.flm‘vév. ‘.a:. a. y‘. Vt .k an. :a ~ 9 .3192.“ A}? x‘ ‘ , If s ‘ . 9.1. “the . L 5 ‘ . . as. . n." in. ‘Mfw {yuan um...“ .- . w . [51.2.1- I -.rm¥.fi_fia.fizm.m . a ‘ 15.: in»? y s . o. 5N. 5:44.“.th if: , \‘W‘ Uri. it :v. ur ’3‘an . .3 g. :1119 a. 2.]: t .: ”inf. . .. r 7‘ . L y .. . £5 {:11 , ,.\.l._.: .l‘vlr.uv.¢llfit 3. I I ll. . This is to certify that the thesis entitled SYNTHESIS AND STRUCTURAL CHARACTERIZATION OF NEW MULTINARY GROUP 15 (BISMUTH AND ANTIMONY) CHALCOGENIDES presented by SUMOHAN MISRA has been accepted towards fulfillment of the requirements for the MASTER OF degree in CHEMISTRY SCIENCE Major Pr essor’ [Signature €][/Z 0 / Date MSU is an Affinnative Action/Equal Opportunity Institution LIBRARY Michigan State University PLACE IN RETURN BOX to remove this checkout from your record. To AVOID FINES return on or before date due. MAY BE RECALLED with earlier due date if requested. DATE DUE DATE DUE DATE DUE 6/01 c:/CIRC/DateDue.p65p.15 SYNTHESIS AND STRUCTURAL CHARACTERIZATION OF NEW MULTINARY GROUP 15 (BISMUTH AND ANTIMONY) CHALCOGENIDES By Sumohan Misra A THESIS Submitted to Michigan State University in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE Department of Chemistry 2004 (I: “.371 E m V4. . ALA-s Tiff. CORPUS VJ ' »o“.. u 'CI'SdnA\ IRJIHn “'9’ ”Mk“ 5145; w ' I . h: ”503?; 4 bubkthuh *Q1. " ‘1'». M'I ‘- , “ML ABSTRACT SYNTHESIS AND STRUCTURAL CHARACTERIZATION OF NEW MULTINARY GROUP 15 (BISMUTH AND ANTIMONY) CHALCOGENIDES By Sumohan Misra Multinary bismuth chalcogenides are an attractive class of compounds due to their rich compositional and structural variety which makes them some of the most adaptable and versatile systems. Together with this rich structural heterogeneity, their potential as leading thermoelectric materials led us to the investigation of these multinary bismuth chalcogenide. Three new compounds KszBiSSIO, Kbe4-2xBi4+xSm-yTey, and NaxSr4-2xBi4+xSe10 all having KBI633S|o type structure and showing variation in either the metal or the chalcogenide site were obtained. Physicochemical characterization of KszBissm is reported. We also obtained two derivatives of the K2,sBig,5Se14 structure type: Rb1+be3- 2,.Bi7+,‘Sem.yTey and NaxBa5-2xBi6+xSe.4. Physicochemical characterization of NaxBas- 2xBi6+xSel4is reported. We also employed solvothennal synthetic conditions to study the system Cszse/M/Se (M = Bi, Sb). C53Sb58e9 was obtained which is an ordered structural variant than the one previously reported. This thesis describes the synthesis and structural characterization of the above mentioned compounds. Iaould like 3; 5.73m and at 23:5 for their he? ACKNOWLEDGEMENTS Iwould like to thank my advisor, Professor Mercouri G. Kanatzidis for all his help, support and advice. I would also like to thank all my past and present group members for their help and support. iii ISTOFTABLEE SYOFHGLRE €3.71: 1. .Iluitm. Fmoeiectn'r M. lntrodu. Bhflnna Apphca Malena Referen Cater 2. Sim/w: .IJSHQBD. rSé’. U A. Irim B. Exp Re; 5}: C. PI Table of Contents LIST OF TABLES viii LIST OF FIGURES x Chapter 1.Multinary Bismuth Chalcogenides and Their Application as Thermoelectric Materials 1 Introduction 1 Multinary Bismuth Chalcogenides 1 Application of Multinary Bismuth chalcogenides as Thermoelectric Materials 5 References 8 Chapter 2. Synthesis and Structure of KszBi 5S ,0, Kbe4-2xBi4+xS 10.yTey, and Na,Sr4-2xBi4+xSem belonging to the Cosalite structure type 10 A. Introduction 10 B. Experimental Section 11 Reagents 11 