7-C02-Cl1 176.9109) N4-Co l -Cl2 89.47(16) N 3-Co2-Cl 1 89.8007) Cll-Col-CIZ 88.14(7) The angle between the pyridyl and pyrazine ring in this polymer is 75.7 [3]°. which represents a 143° difference from the ideal value of 90°. The two chlorine atoms are asymmetrically bound, as evidenced by the two distances Co(1)-Cl( l) = 2.326 (2)A 167 666:6 0:688: 68 :6: 6686 .6: 66666.3 3. 662:6 0:688: so. 6:: as ..........Em.6.2086066666060.. 66:6: 0-. 6.: 6 6:68.262 66:6 666:... 3 .3 2:6... 3:0 \ J 6004.. l. . . . . .4 z 0 N 0 P. . .00 Ame—v0 A v 4‘1 ‘z. 4 _ 0 .t 330.. u. 330 r‘ .30 .65 0.0.0533. s. .32 32 .._.“ .0 .3... ..v. / u a .50 8.2 800 ,4, ‘ 4.. VI .M H000 4. m. «60 ..4 6.0 ... is a: 2 .80 “a. 66 .02 . $80 .Cz . 3:0 4..., 62 /7 ...V .60 4 ...4 .80 600 . 4... D. Av. 280.1 .300 3:0 \ 4. .450 «.0 t .80 890 ....U ‘2‘ -.xz C 13.0 AOCU 168 and Co(1)-Cl(2) = 2.563 (2)A. In the case of the Co(2)-Cl angles, the inverse situation is encountered (Figure 58). The Cl(2)-Co(l)-N(4) angle is 89.5 (2)°, which is close to the ideal value of 90°. On the other hand, the Cl(1)-Co(1)—N(6) angle is 103.6 (2)°, which is a large deviation from 90°. The M-N distance trend was the same as that observed in [Coz(tpy)C12(CH3CN)2][B13412 (26). The angles are Co(1)-N(5) = 2.086 (6) A, Co- N(6)/(4) = 2.108 [3] A, and Co(l)-N(8) = 2.113 (6)A for pyrazine, pyridyl and acetonitrile interactions, respectively. Table 27. Selected bond distances (A) and angles (°) for {[Coz(tppz’)2][PF6][C02CI7] (25). Col-N1 2.112(3) Col-N2A 2.149(3) Col-NlA 2.112(3) Col-N2B 2.149(3) Col-NIB 2.112(3) Col-NZC 2.149(3) Nl-Col-NIA 98.86(11) Nl—Col-NZB 88.6402) Nl-Col-NIB 98.86(11) N2A-Col-N2 95.84(12) NlA-Col-NlB 98.86(11) NlA-Col-N2C l71.99(12) Nl-Col-N2 88.6402) NlB-Col-N2C 8864(12) NlA-Col-N2 7705(12) NIB-Col-NZC 7705(12) NlB-Col-N2 l71.99(12) N2B-Col-N2C 95.84(12) NlA-Col-NZB 7705(12) N2-Col-N2C 95.84(12) NIB-Col-NZB l71.99(12) In [Coz(tppz’)2][PF6][C02Cl7] (25), the tppz’ ligand is the result of a rearrangement of tppz in the presence of C00; (Figure 59). The rearranged tppz ligand is composed of two equivalent units linked by a C-C tether (Figure 59a). Each one of these units is composed of a pyridyl ring joined to a six-membered ring which is fused to a five-membered ring (Figure 59). These two equivalent units can rotate around the C-C bond that links them together, which allows them to coordinate to two Co(II) metal centers 90° from each other. Two more units can be added to complete the cyclic unit 169 093.0 .0. 08.80 :08. 02:. 6.80... 880...»... 30.3....3 43.3.30... 3% ....3 88%.... $5.80 .8 .8: .8: 0.0.088»... . 6. 866268.666 6. 6.6 S. ..6: 666: 3 an. ......1.060.104.6680. 6 66:66 666:6 656:... am 2:6... 170 viewed in Figure 62a. The distance Co(1)-N(2) = 2.149 A is longer than the metal interaction to the fused rings at Co(1)-N(l) = 2.112 A. The metal center resides in a highly distorted octahedral geometry composed of three equivalent chelating interactions from a pyridyl and a five-membered ring. The angle between the pyridyl and the five membered ring N (1*)-Co(1)-N(2) = 77.1 (2)0 (Figure 59). E. Reactions of cis-[Rh2(02CCH3)2(CH3CN)6][BF4]2 and [Rh2(CH3CN)101[BF 414 With tppz. E.l. Synthesis A careful search of the literature in the last 40 years reveals that tppz has been used exclusively in mononuclear metal complexes'é“ Reports by Pruchnnik and coworkers17 and observations in our own laboratories with bipyridine and terpyridine ligand on [Rh2]4+ prompted us to react tppz with metal-metal bonded compounds. In one such reaction, [Rh2(OzCCH3)2(CH3CN)6][BF4]2 was selected as a source of RM” because of its availability and stability. The reaction with tppz was performed in a 1:1 ratio in H20. At room temperature no reaction was observed, but, with heating, the purple solution of the starting material gradually changes to a pale brownish red color and finally to green. At this point, the reaction must be ceased, otherwise cleavage of the metal-metal bond with concomitant oxidation to Rh(III) bond takes place, as evidenced by isolation of [Rh(tppz)2]3+. The product is recovered by evaporation of the H20. A methanol solution of the product was layered with toluene and green platelet crystals were observed to grow over a period of two months (yield 15%). X-ray studies revealed that these crystals are the “dimer of dimers” [Rh4(02CCH3)2(IPPZ)2(CH30H)4][PF616'CH30H (24)- 171 With the successful isolation of the [Rha]4+ compound from [Rh2(OzCCH3)2(CH3CN)6][B134]; we turned to another source for the [Rha]4+ core, namely [Rh2(CH3CN)to][BF4]4. The 1:1 reaction between [Rh2(CH3CN)m][BF4]4 and tppz was performed in acetonitrile, and, upon mixing, the orange solution changed immediately to a brown color solution from which the mononuclear Rh'" species, was isolated [Rh(tppz)2][BF4]3. In an attempt to avoid the presumed disproportionation reaction, the reaction was performed at low temperature and in the absence of light, but we were not able to avoid the formation of [Rh"'(tppz)2]3+. The fate of the other half of the reaction, namely the Rhl species is not known. E2. Spectroscopic studies. The mononuclear species [Rh(tppz)2][BF4]3 (23) exhibits interesting electronic spectral properties. Four electronic transitions were located in the range of 200-800 nm. The lowest energy transition occurs at Am. = 749 nm (e = 2.9 x 103 L°(mol'cm)"). The others appear at Km“ = 517 nm (e = 1.6 x 104 L-(mol-cm)"), at Am = 437 nm (e = 1.4 x 104 L-(mol-cm)"), and at Am = 405 nm (e = 1.45 x 10‘ L-(mol-cm)°'). All of these transitions are presumed to be MLCT transitions based on their high molar absorptivity coefficients. B.3. X-ray crystallographic studies. Compound (24), [Rh4(OzCCH3)2(tppz)2(CH3OH)4][PF6]6-CH30H, consists of a rectangular unit based on two Rh-Rh bonds and two M-tppz edges. The coordination sphere of the Rh" ions consists of three nitrogen atoms from the tppz ligand, two oxygen atoms, (one from the bridging acetate and the other from 21 methanol molecule), and finally the Rh-Rh bond (Figure 61). The angle between the pyridyl and pyrazine 172 nitrogens, Rh(2)-N(2)-N(3) is 81.2 (3)°. The N(l)-Rh(2)-N(3) = 160.3 (3)° angle, which involves the pyridyl rings, is far from the ideal 180°. The shortest of the three Rh-N distances is the Rh-pyrazine distance of Rh(2)-N(2) = 1.934 (7) A, followed by the Rh- pyridyl distance Rh(2)-N = 2.030 [8] A (Figure 60). Table 28. Selected bonds distances (A) and angles (°) for [Rh4(02CCH3)2(tppz)2(CH30H)4][PF6]6-CH3OH (24)- Rhl-N2A 1.929(7) Rh2-N2 1.934(7) Rh l-N l A 2.041(7) Rh2-N1 2.010(8) Rh 1-02 2.054(7) Rh2-N3 2.047(8) Rh 1—03 2.245(7) Rh2-Ol 2.053(7) Rh 1-Rh2 2.6058(11) Rh2-O4 2.216(8) N2A-Rh l -N3A 81.7(3) N 2-Rh2-N1 80.7(3) N2A-Rh1-N1 A 81.0(3) N2-Rh2-N3 81.2(3) N 3A-Rh l -N l A 160.6(3) N1-Rh2-N3 160.3(3) N2A-Rh1-02 179.0(3) N2-Rh2-Ol 178.5(3) N3A-Rh1-02 98.8(3) N l -Rh2-Ol 1002(3) N 1 A-Rhl-02 98.4(3) N3-Rh2-Ol 97.8(3) N2A-Rh1-O3 93.0(3) N 2-Rh2—O4 95.3(3) N3A-Rh1-O3 88.4(3) N1-Rh2-O4 89.6(3) N1A-Rhl-O3 83.8(3) N3-Rh2-O4 84.4(3) OZ-Rhl-OB 862(3) Ol-Rh2-O4 83.5(3) N2A-Rh1-Rh2 95.9(2) N 2—Rh2-Rh1 962(2) N3A-Rh1-Rh2 91.2(2) N 1—Rh2-Rhl 90.6(2) N1A-Rh1-Rh2 99.3(2) N 3-Rh2-Rh1 99.0(2) 02-Rh 1 -Rh2 85.0(2) Ol-Rh2-Rh1 85.0(2) O3-Rh 1-Rh2 171.0(2) O4-Rh2-Rhl 168.4(2) The molecular cation is a rectangle in which each Rh-Rh unit is a short edge of the rectangle and tppz units are the long edges. The Rh-Rh bond distance is 2.606 (1)A, which is within the expected range for a Rh-Rh single bond.‘8 The distance between tppz bridged Rh" atoms along is 6.749 A and the diagonal of the rectangle is 6.977 A. The tppz units are highly distorted, with the planes of the two coordinating pyridyl units on the same Rh atom forming a dihedral angle of 27.4°. The pyrazine ring exhibits a dihedral 173 446m 2: a :40 8048066....080480.466...4.4800406:... 6 .6: 6:66:66 6:. 6 6.4. .90 8:0 830 4\\\~ 404 .30 .’ WV R .40 s. 2% ....U (1.1.1 \ . .82 .80 Ir 1 ..._.i ...O ..o>0. 5:530... 0.3050 .6808... . , 2.30 fun/... ‘4. 22.02% 252 . (‘54 \ Aw=—r “E. 3.30 1‘ ‘ .NVO . .. $80 .._w 44.444 9430 .200 K 4...: .8 2:»... 174 .4953. . .945 08% 5 .92 $5384. 4444 cm 2: 0 EEO : 022.. 2:03 cowegm .8an 05 ..o Efiwfiu . . an 4m AWWmMmfiwofimaEmfiuiaéfimouavaa s 8:8 54.8.2: :3 05 40 8334.32? 289:0 3542: 3 G 2 E a a I, 1.... .2' 175 angle of 19.46 °. A close look at the space filling diagram in Figure 68 shows the remarkably good fit of the two twisted tppz units in this molecule. Table 29. bond distances (A) and angles (°) for [Rh(tPPZh] [BF413'2CH3CN'C4H80 (23)- Rh 1 -N2A 1.962(6) N2-C19 1.345(10) Rh 1-N2 1.975(6) N4-C7A 1.347(10) Rhl-N3 2.035(7) N4A-C13A 1.348(9) Rhl-Nl 2.032(7) N4-C13 1.335(10) Rh l-NlOA 2.054(6) N4-C7 1.355(10) Rh 1-N3A 2.066(7) N2A—C19A 1.334(10) N 2-N 6 1.334(9) N2A-Rh 1 -N2 178.0(3) N3-Rh l -N10A 91 .3(3) N2A-Rhl- 100.7(3) Nl-Rhl-NIOA 91.8(3) N2-Rh1-N3 80.3(3) N2A-Rhl-N3A 80.7(2) N 2A-Rh 1 -N1 98.9(3) N2-Rh l-N3A 97.5(3) N2-Rh1-Nl 80.2(3) N3-Rh l -N3A 91 .9(3) N3-Rh 1 -N1 160.4(2) N 1 -Rh 1 -N 3A 91 .3(3) N2A-Rh1-N10A 80.5(3) N lOA-Rh 1 -N3A 161.2(2) N2-Rh1-N10A 101.3(3) Compound (23) contains a mononuclear Rh(HI) cation in a distorted octahedral geometry (Figure 69). The angle between the pyrazine and pyridyl rings and the Rh atom is N(l)-Rh(l)-N(2) = 80.2 °, which is much less than the ideal 90°. The angle N(l)-Rh(1)- N(3) between two pyridyl rings is 160.4°, also far from the ideal. The tppz experiences severe distortions, with two of the non-coordinating pyridyl rings forming an angle of 37.11° between them. The pyrazine ring is twisted by 9.68 °. In the case of coordinated and non-coordinated pyridyl rings, they are twisted as far as possible at 48.31 °. The driving force for this is most likely the steric interaction of the 4,4’ hydrogen atoms. 