Synthesis 12 Bi28e3 12 PbTe 12 KzBigsl 3 12 KszBisslo 12 K,‘Pb4.2,,Bi4+xS10.),Tey 13 NaxSr4-2xBi4+xSem 13 C. Physical Measurements 14 Energy Dispersive Spectroscopy 14 iv .I Q9 " 1“. Sim Conclu Refers ii. PithBi .,5. A. In B. Ei. R; S; Differential Thermal Analysis Charge Transport Measurements Powder X-ray diffraction Single-Crystal X-ray Crystallography KszBiSSm Ko.93Pb3.043i4.34S9.60T€0.40 Nao.4755f2.7933i4.7133610 D. Results and discussion Structure Description of KszBiSSlo Thermal Analysis of KszBisslo Charge Transport Measurement of KszBISSm Structure Description of K,,Pb4.2,,Bi4+,,S10.),Tey Structure Description of NaxSr4-2xBi4+xSelo Conclusion References Chapter 3. Variation in the K 2, 531's. 5Se14 structure type: Synthesis and Structure of Rbl+be3-2xBi7+,Sel4.yTey and NaxBa5-2xBi6+xSe,4 A. Introduction B. Experimental Section Reagents Synthesis Bi28e3 14 14 15 25 15 15 16 21 21 22 22 29 35 4O 41 43 43 fi t 45 C. Ph) Enc‘ Dif C h: For Sin D. Res Stn Sin PbTe szBIsSCl 3 Rb]+be3-2xBl7+xSCI4-yTey NaxBa5-2xBi6+xSe14 C. Physical Measurements Energy Dispersive Spectroscopy Differential Thermal Analysis Charge Transport Measurements Powder X-ray diffraction Single-Crystal X-ray Crystallography Rbl.73Pbl .29Bi83613.42T60.59 NaiBaz.7oBi7.37S€i4 D. Results and discussion Structure Description of Rb]+,(Pb3,.2,,Bi7+xSe14.yTey Structure Description of NaxBa5-2xBi6+xSei4 Thermal Analysis of NaxBa5-2xBi6+xSe14 Charge Transport Measurement of NaxBa5-2xBi6+xSe14 Conclusion References Chapter 4. Solvothermal Synthesis of Ordered Structure of Cs 3Sb 5Seg A. Introduction B. Experimental Section vi 45 45 45 46 46 46 46 47 47 48 48 48 54 54 61 62 62 7O 71 73 73 75 Sol SW C. Phj En Sir D. Re iDPExDICES APPE APPE Reagents Solvent Synthesis CS3Sb5$69 C. Physical Measurements Energy Dispersive Spectroscopy Single-Crystal X—ray Crystallography D. Results and discussion Structure Description of Cs3Sb58e9 Conclusion References APPENDICES APPENDIX A. CIF FILE FOR KszBisslo APPENDIX B. CIF FILE FOR Kbe4-2xBi4+xSlo-yTey APPENDIX C. CIF FILE FOR NaxSr4-2xBi4+xSe10 APPENDIX D. CIF FILE FOR Rb.+,‘Pb3.2,,Bi7+,.Se14.yTey APPENDIX E. CIF FILE FOR NaxBa5-2xBi6+xSel4 APPENDIX F. CIF FILE FOR CS3Sb58€9 vii 75 75 76 76 76 76 77 82 82 93 94 96 97 107 118 134 151 169 Table ll '1 1 7 T331: ---' Table 2 Table 2-7. Table 2-8. Table 3.3. Iable 3.4_ T”able 3.5. Table 36 Table 2-1. Table 2-2. Table 2-3. Table 2-4. Table 2-5. Table 2-6. Table 2-7. Table 2-8. Table 2-9. Table 2-10. Table 3-1. Table 3-2. Table 3-3. Table 3-4. Table 3-5. Table 3-6. Table 3-7. LIST OF TABLES Crystallographic Data for KszBisslo, Kbe4-2xBi4+xSm-yTey, and Naxsr4-2xBi4+xsel 0 Atomic coordinates (x 104) and equivalent isotropic displacement parameters (A2 x 103) for KszBisslo Atomic coordinates (x 104) and equivalent isotropic displacement parameters (A2 X 103) for K0.93Pb3.043i4.3439.60T€o.4o Atomic coordinates (x 104) and equivalent isotropic displacement parameters (A2 X 103) for Nao.4753f2.79sBi4.7i3Seio Bond distances (A) for KszBisslo Selected Angles (deg) for KszBi5810 Bond distances (A) for Kbe4-2xBi4+xSlo-yTey Selected Angles (deg) for K,,Pb4_2,,Bi4.t,‘S10.,Tey Bond distances (A) for NaxSr4-2xBi4+xSe10 Selected Angles (deg) for NaxSr4-2xBi4+xSe.o Crystallographic Data for Rb;+,,Pb3,.;z,,Bi7+,,Se14.yTey and NaxBa5-2xBi6+xSe14 Atomic coordinates ( x 104) and equivalent isotropic displacement parameters (A2 x 103) for Rb],73Pb1,ngigSe.3,42Teo,59 Atomic coordinates (x 104) and equivalent isotropic