176 .4953 be 8.3 05 .5.“ 3280 coon 0%: 2:9“ come??— .mEOm&=u 38.85 bzfianoa 8% 543 Andy ZUMEUNéameuhfimm—H339E”: E 8:8 05 46 :ozaucomoaom .Nw 95”.,”— A<~NVU . $1 226 ,3 .4 //. t :32 4.4 330 .k :58 ' .Ir; DE. 4. \ » .\\ $2 so I A [Mn(tptaz)(H20)][CF3SO3]2 (Eq. 12) yield: 91% In a typical reaction, [Ni(CH3CN)6][BF4]2 was dissolved in acetonitrile to form a bright blue solution, and one equivalent of tptaz was added. The color of the reaction changed to pale yellow and finally to pale yellow green within 8 hours (Eq. 10). Layering of the solution with toluene, benzene or diethyl ether affords crystals of [Ni(tptaz)(CH3CN)2(H20)2][BF4]2 within days. It must be pointed out that the acetonitrile cannot be completely dry, otherwise, the compound will not crystallize. Several attempts to coordinate a second Ni" center to the already formed [Ni(tptaz)(CH3CN)2(H20)]2+ (27) 178 molecule were unsuccessful. This may be due to the inductive effect of the first metal on the triazine ring, which renders the triazine ring much less basic. The compound [Fe(tptaz)2][ClO4]2, (28), results from the reaction of [Fe(H20)6][ClO4]2 with tptaz in a 1:2 ratio (Eq. 11). The reaction takes place instantaneously, with the color changing from a colorless Fe(II) solution to a deep blue solution within minutes. All attempts to prepare polynuclear compounds by varying the reaction conditions were unsuccessful. Crystals of the mononuclear compound were obtained by layering with diethyl ether or THF or by slow evaporation of the reaction mixture. For the synthesis of [Mn(tptaz)(phen)(H20)][O3SCF3]2 (29), a slightly different approach was taken. Instead of using a “naked” cation (in which all six coordination sites are occupied by labile water or acetonitrile molecules), [Mn(phen)2](O3SCF3]2 was employed. This precursor contains four coordination sites occupied by phenanthroline molecules (capping ligands), and two sites occupied by weakly coordinating triflate ([CF3SO3']) anions. By using this precursor, it was intended that the tptaz would coordinate in its middle bidentate coordination site (Figure 46), allowing for the coordination of a second metal center in a subsequent step in the tridentate site. The reaction was performed anaerobically, with a 1:1 ratio of [Mn(phen)2(O3SCF3]2] and tptaz in acetonitrile (Eq. 12). The reaction was instantaneous, as judged by an immediate color change to light yellow. The outcome of the reaction is the mononuclear species [Mn(tptaz)(phen)(H20)][O3SCF3]2 (29) in which the tptaz ligand is coordinated through its major coordination site (tpy mode), which requires the displacement of one phenanthroline molecule. Further attempts to coordinate a second Mnll metal center on 179 the available bpy coordination site (middle coordination site, Figure 46) by adding an excess of either [Mn(CH3CN)4][BF4]2 or [Mn(phen)2(03SCF3]2] (with and without refluxing) were unsuccessful. The mononuclear product was always obtained as evidenced by X-ray crystallographic studies. F.2. Spectroscopic and cyclic voltammetric studies UV-Visible spectroscopy of [Ni(tptaz)(CH3CN)2(H20)2][BF4]2 [Fe(tptaz)2][ClO4]2, [Mn(tptaz)(phen)(H20)][O3SCF3]2 revealed numerous electronic transitions. The tptaz ligand exhibits two electronic transitions in the UV region, the lowest energy one being at Amax = 279 nm (e = 3.0 x 104 L-(mol'cmf') and the higher energy one at Am“ = 244 nm (e = 3.0 x 104 L-(mol-cm)"). Both transitions are assigned to 1t—> 1t* electronic transitions. [Ni(tptaz)(CH3CN)2(H20)][BF4]2 (27) displays two electronic transitions at km, = 293 nm (e = 5.9 x 104 L'(mol-cm)") and Am” = 253 nm (e = 2.5 x 102 L-(mol-cm)"). The transition at A = 293 nm corresponds to a MLCT transition, based on its location and its absorption coefficient. The higher energy transition at Am“ = 253 nm is assigned to a rt—> 1t* transition of the ligand. [Fe(tptaz)2][ClO4]2 (28) exhibits three electronic transitions in the UV-Visible spectrum at Am” values of 568 nm, 341 nm and 243 nm with 8 values of 6.1 x 102, 6.5 x 105 and 4.3 x 103 L-(mol-cm)", respectively. The two lower energy transitions are assigned to MLCT transition and the higher energy one at km“ = 243 nm is a 1t—-> 1t* transition, as inferred from a comparison to the free ligand spectra. Finally, [Mn(tptaz)(phen)(I-120)][O3SCF3]2 (29) displays three electronic transitions at Am = 227 and 272 nm (assigned to 1t—> 1t* electronic transitions) and at Am“ = 292 nm, attributed to 180 4“ a MLCT transition. The e values are 5.0 x 10“, 7.0 x 10“, and 6.7x 104 L-(mol-cm)" for Am, = 292, 272 and 227 nm, respectively. Table 30. UV-Visible spectrosc0pic data for compounds (27)-(29). Mnm) 8 L-(mol-cm)’l 279 3.0 x 104 Tptaz 244 3.0 x 104 293 5.9 x 104 [Ni(tptaZXCHsCNXHzOH[BF412 253 2.5 x 102 568 6.1 x 102 [Fe(tptazhHClOdz 341 6.5 x 105 243 4.3 x 103 227 6.7 x 104 [Mn(tptaZXPhenXHzOH[038CF312 272 7.0 x 10‘ 292 5.0 x 10‘ The presence of energetically accessible 1t* orbitals leads to a rich electrochemistry for these molecules. Cyclic voltammetric studies show that [Fe(tptaz)2][ClO4]2 (28) exhibits the richest electrochemistry. The free ligand exhibits only a reversible reduction (Er, = -l.2 V), but upon coordination to Fe(II), four one- electron reductions became accessible as depicted in Figure 63. The four one-electron reductions of [Fe(tptaz)2][ClO4]2 (28), are found within the range —O.4 to -l.85 V. These reduction couples occur at El)” = -0.62 , Ewes = -0.75, E(3)% = -l.47 and EN)” = -l.7lV (Figure 63). In addition, there is an irreversible oxidation at E = +1.54 V that corresponds to the oxidation of Fe(II) to Fe(III) . An examination of the separation of the four couples allows for the calculation of the comproportionation constants for the two intermediates 181 as shown in scheme 4, based on the Robin and Day approach.19 The first two couples lead to a comproportionation constant of 1.57 x 102, which corresponds to a value on the borderline of class I and H. For the next two reversible couples, the Kc is 1.14 x 104, which falls in the category of class 11 (Scheme 4). 8x10.6 1 I 1 6x10'6 4x10"’ 2x10'6 4 x 10 '6 1 . 1 J -0.4 -0.8 -1.2 -l.6 -2 Volts Figure 63. Cyclic voltammogram of [Fe(tptaz)2][ClO4]2 in 0.1 M TBAPF6 acetonitrile at 3 Pt disk electrode versus Ag/AgCl. In marked contrast to the Fe(II) derivatives, [Mn(tptaz)(phen)(HzO)][OgSCF3]; (29) exhibits only one reversible reduction at Ev, = -1.47 V. There are three irreversible waves at Ep,c = —0.55, -O.72 and -0.80 V without corresponding anodic return waves. Finally, [Ni(tptaz)(CH3CN)2(H20)][BF4]2 exhibits a reversible reduction at EV2 = -O.5 V and a cathodic wave at EN = -l.03V with a return wave at E = -0.85V. 182 [1=e(tptaz)2]2+ ‘ _ L [Fe(tr>tetz)2]+ -e KC =1.57 x 102 +e' [Fe(tptaz)2]+ ‘ _ ‘ [Fe(tptaz)2] -e [Fe(tptaz)2] ‘ +8. ¥ [Fe(tptaz)2]' -e Kc=1.14x104 [Fe(tpta2)2]' ‘ +e ‘ [Fe(tptaz)2]2“ -e Scheme 4. E3. X-ray crystallographic studies. The compound [Ni(tptaz)(CH3CN)2(H20)][BF4]2 (27) consists of 21 Ni" center in distorted octahedral geometry (Figure 71). The coordination sphere is composed of two acetonitrile molecules, one water molecule and tptaz ligand coordinated at the tpy site (Figure 70). The shortest Ni-N bond is to the nitrogen of the triazine ring, (Ni(1)-N(2) = 1.982 (3)/31), followed by the acetonitrile interaction (2.037 [3]A). The longest distance is to the pyridyl rings at an average Ni-N distance of 2.134 [3]}t. The angle between the pyridyl and pyrazine rings and the nickel center is N2-Nil-Nl = 77.05 (11)°, which is far from the ideal 90°. The angle between the pyridyl and the acetonitrile ligands is N(l)- Ni(1)-N(8) = 103.17 (11)°. The two trans pyridyls are 154.1° apart from each other, 183 which is 259° from the expected 180°. With respect to the open middle coordination site, the dihedral angle between the triazine and pyridyl rings is only 9.4°. Table 31. Selected bond distances (A) and angles (°) for [Ni(tptaz)(CH3CN)(HzO)][BF4]2 (27). Nil-N2 1.982(3) Nil-OI 2.063(2) Ni l-N8 2.027(3) Nil-N3 2.134(3) Ni l-N7 2.047(3) Nil-N1 2.135(3) N 2-Ni 1-N8 179.70(12) N7-Ni1-N3 89.0801) N2-Nil-N7 91.51(12) Ol-NiI-N3 91.6600) N8-Nil-N7 88.29(12) N2-Nil-N1 77.05(11) N2-Ni l-Ol 88.84(l l) N8-Ni1-N1 103.l7(l 1) N8-Nil-Ol 91.37(11) N7-Ni l-Nl 90.68(11) N7-Ni l-Ol 179.24(11) Ol-Nil-Nl 88.7400) N2-Nil-N3 77.05(11) N3-Nil-N1 154.0901) N8-Nil-N3 102.72(11) In compound [Fe(tptaz)2][ClO4]2 (28), two tptaz units are present in the coordination sphere. The Fe" center resides in a distorted octahedral environment (Figure 72). The longest Fe(1)-N interaction is to the pyridyl ring, with an average value of 1.984 [3]/K, followed by the triazine with an average value of 1.862 [3]A. The angles throughout the coordination sphere reflect the distortion from an ideal octahedron. The angle between the pyridyl and triazine units and the Fe" center is 80.10 [12]° (almost a 10° difference from the ideal 90°). The coordinated pyridyl rings of the same tptaz molecule are 160.2° apart from each other, which is a 198° deviation from the expected 180°. The compound { [Mn(tptaz)(phen)(H20)] [CF330312 } { [Mn(tptaz)(phen)(H20)] [CF350312 } “H20 (29) crystallizes in the P-l space group with two independent co-crystallized molecules. Both 184 5.530 go 8.8 05 48 682:5 :39 024: 383 :w comes»: .35. 553242 seem 2: 44 ch v NEE:ONEAzofioxaaéE 5 8:8 2: 4o 83 289.3 .85.: a. s.. ..._ 2.30 4N. / $30 1 ‘x/ 630 .\\. . 7 2:0 5.5. ‘1 52 £30 and 830 4'4 t :80 74% :5 @z ”a... 330 5 .I/ 33o AW... 185 molecules contains a Mn(II) ion, but they exhibit different geometries. The first molecule consists of a Mnll ion in a distorted octahedral environment (Figure 74) whereas the second molecule contains a heptacoordinate Mn(II) ion. Table 32. Selected bond distances (A) and angles (°) for [Fe(tptaz)2][C104]2-2CH3CN (28). Fel-N2 1.859(3) Fel-N3A 1.983(3) Fel-N2A 1.865(3) Fel-Nl 1.988(3) Fel-N3 1.981(3) Fel-NlA 1.989(3) N2-Fe1-N2A 178.2303) N3-Fel-Nl 160.3802) N2-Fel-N3 80.3002) N3A-Fe1-N1 93.2802) N2A-Fe1-N3 101.0802) N2-Fel-N1A 98.8702) N2-Fel-N3A 101.1202) N2A-Fe1-N1A 79.9902) N2A-Fe1-N3A 80.0502) N3-Fe1-N1A 93.0302) N3-Fel-N3A 89.4202) N3A-Fe1-N1A 159.9902) N2-Fel-Nl 80.1102) Nl-Fel-NlA 91.0402) N2A-Fel-N1 98.5302) A close look at the molecule with seven ligands shows that it has pentagonal bipyramidal geometry (Figure 73). The equatorial plane is occupied by the tptaz nitrogens atoms (N(l), N(2), N(3)), a nitrogen from the phenanthroline N(7), an oxygen from a triflate 0(4), and finally the water molecule 0(7). In an ideal case, each atom in the pentagon should be 72° apart, which is close to what is observed in the structure. Some characteristic angles found in this plane are N (l)-Mn(2)-N(7) = 76.61 (11)°, N(1)-Mn(2)- N(2) = 67.00 (10)°, N(3)-Mn(2)-N(2) = 69.24 (11)° and O(3)-Mn(2)-N(7) = 75.11 (11)°. The two axial sites are occupied by a triflate molecule weakly coordinated through an oxygen atom, Mn(2)-O(4) = 2.164 (3)/X, and a nitrogen from the phenanthroline ring Mn(2)-N(8) = 2.277 (3)A. The molecule with the octahedral geometry (Figure 74) does not contain a coordinated triflate molecule; its coordination sphere is composed of a 186 .4956 we exam of 8... “48:80 soon 92 2:8.“ comegm 525895 44.44% a +~H~Ansacofi .538 05 we 8E 289:0 3:55. .me 2:»:— Ao_ b=BBEQ soon 05 a as 045 41842854522382855C4 4.40.04282048223448392.C E :2 :54 836.88 .5 05 .6 BE 20350 BEBE. .8 953.: 22 V0 $425 4' $580 230 225 250 a! “v ) «44v 2:6 A0_ 8cm 2: a as 04:: 4:48.00.2048923848062:_: 4:400nt:ONEABfixNaéeav 0:33er E 5:00 :52 0005280800: 05 .3 SE 289:0 3802:. .3 2: Cu , 50 $0 r440 » So / 0 \w 34va 2004 9 $va 4 ‘ l. W’ NNVU €90 1.. $30 AGO EU So flaw M. 3m , 2va ..\\\. iv. 50 7. (.4... Em \WW Amy: ‘11 0.5”...— 190 IV. Conclusions The ligand 2,3,5,6-tetrapyridylpyrazine (tppz) possesses two tridentate coordination sites which in principle can allow for the assembly of metal arrays. In our attempts to prepare such metal arrays, the mononuclear series [M(tppz)2][X]2 (M = Niz+, Co“, Fe“, Mn“; x = 004’, PFG‘, N03) was obtained by the reactions of [M(S),]2+ (s = CH3CN or H20) cations with two tppz ligands. The products exhibit interesting properties in their own right, and could give rise to interesting properties by associative effects if extended metal arrays can be obtained. Magnetic studies of [Co(tppz)][PF6]2 (17) revealed that this compound exhibits spin-crossover behavior. Previous studies with Coll and tpy derivatives have indicated similar behavior.20 The low spin configuration is obtained at T = 55K with S = '/2 and the high spin configuration is reached at T = 260 K with S = 3/2. From a structural point of view, [Co(tppz)2][PF6]2 presents a major difference from other spin-crossover Co(II) complexes, namely the availability of coordination sites for further chemistry. This compound is ideal as a potential building block for the construction of higher nuclearity species that incorporate a building block with spin-crossover behavior. A cyclic voltammogram of [Fe(tppz)2][C104]2 shows five fully reversible redox couples, which is quite remarkable. The four reductions indicate electronic communication between the two ligands. Calculation of the comproportionation constants show class I/II behavior for the first two reduction couples with Kc = 7.5 x 102. The next two reduction couples exhibit class II behavior with Kc = 3.7 x 104 (Scheme 3). Attempts to synthesize the dinuclear products [M2(tppz)2(CH3CN)(,]+4 (M = Ni", Co", Fe", Mn") were unsuccessful except in the case of [Ni2(tppz)(CH3CN)6][BF4]4. The 191 reaction was performed with a 1:2 ratio of tppz and [Ni(CH3CN)6][BF4]2. The identical reactions performed with any other anions e.g ([ClOa]', [PF6]', [NO3]') did not afford this product, but produced only [M(tppz)2]2+ instead. The choice of anion evidently plays a major role in the self-assembly process. Reactions of tppz with [Rh2(OAc)2(CH3CN)6][BF4]2 led to the isolation of a novel rectangle in which the longest sides are occupied by the tppz ligand units and the shorter sides are defined by the two Rh-Rh bonds. In the case of [Rh2(CH3CN).o][BF4]4 reactions, one observes only metal-metal cleavage and disproportionation with isolation of [Rh(t992)3l[BF413. In the tptaz chemistry, all of the metal ions coordinate only to the major tridentate site. In principle, it should still be possible to use these building blocks in further chemistry based on metal coordination to the bpy site. 192 V. References 1. (a) Goodwin, H. A.; Lions, F.; J. Am. Chem. Soc., 1959, 81, 6415. 2. Thummel, R. P.; Chirayil, S. Inorg. Chim. Acta, 1988, 154, 77. 3. (a) Constable, E. C.; Ward, M. D. J. Chem. Soc. Dalton Trans., 1990, 1405. (b) Collin, J-P.; Lainé, P.; Launay, J-P.; Sauvage, J-P.; Sour, A. J. Chem. Soc. Chem. Commun., 1993, 434. (c) Ruminski, R. R.; Letner, C.; Inorg. Chim. Acta, 1989, 162, 175. (d) Ruminski, R.; Kiplinger, J.; Cockroft, T.; Chase, C. Inorg. Chem, 1989, 28, 370. (e) Tondreau, V.; Leiva, A. M.; Loeb, B.; Boys, D.; Stultz, L. K.; Meyer, T. J. Polyhedron, 1996, 15, 2035. 4. Robin, M. B.; Day, P.; Adv. Inorg. Radiochem, 1967, 10, 247. 5. (a) Graf, M.; Stoeckli-Evans, H.; Escuer, A.; Vicente, R. Inorg. Chim. Acta, 1997, 25 7, 89. (b) Graf, M.; Greaves, B.; Stoeckli—Evans, H. Inorg. Chim. Acta, 1993, 204, 239. 6. Vagg, R. S.; Warremer, R. N.; Watton, E. C.; Aust. J. Chem, 1969, 22,141. 7. Half-Penny, J .; Small, R. W. H. Acta Crystallogr. B, 1982, 38, 939 8. (a) Thomas, N.C.; Foley, B. L.; Rheingold, A. L. Inorg. Chem, 1988, 27, 3426. (b) Chirayil, S.; Hegde, V.; Jahng, Y.; Thummel, R. P. Inorg. Chem, 1991, 30, 2821. (c) Berger, R. M.; Ellis, D. D., II. Inorg. Chim. Acta, 1996, 241, 1. 9. (a) Durharrn, D. A.; Frost, G. H.; Hart, F. A. J. Inorg. Nucl. Chem, 1969, 31, 571. (b) Lerner, E. 1.; Lippard, S. J. J. Am. Chem. Soc., 1976, 98, 5397. (b) Lerner, E. 1.; Lippard, S. J. Inorg. Chem, 1977, 16, 1546. (c) Embry, W. A.; Ayres, G. H. Anal. Chem. 1968, 40, 1499. (d) Janmohamed, M. J .; Ayres, G. H. Anal. Chem, 1972, 44, 2263. (e) Paul, P.; Tyagi, B.; Bilakhiya, A. K.; Bhadbhade, M, M.; Suresh, B.; Ramachandraiah, G. Inorg. Chem, 1998, 37, 5733. (f) Paul, P.; Tyagi, B.; Bilakhiya, A, K.; Dastidar, P.; Suresh, E. Inorg. Chem, 2000, 39, 14. (g) Paul, P.; Tyagi, B.; Bhadbhade, M. M.; Suresh, E. J. Chem. Soc., Dalton Trans., 1997 , 2273. 10. Hathaway et al. J. Am. Chem. Soc., 1962, 2444. 11. Case, F. H.; Koft, E. J. Chem. Soc., 1973, 905. 12. Theory and Applications of Molecular Paramagnetism, Boudreaux, E.A.; Mulay, L.N., Eds; John Wiley & Sons: New-York, 1976. 13. SAINT, Program for area detector absorption correction, Siemens Analytical X-Ray Instruments Inc., Madison WI 53719, USA 1994-1996. 193 14. SHELXL-97 — g.m. Sheldrick, SHELXL — 97 , Program for refining crystal structures, University of Gottingen, 1997. 15. Sawyer, D. T.; Sobkowiak, A.; Roberts, J. L. Electrochemistry for Chemists. 2nd edition. John Wiley & Sons, 1995. 16. (a) Tondreau, V.; Leiva, A. M.; Loeb, B. Polyhedron, 1996, I5, 2035. (b) Gourdon, P. L. A.; Launay, Inorg. Chem, 1995, 34, 5156. (c) Brewer, R. G.; Jensen, G. E.; Brewer, K. J. Inorg. Chem; 1994, 33, 124. (d) Ruminski, R. R.; Letner, C.; Inorg. Chim. Acta, 1989, 162, 175. (e) Ruminski, R. R.; Kiplinger, J .; Cockroft, T.; Chase, C.; Inorg. Chem, 1989, 28, 370. 17. Pruchnik, F. P.; Robert, F.; Jeannin, Y.; Jeannin, S. Inorg. Chem, 1996, 35, 4261. 18. Cotton, F. A.; Walton, A. R. Multiple Bonds Between Metal Atoms. Second ed., 1993 and references therein. 19. Robin, M. B.; Day, P.; Adv. Inorg. Chem. Radiochem., 1967, 10, 247. 20. (a) Zarembiwithch, J .; Kahn, 0.; Inorg. Chem, 1984, 23, 589. (b) Judge, J. S.; Baker, W. A.; Inorg. Chim. Acta, 1967, I, 68. (c) Kremer, S.; Henke, W.; Reinen, D.; Inorg. Chem, 1982, 21, 3013. (d) Heinze, K.; Huttner, G.; Zsolnai, L.; Schober, P. Inorg. Chem, 1997, 36, 5457. 194 Chapter IV A Homologous Series of Redox-Active, Dinuclear Cations [M2(ozccn3)z(pynp)]2+ (M = Mo, Ru, Rh) with the Bridging Ligand 2-(2-Pyridyl)-1,8-naphthyridine (pynp). 