displacement parameters (A2 x 103) for NalBa2.7gBi7,378e14 Bond distances (A) for Rb1+be3-2xBi7+xSe14-yTey Selected Angles (deg) for Rb1+,,Pb3.2,,Bi7+,,Se14.),Tey Bond distances (A) for NaxBa5-2xBi6+xSe14 Selected Angles (deg) for NaxBa5-2xBi6+xSel4 viii 17 18 19 20 25 26 32 33 38 39 49 50 52 57 59 64 66 Table-H- iale #2. Table #3. Table 4-1. Table 4-2. Table 4-3. Table 4-4. Table 4-5. Physical constants for ethylene diamine Crystallographic data for the ordered CS3Sb5$e9 and the structure reported by Sheldrick and Hausler Atomic coordinates (x 104) and equivalent isotropic displacement parameters (A2 x 103) for CS3SbSSe9 Bond distances (A) for CS3Sb5869 Selected Angles (deg) for C53Sb58e9 ix 78 79 80 87 90 Figure 1-1. Figure 1-1. Figure 1-2. Figure 2-1. Figure 2-2. Figure 2-3. Figure 2-4. Figure 2-5. Figure 2-6. Figure 2-7. Figure 2-8. Figure 3-1. LIST OF FIGURES Some of the different types of coordination environment that Bi atoms adopt in various multinary bismuth chalcogenides: (a) trigonal pyramidal in B-CsBiSz, (b) square pyramidal in Rb23138613, (c) perfect octahedral in RbBiSz, (d) distorted octahedral in B-KzBi38e13, (e) bicapped trigonal prismatic in KBi6,33Sm, (t) monocapped trigonal prismatic in szLaxBig-xSI4 Different building blocks that are found in multinary bismuth chalcogenides: (a) NaCl-type fragment, (b) BizTe3-type fragment, (0) CdIz-type fragment, (d) SbZSe3-type fragment Projection of the structure of KszBisslo down the b-axis Polyhedral representation of KszBisslo down the b-axis showing the connectivity of the M86 octahedra (M = Bi, Pb) DTA diagram of KszBisslo showing the endothermic and exothermic peaks. The heating and cooling rates were 10°C/min Variable temperature thennopower for a polycrystalline oriented ingot of KszBiSSm Projection of the structure of Ko,93Pb3,o4Bi4,3489,60Te0,4o down the b-axis Polyhedral representation of Ko,93Pb3_04Bi4,3489,60Teo,4o down the b-axis showing the connectivity of the M86 octahedra (M = Bi, Pb, Bi/K) Projection of the structure of Nao,4758r2,7ggBi4,7138e10 down the b- axis Polyhedral representation of Nao,4758r2,793Bi4,713Se10 down the b- axis showing the connectivity of the M86 octahedra (M = Bi, Bi/Sr) Projection of the structure of Rbl,73Pb1.2gBi3$e13,42Te0,59 down the b-axis 3 4 23 24 27 28 30 31 36 37 56 Table 3—1. Table 4—1. Table 4-2. Table 4—3. Table 4—4. Table 3-2. Table 3-3. Table 3-4. Table 4-1. Table 4-2. Table 4-3. Table 4-4. Projection of the structure of NalBa2,7gBi7,37Sel4 down the b-axis DTA diagram of NaxBa5-2xBi6+xSe14 showing the endothermic and exothermic peaks. The heating and cooling rates were 10°C/min Variable temperature thennopower for a polycrystalline oriented ingot of NaxBa5-2xBi6+xSe14 SEM image of the hexagonal rod type crystal of CS3Sb5$e9 Projection of the structure of CS3SbSSe9 down the c-axis Different selenoantimonate units which act as building-blocks Projection of one of the layers in C53Sb5$e9 down the b-axis showing the tunnels occupied by the alkali atoms. It also shows the chains connected by the (SbZSe5)4' unit xi 63 84 85 86 Mulllr Introduction The gen a)l.)l'.Bi,Q, ital}- is an it ii'ersity and iTITIOCIECIYII: a Multinary Bisn Bismuth {as of compo him some 0i ii (Ely well exprc Bmuih 310m: hf “Walla!C 813315311] 310m CHAPTER 1 Multinary Bismuth Chalcogenides and Their Application as Thermoelectric Materials Introduction The general formula for multinary bismuth chalcogenide family can be expressed as MwM'xBinz Where M & M' could