195 I. Introduction In our quest for nitrogen heterocyclic ligands that are capable of spanning a dinuclear unit, we found several references on the use of cavity-shaped ligands such as 2- (2-pyridyl)—1,8—naphthyridine (pynp)l and 2,7-bis(2-pyridyl)-1,8-naphthyridine (bpnp)6(°)‘(d)'(g) (Figure 68). The pynp and bpnp molecules are relatively rigid tridentate and tetradentate ligands, that possess, in addition to the naphthrydine bridging unit, one or two pyridyl binding sites that can be used to bind to the axial positions of a dimetal unit. The pynp ligand (Figure 68) can act as a tridentate combination bridging/chelating ligand as in the case of [Rh2(OzCCH3)2(pynp)2]2+ or a chelating, bpy mode in the case of [Rh2(pynp)3C12][PF45]-CH3CN.lb These compounds were found to exhibit interesting electronic properties, but, in the intervening years since these examples were published, no additional reports of M-M bonded pynp compounds have appeared in the literature, and only one X-ray structure has been reported.lc This chapter is devoted to the study of the coordination chemistry of 2-(2-pyridyl)—l,8—naphthyridine (pynp) with [M02]4+, [Rufl‘w5+ and [ha]4+ dimetal complexes and a comparison of the structures and redox properties of the homologous series [M2(02CCH3)2(pynp)2]2+ (M = M0, Ru, and Rh). /|\ \ / N |\ N/ bpnp PynP Figure 68. Schematic drawings of the bpnp and pynp ligands. 196 11. Experimental Section All manipulations were performed under an inert atmosphere with the use of standard Schlenk-line techniques. Acetonitrile was freshly distilled over 3A molecular sieves and methanol was pre-dried over 4A molecular sieves and then distilled over NaOMe. The solvents diethyl ether and toluene were freshly distilled over Na/K amalgam. The ligand 2-(2-pyridyl)-l,8-naphthyridine (pynp) was prepared by a modified literature procedure.2 The starting materials [Rh2(02CCH3)2(CH3CN)6][BF4]2,3 [Moz(02CCH3)2(CH3CN)6][BF.4]23'4 and Ru2(OzCCH3)4C15 were prepared by literature methods. Physical Measurements. 'H NMR spectra were obtained on a Varian VXR BOO-MHz spectrometer Gemini- 200. Electrochemical measurements were carried out by using an H CH Electrochemical Analyser model 620A. Cyclic voltammetry experiments were performed in CH3CN containing 0.1M tetra-n-butylammonium hexafluorophosphate (TBAPFs) as the supporting electrolyte. The working electrode was a BAS Pt disk electrode, the reference electrode was Ag/AgCl and the auxiliary electrode was a Pt wire. The ferrocene couple occurs at E”; = +0.52V vs Ag/AgCl under the same experimental conditions. Magnetic susceptibility measurements were obtained with the use of a Quantum Design SQUID magnetometer MPMS-XL (housed in the Department of Chemistry at Texas A&M University). Data was collected in the temperature range 1.8-350 K at 1000 G on finely divided polycrystalline samples. The raw data was corrected for the contribution of the sample holder and the diamagnetism of the constituent atoms by the use of Pascal constants.° 197 Theoretical Details. A companion theoretical study for the experimental work in this chapter was performed by Dr. Lisa Thompson at Texas A&M University. The compounds, [M(OZCCH3)2(pynp)2]2+ (where M = Moz“, Ruz", Rh”) (30-32), without the solvent molecules, were subjected to density functional theory (DPT) calculations7 with the Becke3 hybrid exchange functional and the Lee-Yang-Parr correlation functional (B3LYP).8 Details of the calculation are contained in Appendix I, which is provided as supporting information. Syntheses Preparation of 2-(2-pyridyl)-1,8-naphthyridine (pynp). The preparation of pynp requires the precursor 2-aminonicotinaldehyde, which must be freshly prepared and used immediately after isolation to avoid self—condensation side reactions. 2-aminonicotinaldehyde. The method of Caluwe and co-workers2 was followed with some modifications. Nicotinamide (9.1 g, 0.07 mmol) was mixed with 13.0 g (0.11 mmol) of ammonium sulfamate in a round-bottomed flask equipped with a condenser. The temperature was slowly increased to 150 °C until the entire solid had melted. At this point the temperature was continuously increased until it reached 200 °C, after which time the reaction was allowed to reflux for 8.5 h. The grayish-white solid obtained from this procedure was washed with copious amounts of water and diethyl ether to remove unreacted nicotinamide and sulfamate. The remaining solid was refluxed in 75 mL of 4N HCl for 6.5 hours and the solution was made basic (pH ~ 9.0) by adding portions of a saturated 198 NaOH solution. The resulting solution was subjected to four extractions with diethyl ether, and the combined extracts were dried over anhydrous MgSOa for one hour. The diethyl ether was evaporated and the remaining light yellow solid was sublimed at 60 °C under vacuum to obtain pure 2-aminonicotinaldehyde; yield, 3.1g (34%). This product must be stored in an inert atmosphere at 0 °C to avoid self-condensation reactions. IR (KBr mull) cm": 3412 (br,w), 2924 (br,w), 2750 (w), 1669 (w), 1624 (w), 1568 (w), 1458 (w), 1402 (w), 1377 (w), 1296 (w), 1273 (w), 1194 (w), 1136 (w), 912 (w), 775 (w), 675 (w), 623 (w). 1H NMR spectrum in CDCl3 at 25 °C: 5 9.82 (s, OH), 8.22 (dd), 7.78 (dd), 6.95 (b), 6.72 (dd) ppm. Preparation of 2-(2-pyridyl)—1,8-naphthyridine (pynp). An amount of freshly prepared 2-aminonicotinaldehyde (1.6 g, 14.8 mmol) was placed in a Schlenk flask under nitrogen and dissolved in 25 mL of freshly distilled ethanol. To this solution was added 1.0 mL of 2-acetyl-pyridine. The solution was refluxed under nitrogen and treated with one drop of a freshly prepared methanolic solution saturated with NaOH. A color change from yellow to a pale brown-yellow immediately ensues. The solution was refluxed overnight under nitrogen and the solution was concentrated to one half of its original volume. White crystals were observed to form after a few hours; yield, 1.1 g (43 %). IR (KBr mull) cm": 1550 (m), 1520 (w), 1470 (s), 1350 (m), 1050 (w), 850 (w), 800 (m), 750 (w). lH NMR spectrum in CD3CN at 25 °C, 5 9.1 (q), 8.75 (m), 8.68 (d,d), 8.45 (d), 8.36 (d,d), 7.95 (t,d), 7.56 (q), 7.48 (m) ppm. [M02(02CCH3)2(PYDP)2][BF412 (30). A sample of [M02(02CCH3)2(CH3CN)6][BF4]2 (0.2 g, 0.27 mmol) was dissolved in 20 mL of CH3CN and treated with 114 mg (55 mmol) of pynp, which leads to a color 199 change from a light pink to a dark green. After 12 h, the solution was concentrated and diethyl ether was added to the point of saturation. The solution was then placed in a refrigerator to yield green platelets; yield, 0.145 g (75 %). IR (KBr mull) cm": 2924 (br, s), 2725(w), 1606(w), 1557(w), 1518(w), 1458(8), 1377(s), 1316(w), 1263(w), 1217(w), 1146(w), 1057(br, s), 854(w), 816(w), 781(w), 721(w), 679(w), 521(w) cm". 1H NMR spectrum in CD3CN at 25 °C: 8 9.05 (d, pynp), 8.85 (dd, pynp), 8.68 (d), 8.2 (td, pynp), 7.72 (m, pynp), 7.66 (m, pynp), 7.52(m, pynp), 2.65(s, CH3-acetate) ppm. Ruz(02CCH3)2(PynP)2][PFslz (31)- The starting material [Ruz(02CCH3)4}Cl (0.150 g, 0.32 mmol) was dissolved in 20 mL of MeOH and treated with 0.131 g (0.64 mmol) of pynp. The initial dark brown solution instantaneously turned to a dark blue color. This solution was stirred overnight and the volume was decreased to ~ 10 mL, after which time diethyl ether was added to produce a dark blue crystalline powder. Yield 0.103 g (60%). IR (Nujol, KBr): 2700 (br,s), 2350 (w), 1450 (s), 1380 (s), 1300 (br,w), 845 (br,s), 780 (br,s), 710 (w), 580 (w). The 1H NMR signals of the product were broad and featureless. [ha(02CCHa)z(pynp)2l[BF412 (32)- A sample of [Rh2(02CCH3)2(CH3CN)6][BE]; (0.1 g, 0.13 mmol) was treated with 0.056 g (0.27 mmol) of pynp in 20 mL of CH3CN which led to an instantaneous color change from pale red to intense red. After stirring overnight, the volume was reduced to 5 mL and the solution was layered with toluene. A crop of red crystals was harvested after three days. Yield 0.077 g (70%). IR (N ujol, KBr): 2926 (br, s), 2725 (w), 1604 (w), 1650 (w), 1523 (w), 1462 (s), 1377 (w), 1315 (w), 1265 (w), 1147 (w), 1059 (w), 1012 (w), 841 (w), 779 (w), 736(w), 715 (w), 559 (w). lH NMR spectrum in CD3CN at 25 °C: 200 8 9.70 (d, pynp). 8.87 (dd, pynp), 8.70 (d, Pynp). 8.60 (m, pynp). 8.45 (dd, pynp), 8.35 (td, pynp), 7.48(q, pynp), 2.25 (s,CH3-acetate) ppm. X-ray data collection and Refinement. Geometric and intensity data for compound (30) were collected on a Rigaku AFC6S diffractometer equipped with a graphite-monochromated Mo K0t (ha = 0.71069 A) radiation source. All calculations were performed with VAX computers on a cluster network using Texsan software package of the Molecular Structure Corporation.9 X-ray structural studies for compounds (31)-(33) were performed on a SMART 1K area detector diffractometer equipped with graphite monochromated Mo K01 radiation (3.01 = 0.71073 A). The frames were integrated in the Siemens SAINT software package,'0 and the data was solved using the direct-methods program S1-IELXS-97.ll Crystal data are listed for compounds (30)-(33) in Table 34. M02(02CCH3)2(PYHP)2][BF412'3CH3CN (30). X-ray quality crystals were obtained within three days from a saturated solution of the title compound in acetonitrile with diethyl ether at -5 °C. A green rectangular crystal of dimensions 0.80 x 0.4 x 0.25 mm3 was covered with silicone grease and mounted on the tip a glass fiber. Cell constants were obtained from a least squares refinement using 25 carefully centered reflections in the range 29<20<37°. Data were collected at —100 i 1 °C, by using the (1) scan method, in the range 45203479 A total of 7493 reflections was collected of which 7200 were unique. The final full-matrix refinement was based on 4162 observed reflections with Fo>40(Fo) that were used to fit 550 parameters to give R1 = 0.0598 and wR2 = 0.1690. The goodness-of-fit index was 0.999 and the highest peak in the final difference map was 1.017 e'lA'3. 201 23: 525 u 23 226 n 2 ~83 u .83 223 u E chad 2am 423 2: N €920 36:2 52.: 52.2 5352 52 :2 5202 E 8.2: N§vOSZSm—m_mcmmmm0 mm 52.: 222 n 23 ES 1 E 88o" 23 826 u E momm one: 23 £0: 4. €8.22 8 68:8 8 €622 620. a @842 648 2.22 9.3100 Zw hmmommmm U NM 4.544.038.4240 - 4.038 n as. . _ 4.: _ ..44 __ .a _ - _ .42 __ a i a. who: 226 u SE 285 n E 23 n 98 a God i E dmvm memo :3 as: m @334 8 842.3 2 €222 €388 68%.: 648 2.32 ~3M00022 mmmmmmmmmv E Co.— 880 n 9:3 9420 u E 825 n 9:3 836 u 2: com: move 39o 946.: 4 52 :4 2 €8.22 2 658.2 622.: 642.2 64.8 8.82 moszonmmmmmmomU cm “:00 A88 :3 80:65 m 8:662: 822: m 30: 012:: 58 :82 A7825 1 m88m Q N <5 4 4 a d <6 <5 <40 anew 000% 3.: 22:8: 802880 .025 8:89:00 8.: San 2:228:0me0 .3 030,—. 202 Ru2(02CCH3)2(PynP)2][PFslz‘Cnson (31) X-ray quality crystals were grown by layering a methanol solution of the title compound with toluene. A blue platelet of dimensions 0.11 x 0.07 x 0.05 mm3 was secured on the tip of a glass fiber with silicone grease and placed in a N 2(g) stream at 173 i l K. A total of 9867 reflections was collected of which 3429 were unique. A disordered [PF6]’ anion required modeling in three different orientations. Final least-square refinement of 242 parameters and 3203 data resulted in residuals of le = 0.0812 and wR2 = 0.1798. The goodness-of-fit index was 1.078 and the highest peak in the final difference map was 0.952 e'/A3. Rh2(OzCCH3)2(pynp)2][BF 412'C7Hs (32) X-ray quality crystals were obtained by slow diffusion of an acetonitrile solution of the title compound into toluene. A red, rectangular crystal of dimensions 0.05 x 0.06 x 0.15 mm3 was covered with silicone grease, secured on the tip a glass fiber, and cooled to 173 i 2 K. A total of 7670 reflections was collected of which 3203 were unique. Final least-squares refinement of 294 parameters and 1840 data resulted in residuals of le = 0.1062and wR2 = 0.2365 and a goodness-of—fit of 1.117. A final difference Fourier map revealed the highest peak to be 0.952 e'lA3. [Rh2(OzCCH3)2(PynP)2(CH3CN)2][BF4][PFal'ZCHsCN (33). Suitable crystals for X-ray crystallography were obtained by slow diffusion of a solution of [Rh2(02CCH3)2(CH3CN)6][BF4]2 in acetonitrile layered over a solution of pynp in dichloromethane. A pale red prism of dimensions 0.15 x 0.05 x 0.1 mm3 was covered with silicone grease, mounted on the tip of a glass fiber and placed in a N2(g) cold stream at 173 i 2 K. A total of 23918 reflections was collected, of which 9970 were 203 unique. Final least-squares refinement of 598 parameters and 5987 reflections resulted in residuals of le = 0.0678 and wR2 = 0.1642 and a goodness-of-fit of 0.980. A final difference Fourier map revealed the highest peak to be 2.209 e'lA3 which is associated with a disordered [PF6]'. III. Results and Discussion. A. A homologous series of redox-active dinuclear compounds. A.1. Synthesis of compounds [M2(02CCH3)2(pynp)]2+, M = [Mo]2+, [Ru]2+, [Rh]2*. Synthesis of compounds [M2(02CCH3)2(pynp)]2*, M = M0“, Ru“, Rh“. Reactions of pynp with [M02(OZCCH3)(CH3CN)6][BF412'°, [Rh2(02CCH3)2(CH3CN)6][BF412", and Ru2(02CCH3)4Cl5 carried out in a 1:2 metal/ligand ratio (Eqs. 13, 14) reactions proceed instantaneously as judged by the color changes that occur within minutes of mixing the reagents. CH CN [M2(0Ac)2(CH3CN)6][BF4]2+2pynp _.3._» [M2(0Ac)2(pynp)2][BF4]2 039-13) M = (a) Moz+, (b) Rh2+ yield: a = 75% b = 70% CH3OH [Ru2(OAc)4]Cl + 2pynp = [R02(OAC)2(PYDP)2][PF6]2 (Bil-14) [n-Bu N][PF] 4 6 yield: 60% The pale violet solution of [Moz(02CCH3)2(CH3CN)6][BF4]2 solution changes to a bright green color, the purple solution of [Rh2(02CCH3)2(CH3CN)6][BF4]2 changes to a pale red color, and finally the brown solution of Ruz((02CCH3)4Cl first changes to a dark purple color and later reverts to dark blue. X-ray and NMR studies (vide infra) revealed that the reactions proceed by displacement of the equatorial acetonitrile ligands in the former two 204 cases and, in the case of the diruthenium chemistry, a loss of two acetate ligands accompanied by a reduction from [Ruz]5+ to [Ru2]‘”. The replacement of the six acetonitrile molecules on [M2(02CCH3)2(CH3CN)6][BF412 10 yield [M2(02CCH3)2(PY"P)2][BF412 (M = Rh, RU) occurs in methanol, ethanol and acetone regardless of the use of different ligand/metal ratios or reaction temperature. In the case of the [M02]4+ complex, however, decomposition occurs at higher temperatures. The synthesis of the dinuclear [Ru2]4+ complex is best performed in alcohols, as reactions preformed in acetonitrile and acetone lead to much lower yields. In the case of the reaction of [Rh2(02CCH3)2(CH3CN)6][BF4]2 with pynp, the side-product [Rh2(02CCH3)2(pynp)2(CH3CN)2][BF4][PF6]°2CH3CN (33) was isolated and characterized by single crystal X-ray methods. A.2. X-ray crystallographic studies. The molecular structures of the dinuclear cations for compounds (30)-(32) are essentially identical, as indicated by X-ray crystallography (Figures 69-72). The compounds consist of a dimetal unit spanned by two cis tridentate pynp ligands, in addition to two bridging acetate ligands. Such a series of compounds is convenient for studying the effect on structure and properties of a non-innocent ligand such pynp in a series of related dinuclear compounds. One interesting aspect to consider is the axial interaction between the metal and the nitrogen donor of the pyridyl unit. The pseudo- axial pyridine interaction is relatively long in all three cases, with M-N distances ranging from 2.204 (4) to 2.439 (8) A and M-M-Nax angles in the range 159.01[2] to l69.6(3)°. Compound [Moz(02CCI-13)z(pynp)2][BF4]2-3CH3CN (30) exhibits the longest axial M-N distance of 2.439 [8]A as expected for a [M02]4+ quadruply-bonded complex.12 In the 205 case of [Ru2(02CCH3)2(pynp)2][PF6]2.2CH3OH (31) complex, the axial interaction is of an intermediate value, Ru(l)-N(3)A 2.237(7)A, which is consistent with the fact that this species is a doubly-bonded compound. Finally, [Rh2(02CCH3)2(pynp)2][BF4]2.C7H3 (32) exhibits the shortest axial interaction, 2.204 (4) A (Rh(l)-N(3), as expected for the compound with the weakest M-M bond trans-influence.l2 The strength of the axial interation is closely tied to the M-M distance, as well illustrated by this series of compounds. The quadruply-bonded compound [M02(OZCCH3)2(pynp)2][BF4]2-3CH3CN (30) exhibits a M-M bond distance of 2.124(1) A, whereas the reported M-M distance for the parent molecule Moz(OzCCH3)4 is 2.0934(8) A.” The lengthening of the metal-metal bond by 0.03 A is attributed primarily to the axial interaction. The [Ruzl‘H derivative in this series [Ru2(02CCH3)2(pynp)2][PF6]2.2CH3OH (31) exhibits a Ru-Ru distance of 2.298 (1)A, which is slightly longer than the corresponding distances in [Ruz(02CCH3)4(THF)2] and [Ru2(02CCI-I3)4(H20)2] which are 2.261(3) and 2.265(3)A, respectively." This lengthening can be attributed to the fact that the pyridyl ring is a better axial donor than THF or H20. Finally, in [Rh2(02CCH3)2(pynp)2][BF4]2.C7I-Ig (32) the Rh-Rh distance is 2.408 (2)A which is well within the expected values for a Rh-Rh single bond.'7 This distance is 0.04 A longer than the corresponding distance in Rh2(02CC3H7)4,'5 which is the only dirhodium tetra-carboxylate compound without axial coordination to be structurally characterized. The lengthening of the M-M bond is due to the donation of the pyridyl moiety into the 0* antibonding orbital of the [Rh2]4+ unit. The M—Neq interactions with the naphthyridine bridges are considerably shorter than the M-Nax interactions by comparison, and they decrease as the radius of the metal 206 ion decreases. Since Moll possesses the largest radius, the M-N distances are the longest with the averages being 2.211[8] A followed by Ru" with 20725] A and finally Rh" with 2.018 [41A Table 35. bond distances (A) (°) for [M02(02CCH3)2(P)’“P)2][BF4]2°3CH3CN (30)- MOI-03 2.088(6) M02-02 2.092(6) M01 -01 2.1 14(6) M02-04 2.150(6) Mol-M02 2.124(1) M02-N2 2.165(8) Mol-N6 2.184(8) M02-N5 2.245(7) Mol-Nl 2.251(7) M02-N4 2.450(8) Mol-N3 2.429(8) O3-Mol-Ol 88.4(2) 02-M02-N2 88.5(3) O3-Mol-Mo2 93.5(2) Mol-Mo2-N2 94.7(2) Ol-Mol-M02 89.66(17) 04-M02-N2 174.9(3) O3-Mol-N6 88.1(3) 02-M02-N5 175.9(3) Ol-Mol-N6 174.3(3) Mol-M02-N5 90.7(2) MoZ-Mol-N6 95.1(2) 04-M02-N5 91.2(3) O3-Mol-Nl 174.7(3) N2-M02-N5 92.0(3) Ol-Mol-Nl 87.6(3) 02-M62-N4 106.6(3) MoZ-Mol-Nl 90.1(2) Mo-MoZ-N4 158.7(2) N6-Mol-Nl 95.5(3) O4-M02-N4 84.1(3) O3-Mol-N3 106.1(3) N2-M02-N4 93.4(3) Ol-Mol-N3 84.3(3) N5-Mo2-N4 69.3(3) MoZ-Mol-N3 159.3309) Cl-Ol-Mol 119.8(6) N6-Mol-N3 92.2(3) C1-02-M02 116.8(5) N1-Mol-N3 69.9(3) C2-03-Mol 116.5(6) 02-M02-Mol 93.33(18) C2-O4-M02 118.7(6) 02-M02-04 88.0(2) C4-N1-Mol 121.6(6) Mol-M02-O4 89.20(l9) C8-Nl-Mol 119.9(6) 207 /\—\ C) C17 Figure 69. Thermal ellipsoid plot at the 50% level of the cation in [M02(02CCH3)2(pynp)2][BF4]2-CH3CN (30). Hydrogens have been omitted for the sake of clarity. 208 Table 36. Selected bond distances (A) and angles (°) for [Ruz(02CCH3)2(PYnP)2][PF612-2CH3OH (31)- Rul-Rul 2.298(1) Rul-Nl 2.071(5) Ru1-02 2.054(5) Rul-Ol 2.089(5) Rul—N2 2.072(5) Rul-N3 2.237(7) OZ-Rul-NZ 90.2(2) Ol-Rul-N3 87.6(2) OZ-Rul-N 1 176.7(2) OZ-Rul-Rul 91.22(l4) N2-Rul-Nl 93.0(2) N 2-Ru1-Rul 91. 