be any metal and Q is a chalcogen (S, Se, Te). This family is an interesting class of materials due to their compositional and structural diversity and complexity and this makes them attractive for investigations for thermoelectric applications. Multinary Bismuth Chalcogenides Bismuth chalcogenides from a solid state chemistry perspective are an attractive class of compounds due to their rich compositional and structural variety which makes them some of the most adaptable and versatile systems. In nature these characteristics are very well expressed in the sulfosalts familyl where Bi compounds constitute 20% of them. Bismuth atoms both in naturally occurring sulfosalts and in the synthetically derived compounds show an amazing flexibility in bonding. This fact is an underlying reason for the unparalleled diversity and complexity that bismuth chalcogenide compounds possess. Bismuth atom adopt several different coordination environments ranging from trigonal -l_ T I! I": ‘Ll scandal. to SC égfier coordln. IOIleflIIOII en 53.11 This It coordination gel at d-Otbitals It :ezter. Almost fimhemieal l 755 ID probabl) mime interes 30mg Of domed in Van lines; It 515’ch OCL'ihe honxapped m! 35m“ to the ' “VI ,. Anon»... at“ l: 0% .C‘dra I0 c b‘h‘i' . waking blOCk, 4n . QmC 03563 S pyramidal, to square pyramidal, to octahedral (usually distorted) to trigonal prismatic to higher coordination number extending to nine. The cause of such a variety of coordination environments can be pinned down to the 6s2 lone pair of electrons of bismuth. This lone pair can be stereochemically expressed to locally distort the bismuth coordination geometry or can be suppressed by hybridizing with energetically adjacent p- and d-orbitals to form sp3d2 hybrid orbitals thereby producing a regular octahedral Bi” center. Almost any intermediate stage in the continuum is observed between the full stereochemical expression and complete suppression of the lone pair. This property gives rise to probably the most malleable coordination geometry in the periodic table. It is therefore interesting to observe the role of Bi3+ and its role in stabilizing various structure types. Some of the different types of coordination environment for Bi atoms that can be observed in various multinary bismuth chalcogenides can range from trigonal pyramidal in B—CsBiSz,2 to square p yramidal in szBigSe. 3,3 to p erfect o ctahedral in RbBiSz,4 to distorted octahedral in [3-K2Bi38el3,5 to bicapped trigonal prismatic in I(Bi(,,33Sm,6 to monocapped trigonal prismatic in szLa,.Big.,,Sl4.7 These are shown in Figure 1-1. With reference to the figure, for (a) and (b) the lone pair is being completely expressed while for (c) it is completely suppressed. For ((1) it is only partially expressed leading to short bonds (solid lines) trans to longer bonds (dotted line). Another interesting feature of these families of compounds is the ability of BiQ6 octahedra to combine with each other by sharing their edges thereby forming various building blocks. NaCl-type, BizTeg-type and CdIz-type fragment is the most common and in some cases Sb28e3-type fragment can also be seen (see figure 1-2.). figurt l-l. Sort : various mult. care pnamida 3‘. 