16(15) N2-Rul-Ol 175.6(2) Nl-Rul-Rul 89.4405) Nl-Rul-Ol 90.9(2) Ol-Rul-Rul 86.91(l4) N2-Rul-N3 95.3(2) N3-Rul-Rul 163.7(2) As noted earlier, in addition to the [ha]4+ dinuclear complex with two tridentate pynp units, a by-product was isolated, namely [Rh2(02CCH3)2(pynp)2(CH3CN)2][BFa][PF6]-2CH3CN (33). This compound co- crystallizes as a side product from the reaction that produces [Rh2(02CCH3)2(pynp)2][BF4]2. In this compound, the dirhodium unit possess one pynp ligand coordinated in the tridentate fashion and a second pynp ligand that acts as a monodentate ligand to an axial position through one of the N atoms of the naphthyridine unit (Figure 72). The pseudo-axial distance (Rh(l)-N(4)) between the nl-pynp ligand and the metal center is 2.158 (5) A, which is 0.16 A larger than the Rh-pyridyl interaction Rh(2)-N(3) 1.997 (5) A. The weaker RheN interaction is presumably due to the weaker donor character of the naphthyridine nitrogen atom compared to the pyridine nitrogen unit. 209 / C9A ‘1 ‘3'") %va3 C4 C8 C1 1A s . \ ~0,,'fl§ //, ClOA @I‘ Figure 70. Thermal ellipsoid plot of the cation in [Ruz(OzCCH3)2(pynp)2][PF6]2-CH30H (31) at the 50% probability level. Hydrogen atoms have been omitted for the sake clarity. 210 Table 37. Selected bond distances (A) angles (°) for [Rh2(02CCH3)2(PY"P)2] [BF412-C7H8 (32)- Rh l-Rhl 2.4075( 18) Rh 1 -N1 2.045(12) Rhl—N2 1.985(12) Rhl-Ol 2.051(11) Rh 1-02 2.036(11) Rh 1 -N3 2.204(11) N2-Rh1-02 90.2(5) OZ-Rh 1 -N 3 90.4(4) N2-Rh1-N 1 92.0(5) N 1 -Rh1-N3 95.6(4) OZ-Rh 1-N1 173.8(4) Ol-Rhl—N3 101.7(4) N2-Rh1-Ol 178.7(4) N2-Rh1-Rhl 91 . 1(3) OZ-Rh l -01 88.6(4) OZ-Rh l-Rhl 86.9(2) N 1-Rh- Ol 89.2(4) N 1 -Rh1-Rh1 87.3(3) N2-Rh1-N3 78.9(4) O 1—Rh1-Rhl 88.3(2) Table 38. Selected bond distances (A) angles (°) for [Rh2(02CCH3)2(P)’“P)2(CH3CN )2HBF4IP F61'2CH3CN (33)- Rh 1 -N 8 2.034(6) Rh 1 -N4 2.158(5) Rh 1 -01 2.084(5) Rh 1-03 2.176(5) Rh 1 -N1 2.134(6) Rh2-N3 1.997(5) N8-Rh1-Ol l78.02(17) N1-Rh1-O3 174.15(17) N8-Rh1-N1 95.6(2) N4-Rh 1-03 94.77(l9) Ol-Rh 1 -N1 85.1(2) N8-Rh1-Rh2 93.27(14) N8-Rh 1 -N4 95.5(2) Ol-Rh 1-Rh2 88.46(12) Ol-Rh 1 -N4 82.67(19) ‘ N1-Rh1-Rh2 97.86(l4) N1-Rh1-N4 90.9(2) N4-Rh l -Rh2 l66.96(15) N8-Rh1-O3 85.3(2) O3-Rh1-Rh2 76.30(1 l) Ol-Rhl-O3 94.23(18) 211 ”\ C9A .~ \I} "A “$1., C6A\‘ C5A \ \\\\1 V Figure 71. Thermal ellipsoid plot of the cation in [Rh2(02CCH3)2(pynp)2][BF4]2-C7Hg (32) at the 50% probability level. Hydrogen atoms have been omitted for the sake of clarity. 212 Figure Thermal ellipsoid plot of the cation in [Rh2(02CCH3)2(PY“P)2(CH3CN)2][BF4HPF612'2CH3CN (32) at the 50% probability level. Hydrogen atoms have been omitted for the sake of clarity. 213 A.3. Theoretical calculations. To gain insight into the electronic structure of the series [M2(02CCH3)2(pynp)2]2+ (compounds (30), (31), and (32)), single point energy calculations were performed by Dr. Lisa Thompson at Texas A&M University for the dication, neutral and dianion of these complexes at the B3LYP level of theory. An orbital analysis of the calculated orbital occupancy for the dication of [Moz(02CCH3)2(pynp)2]2+, [Ruz(02CCH3)2(pynp)2]2+, and [Rh2(OzCCH3)2(pynp)2]2+, showed the expected metal orbital occupancy of 021:452, ozn4825*21t*'n*', and 027t4525*2n*4 respectively. Details of the findings as they pertain to the experimental findings in this chapter are found in Appendix I. Only a summary of how the results of the calculations support the spectroscopic and electrochemical results is included in the relevant sections. A.4. UV-Visible and N MR spectroscopic studies. Table 39. UV-Visible data for compounds (30)-(32) Am 6 nm L-(mol-cm)’l [M02(02CCH3)2(P)’DP)2[BF4]2 (30) 432 1.8 x 103 1 857 4.8 x 102 [RU2(02CCH3)2(P)’"P)2[PF6]2 (31) 327 3.4 x 104 671 3.6 x 10‘ 278 3.1 x 10‘ [Rh2(02CCH3)2(P)’"P)2[BF4]2 (32) 355 8.7 X 103 451 2.4 x 103 214 The electronic spectra for the three compounds in the series [M2(02CCH3)2(pynp)2][BF4]2 were recorded in acetonitrile in the range 800-200 nm (Table 6). The spectrum for [M02(02CCH3)2(pynp)2][BF4]2 (30) exhibits an electronic transition in the visible range at 432 nm which is a characteristic energy for a 8—55“ '6'” but the evalue is transition for a quadruply-bonded Moz'"ll complex uncharacteristically high at 1.8 x 103 L-M'Icm'l an order of magnitude greater than the typical values, suggesting the involvement of ligand character. The dinuclear [Ruz]“ complex (31) exhibits two electronic transitions located at 327 nm (e = 3.4 x 104 L-M' lcm") and 671 nm (8: 3.6 x 104 L'M'lcm"). The dirhodium compound [Rh2(OZCCH3)2(pynp)2]2+ (32) displays three transitions located at 278, 355 and 451 nm with e values of 3.1 x 10“, 8.7 x 103 and 2.4 x 103 L-M"cm" respectively. The aforementioned electronic spectral data indicate that the new compounds exhibit very different electronic properties than the parent tetracarboxylate species. Electronic transitions for [Moz(02CCH3)4 are located at 435 nm (8 == 102 L-M"cm"), '7 for Rh2(02CCH3)4]L2 at A = 552 nm (e z 2 x 102 L-M"cm") and it = 437 nm (e z 1 x 102 L-rvr"cm"),'8 and finally for Ru2""'(ozccri3). at 2...... = 448 nm (e = 6 x 102 L-M"crn' l).l2 Clearly the presence of the two pynp ligands has perturbed the electronic structure of the HOMOand/or LUMO levels, a possibility that was probed by theoretical calculations (Appendix I). 1H NMR Spectroscopy. 1H NMR spectroscopic studies of the two diamagnetic compounds [M02(02CCH3)2(PYHP)2][BF412 (30) and [Rh2(02CCH3)2(pYnP)2][BF412 (32) in CD3CN support the existence of the intact cations [Moz(02CCH3)2(pynp)2]2+ and 215 [Rh2(02CCH3)2(pynp)2]2+ in solution. The IH NMR spectrum for [Moz(02CCH3)2(pynp)2][BF4]2 displays an upfield singlet at 5 = 2.65 ppm for the acetate CH3 groups and seven resonances between 5 = 7.5-9.0 ppm for the aromatic pynp protons. The [ha]4+ complex (32) exhibits a similar pattern, with an upfield singlet located at 5 = 2.25 ppm and aromatic resonances in the range 7.5-9.7 ppm. The presence of only one acetate environment in each case and the 1:1 integration of acetatezpynp ligands is in accord with the solid-state structure. A.5. Cyclic voltammetric studies. Electrochemical studies of Compounds (30)-(32) were performed by the cyclic voltammetry technique in acetonitrile solutions (Figure 73). The cyclic voltammogram of [Moz(02CCH3)2(CH3CN)6][BF4]2-3CH3CN (30) exhibits four reversible reduction couples located at Em“) = -0.43v, Em”) = -O.67 v, Em”) = -1.34v and Bug“) = -1.66V (Figure 6). In addition, an irreversible oxidation occurs at 13,,a = 0.86V. The most salient point about these data is that the second reduction occurs at a potential that is 240 mV more negative than the first couple. This corresponds to a comproportionation constant, 4 Kc, for this reaction of 1.2 x10 (scheme 5), which was class H behavior according to the Robin-Day classification.l9 Likewise the second set of one—electron reductions are coupled as judged by the fact that the fourth one-electron reduction occurs at a potential that is 320 mV higher than the third reduction process (Kc value of 2.70 x 105) (Scheme 5). These comproportionation constants are in the range of what has been observed for weakly coupled systems. The compound [Ruz(02CCH3)2(pynp)2][PF6]2 (31) also exhibits four reversible one-electron ligand based reductions; these are located at Em“) = -0.43 V, Buzz) = -0.82 216 V, 131/2‘3) = -1.40 V and E172“) = -1.84 V (Figure 73). The second reduction is shifted to a more negative potential by 390 mV relative to the first one. This separation corresponds to a comproportionation constant of Kc = 3.9 x 106, an indication that the unpaired electron is delocalized over the two pynp units (Class III, Robin-Day behavior).'9 Analogous] y the third and fourth reductions occur at a separation of 420 mV, which leads to a calculated Kc value of 2.7 x 107. This also corresponds to class III behavior (Scheme 5). In addition, the compound displays a reversible couple at Em = 0.85V which corresponds to the oxidation from [Ruzm to [Ruz]5+. +e- [M2(02CCH3)2(pynp)2]2+ _ _ [M2(02CCH3)2(PY“P)2]+ Emy, M = a) Mo, Kc(a) = 1.2 x 10‘ b) Ru Kc(b) = 3.9 x 10" [M2(02CCH3)2(P)’"P)2]+ 4: : [M2(02CCH3)2(PYHP)2] Emr/2 + - - [M2(02CCH3)2(pynp)zl _ : [M2(02CCH3)2(pynp)2] Early: Kc(a) = 2.7 x 105 Kc(b) = 2.7 x 107 [M2(02CCH3)2(PY“P)2]' + :- [M2(02CCH3)2(PY“P)2]2° E(4)y2 Scheme 5 In contrast to the previous two cases, [Rh2(02CCH3)2(pynp)2]2+(3l) exhibits only two reduction features in the cyclic voltammogram; these are located at Em“) = -0.78 V and Ema) = -1.42 V (Figure 6c). The first reduction process is associated with a two- 217 —. En) | [Rh2(0AC)2(pynp)2][BF4]2 I E(4) I [M02(0Ac)2(pynp)2][BF4]2 I I [R92(0AC)2(PYDP)2][PF6]2 I AEy2=420 mV Kc: 2.7 x 107 AEy2= 390 mV Kc =39 x 106 I l 7 1 l I t l l I I’ o 0.5 -1 -1 5 -2 -2.5 E (V) Figure 73. Cyclic voltammograms for compounds (30)-(32) in acetonitrile with 0.1 M [n-BuaN][PF6] at a Pt disk electrode versus Ag/AgCl. 218 electron process whereas the latter one is a one-electron process as determined by coulometry and differential pulse voltammetry (Figure 74). A homologous series such as the present one is an ideal situation for making comparisons based on the differences in metal frontier orbitals. The cyclic voltammetry results for the M02(II,II) and Ruz(II,II) complexes indicate stable mixed-valence intermediates of the type [M2(02CCH3)2(pynp)2]+ and [M2(02CCH3)2(pynP)2]'. whereas for the Rh2(II,II) complex, the mixed valence states are not stable. In order to understand this situation, theoretical calculations were performed (Appendix I), and the results indicated that the dirhodium compound is undergoing decomposition as the LUMO is becoming populated during the reduction processes. In the case of the stable reduced forms of Moz(II,II) and Ru2(H,II), however, the calculations reveal that the ratios of the changes in energy between orbitals before and after reduction are in excellent agreement with the observed differences in potential between the two sets of reductions (neutral/2e reduction and 2e' reduction/4e reduction). 2.5 x 10 -6 T I I I I j I I I I I fi I I I I I T I q l- -1 2.0x 10-6 i A r: O O t o g : -6 L g E _‘ 1.5 X 10 1' g o 4 C o ‘8 Z r- O - 1.0 x 10 '6 :- § ‘1 . . 5.0x 10 '7 " 1 0.“) 1 l 1 1 1 J 1 4 1 l 1 1 1 J : -0.4 -0.6 -O.8 -1 -1.2 Figure 74. Diferential pulse voltammogram of [Rh2(02CCH3)2(pynp)2][BF4]2 in 0.1 M TBAPF5 acetonitrile at a Pt disk electrode versus Ag/AgCl. 219 A 6. Magnetic studies. In this series, only [Ruz(02CCH3)2(pynp)2][PF6]2 (31) is paramagnetic. According to previous studies on various [Ruz]4+ compounds, the ground state spin value is S = 1.20 In order to understand the magnetic behavior of these compounds, it is necessary to understand that a large zero-field splitting is expected due to spin-orbit coupling.24b The actual data for [Ruz(02CCH3)2(pynp)2][PF6]2 confirms this prediction. Figure 75 presents 0.007 IIIIITIIIIIIIIIIIII‘IIITIIIIII1.2 0.0065 0.006 . N 9 f . u-a O _ .. ’8 E ' {3’ 0.8 a (2 0.0055 _ .1 . 2 0 I D = 296 cm : O 2 0.005 _- TIP = 350 x 10‘6 emu: 0-6 a : _3 E Q _ = ‘22“: 0.0045 _- P 3 "10 5 ' " 0.4 2. 0.004 : " 0.2 0.0035 0.003 1 1 l 1 1 1 1 l 1 1 1 1 I 1 1 1 1 l 1 1_1 1 l O 100 150 200 250 300 T (K) Figure 75. Plot of xT versus T (red) and x versus T (blue) for [Ruz(02CCH3)2(pynp)2][PF6]2 at an applied field of 1000 G. the data in two different ways, namely as x vs T and xT vs T plots. The plot of xT versus T shows a constant decrease as the temperature decrease due to the zero field splitting present in this compound. The plot of x versus T displays an increase in susceptibility 220 below 30 K that can be attributed to a small amount of paramagnetic impurity (probably the oxidized Ru(H)-Ru(III) species) which must be taken into account for modeling the magnetic behavior of compound [RU2(02CCH3)2(P)’nP)2][PF6]2. In order to fit this experimental data to a theoretical expression of the magnetic susceptibility for an anisotropic S = 1 system, which accounts for the small paramagnetic impurity and the Tip observed, the equation 14 was used. it = (ZNgM21.1132/3161‘){[e’x + (2/x)(1 — e"‘)]/( 1 + 2e"‘)} + Tip + P/T (Eq. 14) In equation 14 x = D/KT accounts for the zero field splitting and gM was assigned a value of 2, these assignments were based on previous studies done in [Ruz]+4 systems.24 111. Conclusions Extensive research over the past forty years has been carried out on the tetracarboxylate family of compounds of general formula M2(02CCH3)4 (M: Mo“, Ru“, Rh“).l7 Although these compounds are useful starting materials for a variety of M-M bonded derivatives, they do not exhibit extensive redox chemistry or unusual electronic properties. In sharp contrast, the new compounds in this study that contain two pyridyl naphthyridine ligands pynp in addition to two acetate ligands display vastly different behavior. In particular, [Moz(OzCCH3)2(pynp)2][BF4]2'3CH3CN (30) and [Ruz(02CCH3)2(pynp)2][PF6]2-CH30H (31) exhibit four, reversible one-electron reduction processes. In the case of the [M02]4+ compound (30) the four reductions indicate Class II behavior based on the Robin and Day scale.'9 For the [Rug]4+ compound, the potentials of the four, one-electron reduction couples signify Class III behavior, namely a fully delocalized system. 221 Density functional theoretical calculations (Appendix I) lend supporting evidence for the correlation between the degree of mixing of the metal-based orbitals with the ligand orbtials and the degree of delocalization of the electrons upon reduction. The Ruz(II,II) complex exhibits the highest degree of mixing, thus the larger comproportionation constants are observed. The capability of pynp to coordinate as either a tridentate or bidentate ligand had earlier been suggested, but not substantiated with X-ray evidence. This work presents the first well—characterized example of the monodentate coordination mode for the pynp ligand, which is a likely intermediate in the eventual stabilization of the tridentate form. 222 IV. References I. (a) Caluwe, P.; Evens, G. Macromolecules 1979, 12, 803. (b) Tikkanen, W.; Binamira-Soriaga, B.; Kaska, W.; Ford, P. Inorg. Chem, 1984, 23, 141. (c) Tikkanen, W.; Binamira-Soriaga, E.; Kaska, W.; Ford, P. Inorg. Chem, 1983, 22, 1147. (d) Thummel, R. P.; Lefoulon, F.; Williamson, D.; Chavan, M. Inorg. Chem, 1986, 25, 1675. (e) Binamira-Soriaga, E.; Keder, N. L.; Kaska, W. C.; McLoughlin, M. A.; Keder, N. L; Harrison, W. T. A.; Stucky, G. D. Inorg. Chem, 1990, 29, 2238. 2. (a) Majewicz, T. C; Caluwe, P. J. Org. Chem, 1974, 39, 720. (b) Caluwe, P.; Evens, G. Macromolecules, 1979, 12, 803. 3. Pimblett, G.; Garner, C. D.; Clegg, W. J. Chem. Soc., Dalton Trans, 1986, 1257. 4. Cotton, F. A.; Reid, A. H.; Schwotzer, W. Inorg. Chem, 1985, 24, 3965. 5. Martin, D. S.; Newman, R. A.; Vlasnik, I. M. Inorg. Chem, 1980, 19, 3404. 6. Boudreaux, E. A.; Mulay, L. N., Eds Theory and Applications of Molecular Paramagnetism. John Wiley & Sons: New-York, 1976. 7. Parr, R. G.; Yang, W. Density-functional theory of atoms and molecules Oxford University Press, Oxford, 1989. 8. (a) Becke, A. D J. Chem. Phys. 1993, 98, 5648. (b) Lee, C.; Yang, W.; Parr, R. G. Phys. Rev. 3., 1998, 37, 785. 9. TEXSAN-TEXRAY Structure Analysis Package; Molecular Structure Corporation: The Woodlands, TX 1985. 10. SAINT, Program for area detector absorption correction, Siemens Analytical X-Ray Instruments Inc., Madison WI 53719, USA 1994-1996. 11. SHELXL-97 - g.m. Sheldrick, SHELXL — 97, Program for refining crystal structures, University of Gottingen, 1997. 223 IA AAAAA’AIA’J" 'll I'll! 1‘ 12. Cotton, F. A.; Walton, A. R. Multiple Bonds Between Metal Atoms. Second ed., 1993 and references therein. 13. Cotton, F. A; Mester, Z. C.; Webb, T. R.; Acta Crystallogr., 1974, B30, 2768. 14. Lindsay, A. J.; Tooze, R. P.; Motevall, M.; Hursthousean, M. B.; Wilkinson, G. J. Chem. Soc. Commun., 1984, 1383. 15. Cotton, F. A.; Shiu, K. B.; Rev. Chim. Mine’rale, 1986, 23, I4. 16. Trogler, W. C.; Gray, H. B.; Acc. Chem. Res., 1978, II, 232. 17. Trogler, W. C.; Solomon E. 1.; Trajberg, I. B.; Ballhausen, C. J.; Gray, H. B. Inorg. Chem, 1977, 16, 828. 18. Johnson, 8. A.; Hunt, H. R.; Neumann, H. M.; Inorg. Chem, 1963, 2, 960. 19. Robin, M. B.; Day, P. Adv. Inorg. Chem. Radiochem., 1967, 10, 247. 20. (a) Cotton, F. A.; Miskowski, V. M.; Zhong, B.; J. Am. Chem. Soc., 1989, III, 6177. (b) Cogne, A.; Belorizky, B.; Laugier, J.; Rey, P. Inorg. Chem, 1994, 33, 3364. (c) Lindsay, A. J.; Wilkinson, G.; Motevalli, M.; Hursthouse, M. B. J. Chem. Soc. Dalton Trans., 1987, 2723. 224 APPENDIX I Density Functional Calculations on LIST COMPOUNDS. In order to gain insight into the electronic structure of the compounds [M2(OZCCH3)2(pynp)2]2+, single point energy calculations were performed at the B3LYP level of theory for the dication, neutral and dianion versions of all three complexes. In the case of the Ru(II) analog, calculations were also performed on the monocation and monoanion species. Analyses of the calculated orbital occupancies for the dications [M02(02CCH3)2(PYNP)2]2+. [Rh2(02CCH3)2(pynp)2]2+. and [RU2(02CCH3)2(Pynp)2]2+ supports the electronic configurations of 021952, ozn4526*21t*2, and 021:4525*27t*4 respectively. Correlation with electronic transitions The calculated energy differences between the highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) levels for each of the three new compounds from DFT (vide infra) calculations are in good to reasonable agreement with the aforementioned experimental data. In all cases, the lowest energy transition is one that involves little to significant metal-to-ligand charge transfer (MLCT), which is in accord with the higher 8 values than those reported for similar metal-metal bonded compounds. The calculated energy difference of the LUMO and the HOMO of the dication for complexes (30), (31), and (32), corresponds to the lowest energy transitions found in the UV-visible spectra for these species (Figure 76). In the case of [M02(OzCCH3)2(pynp)2]2+ (30), the lowest energy transition is a 8 —> 6* transition, with a calculated (ELUMO'EHOMO) energy gap of 33.6 kcal/mol as compared to the experimental value of 33.3 kcal/mol. The extinction coefficient for this transition (e = 4.75 x 102 LM' 225 Icm") is an order of magnitude greater than those typically found for a pure 5 —-> 8* transition. The calculation indicates that the ligand character of the LUMO involved in the first electronic transition of [M02(OZCCH3)2(pynp)2]2+ is much greater than the ligand character of the HOMO (Table 40). From these results, it is possible to conclude that the lowest energy transition involves a metal-to-ligand charge transfer (MLCT), which are much more intense than pure d-d transitions. The lowest energy transition for [Rh2(OzCCH3)2(pynp)2]2+ was calculated to be a transition from a metal-based 7t* orbital to a ligand-based 11* orbital (Mn. -> Ln.) with a value of 63.9 kcal/mol. This is in good agreement with the experimental value of 63.4 kcal/mol (Figure 76). The e value is 2.4 X 103 LM'l cm‘1 which is an order of magnitude larger than the e value for the first transition of [M02(02CCH3)2(pynp)2]2+. This finding is consistent with an increase in MLCT character for [Rh2(OzCCH3)2(pynp)2]2+ as compared to [Mo;g(02CCH3)2(pynp)2]2+ (Table 40). Finally, the lowest energy transition