5-K;Bl;5613. «It in Pb;l C. {C} lei) ff h/ Figure 1-1. Some of the different types of coordination environment that Bi atoms adopt in various multinary bismuth chalcogenides: (a) trigonal pyramidal in B-CsBiSz, (b) square pyramidal in szBisSCn, (c) perfect octahedral in RbBiSz, (d) distorted octahedral in B—KzBi38e13, (e) bicapped trigonal prismatic in KBi6,33810, (f) monocapped trigonal prismatic in szLaxBi3.xSI4. a (a) (b) (C) (d) (e) (f) figure 1'2. .3: 33C 1'1}? ,. "fix Iffiémfi (I it Figure 1-2. Different building blocks that are found in multinary bismuth chalcogenides: (a) NaCl-type fragment, (b) BizTeg-type fragment, (c) CdIz-type fragment, (d) Sb28e3- type fragment. (a) (b) (C) (d) ruler system “‘f . randomness ini as strongly 5c - - .13 iOZldLiCIlI'lI}. first of merit( This n'c :heir potential : airman; bismt Alimitation of. “hen t “011336 grad an they Can b «‘1. ' Ll 41653 are m . The third characteristic property of bismuth atoms is its ability to display mixed occupancy leading to structural disorder with a variety of similar sized ions like alkali metals, 5'6 alkaline earth metals,8 Pb,8’ 9’ '0 Sns’ '0‘ H or rare earth metals.12 This mixed occupancy ofien results in the formation of new structure types that do not exist in the simpler systems. Also this kind of positional disorder in the structure generates randomness in mass, size and charge of the atoms on a particular lattice position and this can strongly scatter acoustic lattice phonons carrying heat and thus lower the thermal conductivity.” The lowering of thermal conductivity is important in maximizing the figure of merit (ZT) of thermoelectric materials (explained later in this chapter). This rich structural heterogeneity that these compounds possess together with their potential as leading thermoelectric materials led us to the investigation of these multinary bismuth chalcogenide. Application of Multinary Bismuth chalcogenides as Thermoelectric Materials When two dissimilar conductors are in contact with each other then at the junction a voltage gradient is generated automatically whose values depend on the type of conductors used and the temperature. Also if a temperature gradient exists along a conductor, a voltage difference is generated which again depends on the type of conductor and the temperature gradient. These effects are known as thermoelectric effects and they can be distinguished as Thomson, Peltier and Seebeck effects. The applications of these are in thermocouples, refiigeration devices and in power generation. The b est m aterials for thermoelectric c ooling applications c urrently u sed in the industry are solid solutions of BizTe3 and Bi2.,,Sb,,Te3.ySey.l4 These materials possess high , A 4", isCCIFICal “Gnu“ resin-emit?" ll stilt S is t} wzjuctl‘IIV. K .71" 1.0 at 30C mare and mmdently 1 Deleted that perfonnmcels sell is a Z T 2 Our 21; :blcogenides Ions. large un mmsition the simplex electr. s . “will cone. tenductil'ltv u “moeleclfic I ll. 1 ”53 rattler; electrical conductivity and thermoelectric power (Seebeck coefficient) and low thermal conductivity. These properties define the dimensionless figure of merit: 27 = (S20) T/ x where S is the thermoelectric power or Seebeck coefficient, a is the electrical conductivity, x is the thermal conductivity and T is the temperature. These alloys have a ZT~ 1.0 at 300 K. The above properties are determined by the details of the electronic structure and scattering of charge carriers (electrons and holes) and thus are not independently controllable parameters. An increase in the electrical conductivity leads to a simultaneous decrease in the thermoelectric power and a comparable increase in the thermal conductivity. Hence it is not easy to improve the value of ZT. Moreover it is now believed that the BizTe3 compounds may be nearing the limit of their potential performance15 and the requirement for a thermoelectric material to be commercially useful is a ZTZ 1.5. Our approach in improving ZT is to identify new multinary bismuth chalcogenides with higher compositional and structural complexity containing heavy atoms, large unit cells and disorder in the crystal lattice. This rationale is based on the proposition that materials with more complex compositions and structures may have complex electronic structure which may give rise to high thermoelectric power and low thermal conductivities.l6 Another concept which helps in lowering the thermal conductivity was introduced by Slack as the limiting characteristic for a superior thermoelectric.” In these materials a weakly bound atom or molecule ‘rattler’ is used. These ‘rattlers’ create low-fi'equency vibration modes that scatter acoustic lattice phonons .au as 'I - L nnfl-;:'1 rzip shows all “rperties. This In C hap img these 5p rill discuss Ill: 1”Lanziritimon carrying heat thereby lowering the thermal conductivity of the solid without severely affecting the electrical conduction, thus leading to improved thermoelectric efficiency.17 The compounds B-KzBIgSCj3,5 CsBi4Te6,18 KBi6,33S;o 6 reported earlier by our group shows all the above mentioned characteristics and exhibit promising thermoelectric properties. This has leaded us to investigate more complicated multinary systems. In Chapters 2 and 3 we will describe the multinary bismuth chalcogenides found during these synthetic investigations and their structural characterization. In Chapter 4 we will discuss the ‘solvotherrnal’ synthesis technique and how it is used to synthesize a ternary antimony chalcogenide. References 1. (313134“ Miner. 19 160.369-2 E.Krist.1.". g.) McCarthj. C. R.; K3 3. Iordanidi. Chen, \K'. Mater. 21. P Voroshi I. - Chung, Kanneu ; 1997, 9, References 1. (a) Makovicky, E. Eur. J. Mineral. 1993, 5, 545-591. (b) Makovicky, E. Fortschr. Miner. 1981, 59,137-190. (c) Makovicky, E. Neues Jahrbuch Miner. Abh. 1989, 160, 269-297. ((1) Makovicky, E. Fortschr. Miner. 1985, 63,45-89. (e) Makovicky, E. Kristallogr. 1985, 173, 1-23. McCarthy, T. J.; Ngeyi, S. -P.; Liao, J. -H; DeGroot, D.; Hogan, T.; Kannewurf, C. R.; Kanatzidis, M. G. Chem. Mater. 1993, 5, 331-340. Iordanidis, L.; Brazis, P. W.; Kyratsi, T.; Ireland, J.; Lane, M. ;Kannewurf, C. R.; Chen, W.; Dyck, J. S.; Uher, C.; Ghelani, N.; Hogan, T.; Kanatzidis, M. G. Chem. Mater. 2001, 13, 622-633. Voroshilov, Y. V.; Peresh, E . Y.; Golovei, M. I. Inorg. Mater. 1972, 8, 777-778. Chung, D-. Y.; Choi, K. -S.; Iordanidis, L.; Schindler, J. L.; Brazis, P. W.; Kannewurf, C. R.; Chen, 8.; Hu, 8.; Uher, C.; Kanatzidis, M. G. Chem. Mater. 1997, 9, 3060-3071. Kanatzidis, M. G.; McCarthy, T. J.; Tanzer, T. A.; Chen, L.; Iordanidis, L.; Hogan, T.; Kannewurf, C. R.; Uher, C.; Chen, B. Chem. Mater. 1996, 8, 1465-1474. Iordanidis, L.; Kanatzidis, M. G. Inorg. Chem. 2001, 40, 1878-1887. Wang, Y. C.; DiSalvo, F. J. Chem. Mater. 2000, 12, 1011-1017. Chung, D-. Y.; Iordanidis, L.; Rangan, K. K.; Brazis, P. W.; Kannewurf, C. R.; Kanatzidis, M. G. Chem. Mater. 1999, 11, 1352-1362. 10. Choi, K. -S.; Chung, D-. Y.; Mrotzek, A.; Brazis, P. W.; Kannewurf, C. R.; Uher, C.; Chen, W.; Hogan, T.; Kanatzidis, M. G. Chem. Mater. 2001, 13, 756-764. 11. Mrotzek, A.; Chung, D-. Y.; Hogan, T.; Kanatzidis, M. G. J. Mater. Chem. 2000, l 0( 7), 1667-1672. 