for [Ruz(OzCCH3)2(pynp)2]2+ was also calculated to be a M“. —) Ln. transition (MLCT) with an energy of 59.3 kcal/mol. The experimental value is 42.6 kcal/mol, which is in reasonable agreement with the calculations (Figure 76). The MLCT character for Ruzz“ is calculated to be slightly smaller than for Rh22+ which is consistent with the slightly smaller extinction coefficient for Ru;2+ (e = 3.1 X 104 LM" cm") compared to Rh;2+ (e = 3.1 X 104 LM'l cm'l). An overestimation of the excitation energy is not entirely unexpected for this type of estimation, as the correlation energy at the excited electron is not used, but it is somewhat surprising given the close agreement of the calculated and experimental results for the other two compounds. Obviously, solvation of [Ruz(OZCCH3)2(pynp)2]2+ could lead to subtle geometry changes, which affects the 226 validity of comparing calculations performed on parameters taken from the solid-state structure with electronic spectra] measurements measured in solution. One other point that should be emphasized is that the dication of [Ruz(OZCCH3)2(pynp)2]2+ is an unrestricted open-shell calculation with two unpaired electrons (S = l with the alpha and beta orbitals optimized independently), whereas [Moz(OzCCH3)2(pynp)2]2+ and [Rh2(OzCCH3)2(pynp)2]2+ were both closed shell calculations (3 = 0). Correlation with Electrochemistry. DFT single point energy calculations on the X-ray crystal structure of the dications were performed for three different oxidation states of the Mo and Rh compounds. namely [MostozccmlztpynphlW“. [RhstosCCHslztpynplzl"*m°’ and five different oxidation states of the Ru(H) compound [Ru2(02CCH3)2(pynp)2](2m”0"'0‘). These calculations were analyzed and compared to the electrochemical potentials for the reduction of the three parent compounds [M2(OZCCH3)2(pynp)2]2+. An open-shell calculation was unavoidable for [Ruz(OzCCH3)2(pynp)2]2+ (31), because the ground state was determined experimentally to be a triplet (S = 1), therefore, 1e' and 2e' reductions were calculated. A single point energy calculation was performed on both the singlet (S = 0) and triplet (S = l) for (32), and the triplet was found to be 35.4 kcal/mol lower in energy, in agreement with the magnetic measurements. For compounds lM02(02CCH3)2(P>'H1))2]2+ (30) and [Rh2(02CCH3)2(Pynphl2+ (32). 29' reductions were simulated instead of le' reductions to decrease the difficulty of the computations. The 2e" reductions produce compounds with all electrons spin-paired (S = 0), while le’ reductions would produce open-shell (S = 1/2) species for (30) and (32), which are harder to compute than the closed-shell species (8:0). 227 To correlate the calculated energetics with the observed electrochemistry the change in the AE(LUMO — HOMO) (energy difference between the HOMO and LUMO) of the unreduced species and the AE(HOMO — HOMO-1) of the reduced species was originally calculated with the expectation that the larger the calculated change the larger the splitting in the le' reduction potentials. It was found that the absolute change in orbital energy differences did not correlate due to the lack of solvation of the charge in the gas phase calculations. In an attempt to compensate for the effect that the change in charge has on the orbital energetics, the difference in the change in the frontier orbital energies was normalized to the average value of the change in the respective orbital energies. For example, the normalized change in orbital energy (NCOE) for the 2e" reduction of [Moz(OzCCH3)2(pynp)2]2+ is shown in equation 15. (E hbmo - EIZIJMO )" (EPOMO-l - E00140) l 2((E1210M0 _ E80140 )+ (Echomo-l - E(PIOMO » (Eq. 15) According to this approach, the calculated NCOE values should be proportional to the splitting of the le' reduction potentials in the cyclic voltammetry for this series of compounds. The relevant orbital energies, differences and NCOE values for compound (31) are listed in Table 41. As mentioned previously, [Ru2(OZCCH3)2(pynp)2]2+ (31) is paramagnetic with two unpaired electrons (8:1), unlike the [M044] (30) and [Rh‘“] (32) derivatives. Since the ground state of the [Ru“] complex is an open-shell calculation, the four 1e' reductions in this series were calculated, as apposed to only calculating two 2e' reductions. The NCOE for the le' reduction of the dication of (31) was calculated to be 0.45, which indicates a fairly large splitting of the 1e“ process (0e'/ 1e" to 1e'/2e' reduction potentials). The NCOE for the le' reduction of the neutral species was calculated to be 228 0.66, indicating a larger splitting of the second le' process (2e'/3e' to 3e'/4e' reduction potentials). The cyclic voltammogram for (31) exhibits four 1e' reductions with separations of AB“; = 390mV (le'l2e') and AB“; = 420mV (3e'/4e'), which is consistent with the calculated larger splitting of the second Ie' process. To determine if the modeling of 2e' reductions would produce the same trend found when modeling the le' reductions, the NCOE values for the 2e' reduction of the dication and neutral species of (31) were calculated. The NCOE value for the 2e’ reduction of the dication was calculated to be 0.70, and the NCOE value for the 2e' reduction of the neutral species was calculated to be 0.88, which also indicates that the splitting of the second 1e' process should be larger than the first. Therefore, modeling the le’ process with a 2e' reduction should also give a qualitative description of the splitting of the two 1e' reduction potentials. The orbital energies, differences and NCOE for compounds (30) and (32) are listed in Table 42. For the dinuclear complex (30), the NCOE for the first 2e' reduction is 0.59, and for the second 2e' reduction, the NCOE is 0.73. The cyclic voltammogram for [M02(OZCCH3)2(pynp)2][BF4]2 also exhibits four le' reductions with separations of AEm = 240mV (1e'/2e') and ARI/2 = 320mV (3e'/4e'). The NCOE for the second 2e' reduction is larger than for the first 2e' reduction, in agreement with the experimental results, which has a larger splitting of the second le' process. The calculated NCOE values for both of the le' processes of (30) are smaller than the corresponding NCOE calculated using the 2e' reduction method for (31), a result that is also in agreement with the smaller splitting found in the cyclic voltammetry of (30). 229 For the complex [Rh2(OzCCH3)2(pynp)2]2+ (32), the NCOE for the first 2e' reduction is 0.16, and for the second 2e' reduction is 1.77. As previously mentioned, the cyclic voltammogram for the [Rh2(OzCCH3)2(pynp)2]2+ complex (32) is very distinct from its [M02]4+ (30) and [Ruz]4+ (31) counterparts. The calculated NCOE value for the 2e' reduction of [Rh2(OzCCH3)2(pynp)2][BF4]2 (32) is much smaller than the NCOE values calculated for (30) or (32); which is consistent with the fact that the first two le’ reductions occur at nearly the same potential; this is entirely consistent with the electrochemical data. The NCOE value of 1.77 calculated for the second le' process (3e' /4e') for (32) indicates that the splitting of the le' reduction potentials should be extremely large (Table 42). A differential pulse voltammetry (DPV) experiment performed on [Rh2(OzCCH3)2(pynp)2][BF4]2 revealed that the first reversible process is a 2e' reduction, whereas the second quasi-reversible couple is only a 1e' reduction (Figure 73) in agreement with the calculated NCOE value. The orbital occupation for the neutral species of the [Rh2]4+ dinuclear complex (32) is ozn4526*21t*4L(n'2) and the LUMO is an anti-bonding interaction of the metal-5* with a ligand-11* orbital. Based on the fact that the electrochemical processes for this complex is quasi-reversible and that the second reduction is only a le' reduction, it appears that the neutral species Rh2(OzCCH3)2(pynp)2 begins to decompose upon occupation of the anti-bonding LUMO. Overall, the calculated NCOE values, as calculated by the 2e’ reduction method, for complexes, (30), (31), and (32), are in qualitative agreement with the experimentally determined splitting of the le’ reduction potentials, shown in the cyclic voltmmograms. 230 Table 40. Ratio of Metal to Ligand (MIL) and Ligand to Metal (UM) character of the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO) as calculated at the B3LYP level of theory for the dication [M2(02CCH3)2(pynp)2]2+ (M = Mo“, Ru2+ and ha“) of (30), (31), and (32). HOMO LUMO HOMO LUMO MIL M/L IJM L/M Mo(+2) 1.63 0.36 0.61 2.74 Ru(+2)al 1.53 0.01 0.65 9.87 Rh(+2) 1.33 0.09 0.75 11.5 a HOMO and LUMO for the alpha molecular orbitals. 231 Table 41. Orbital Energies (hartrees) and Ratios for Important Molecular Orbitals in singlet (S = 0) dinuclear complex Mo(II) (30) and dinuclear complex Rh(II) (32), dication, neutral and dianion species. c1 c2 c3 Alaa AB” NCOE NCOE M2(+2) HOMO LUMO LUMO+1 AE. AE3 M2(O) HOMO-1 HOMO LUMO AE3 AB, A.; M2(-2) HOMO-2 HOMO-1 HOMO A85 AE6 A4,, M02(+2) 0.3745 0.3193 0.3042 0.055 0.015 M02(O) 0.1447 0.1 148 -0.0807 0.030 0.034 0.59 Moz(-2) 0.0713 0.1030 0.1189 0.032 0.016 0.73 Rh2(+2) 0.4109 0.3090 0.3062 0.103 0.003 Rh2(O) 0.1870 0.1003 0.0791 0.087 0.021 0.16 Rh2(-2) 0.0435 0.1210 0.1223 0.078 0.001 1.77 a ABl1 = (orbital energy in column C2 - orbital energy in column C1) b AB", = (orbital energy in column C3 — orbital energy in column C2) AB, —AEy “fill ) EAEx+AEy 232 Assn? + amfi m mgmfio 80m o £89080 2808 80m u 88¢. .. 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