12. IordzmlC Chem. 1 13. (a) 5131‘ Coohng Boca R Ehrenre p l. 14. la) Yim W. M; Przylusl 15. Goldsm 16. Mon, ,\' Publicat 17. Sales, B 18- (a) Nola 73. 173- C- J. Ap 12. Iordanidis, L.; Schindler, J. L.; Kannewurf, C. R.; Kanatzidis, M. G. J. Solid State Chem. 1999, 143(2), 151-162. 13. (a) Slack, G. A. New Materials and Performance Limits for Thermoelectric Cooling. In CRC Handbook of Thermoelectrics; Rowe, D. M., Ed,; CRC Press: Boca Raton, F1, 1995; pp 407-440. (b) Slack, G. A. Solid State Physics; Ehrenreich, H., Seitz, F., Tumbull, D., Eds.; Academic: New York, 1997; Vol. 34, pl. 14. (a) Yim, W. M.; Fitzke, E. V. J. Electrochem. Soc. 1968, 115, 556-560. (b) Yim, W. M.; Fitzke, E. V.; Rosi, F. D. J. Mater. Sci. 1996, 1, 52-65. (c) Borkowski, K.; Przyluski, J. Mater. Res. Bull. 1987, 22, 381-387. 15. Goldsmid, H. J. Electronic Refrigeration, Pion: London, 1986. 16. Mott, N. R; Jones, H. The theory of the Properties of Metals and Alloys, Dover Publications: New York, NY. 17. Sales, B. C.; Curr. Opin. Solid St.Mater. 1997, 2, 284-289. 18. (a) Nolas, G. S.; Cohn, J. L.; Slack, G. A.; Schujman, S. B. Appl. Phys. Lett. 1998, 73, 178-180. (b) Nolas, G. S.; Slack, G. A.; Morelli, D. T.; Tritt, T. M.; Ehrlich, A. C. J. Appl. Phys. 1996, 79, 4002-4008. Synthesis an “fill-213i“ .tlntroducl Bismutl henoeleetrics niitation in 1 suitinn bism fie lo their co b.1165: lone p me which i Times of th A supe iifibril coeffi. Lime Ofmeri: tinsel lat: it. - . “Minis. CHAPTER 2 Synthesis and Structure of KszBiSSw, KbenszimSIMTey, and Na,Sr4.2,Bi4+,Selo belonging to the Cosalite structure type. A. Introduction Bismuth chalcogenides have a wide range of applications including thermoelectrics,1 and non-linear optical materials.2 From the point of view of their application in thermoelectrics our approach has been to focus on new semiconducting multinary bismuth chalcogenides. These materials are an interesting class of compounds due to their compositional and structural complexity arising due to the presence of an inert 6s2 lone pair of electrons on bismuth which may or may not be stereochemically active which in turn affects the lattice structure, the electronic structure and thus the properties of the resulting compounds. A superior thermoelectric material has high electrical conductivity (0), high seebeck coefficient (S) and low thermal conductivity (rc). These together define the TE figure of merit ZT = (a 82/ x) T. Factors contributing to low thermal conductivity and thus higher ZT are the presence of heavy atoms like Bi and Pb, large unit cells and disorder in the crystal lattice. The rationale behind using lead is that in addition to being very heavy it has similar electronic properties as Bi and has a well known tendency to disorder with Bi or alkali metals, depending on the local environmentf"5 This kind of site occupancy disorder in the structure generates randomness in mass, size and charge of the atoms on a 10 ;afieular lattii Enl- tl‘luS lone tozd‘octiiity i: channels or I. 1555 10115 m; rend in the 133mg} Condu Ripon it: mClure 3:31ch I'Or I new cOmpOu“ £31138;th B'EXperim, Reagen (Cat. Milka). particular lattice position that can strongly scatter acoustic lattice phonons carrying heat and thus lower the thermal conductivity.6 Another approach in lowering the thermal conductivity in these materials is to incorporate alkali or alkaline earth metals in the channels or layers formed by these infinite anionic bismuth-chalcogen frameworks. These ions make relatively weak ionic bonds with chalcogens due to which they rattle around in their channels or in between the layers thereby creating low-frequency vibration modes that scatter acoustic lattice phonons carrying heat, thus reducing the thermal conductivity. 7 Reports previously from our group showed that KBi6,33Sw 8 which has a cosalite like structure has thermal conductivity substantially lower than BIzTC3 making it attractive for further investigations for thermoelectric applications. We report here three new compounds KszBisslo, Kbe4-2xBi4+xSm-yTey, and NaxSr4-2xBi4+xSelo all having KBi6,33Sm type structure showing variation in either the metal or the chalcogenide site. B. Experimental Section Reagents: Chemicals were used as obtained: (i) bismuth chunks, 99.999% purity, Cerac, Milwaukee, WI, (ii) sulfur powder, sublimed, Spectrum Chemical Mfg. Corp., Gardena, CA, (iii) selenium shots (99.999% purity, Cerac, Milwaukee, WI), (iv) tellurium chunks 99.999% purity, Cerac, Milwaukee, WI, (v) potassium metal, Aldrich, Milwaukee, WI, (vi) lead metal, Cerac, Milwaukee, WI, (vii) strontium selenide powder 99.5% purity, -20 mesh, Cerac, Milwaukee, WI. Nazse was prepared by a stoichiometric reaction of sodium metal and selenium shots in liquid ammonia. 11 spthfS al'acuum Am 335 Vail-15d b? {m 573312.110??? 813593: mum “35 I i‘asuum (‘104 3o: 10 hours an .‘taefions. PbTe: claim was I sailed under V; therefor 12 he timer reactior Synthesis: All manipulations were carried out under a dry nitrogen atmosphere in a Vacuum Atmospheres Dri-Lab glovebox. The purity and homogeneity of the products was verified by comparing the X-ray powder diffraction patterns to those calculated by the crystallographically determined atomic coordinates. Bizse3: A mixture of 6.383g (0.031 mol) of bismuth and 3.617g (0.046 mol) of selenium was transferred into a 13mm quartz tube, which was then flame sealed under vacuum (~10‘4 Torr). The tube was heated to 800°C in 10 hours, held at that temperature for 10 hours and then cooled down to 50°C in 10 hours. The product was used for further reactions. PbTe: A mixture of 12.378g (0.060 mol) of lead and 7.622g (0.060 mol) of tellurium was transferred into a 13mm carbon coated quartz tube, which was then flame sealed under vacuum (~104 Torr). The tube was heated to 1100°C in 8 hours, isothenned there for 12 hours and then cooled down to 50°C in 24 hours. The product was used for further reactions. KzBisSu: A mixture of 0.180g (4.60 mmol) of potassium, 3.858g (0.018 mol) of bismuth and 0.962g (0.030 mol) of sulfur was transferred into 13mm quartz tube, which was then flame sealed under vacuum (~104 Torr). The tube was heated to 150°C in 6 hours, and then firrther heated upto 850°C in 6 hours, isothermed there for 1 hour and then cooled down to 50°C in 48 hours. The product was used for further reactions. KszBisslo: A pure synthesis of KszBiSSlo was achieved with a mixture of 0.05g (1.280 mmol) of potassium, 0.265g (1.280 mmol) of lead, 0.668g (3.20 mmol) of bismuth and 0.205g (6.40 mmol) of sulfur in the ratio 2:225:10 which were transferred into a 13mm quartz tube and was flame sealed under vacuum (~10'4 Torr). The tube was 12 sealed to 850T 5511‘C in 30 he 2.:lle like cry sag a Seannir 3153‘. gave an ; le’bH [553 mmol) of tes- flme sea} 5d ISOIITCTmeg t“31110 5135c 11113311131113 3: Electron MICrc WOleaze CC NarSI' XS’: and 047 heated to 850°C in 10 hours and isothermed there for 48 hours and then cooled slowly to 550°C in 30 hours and finally to 50°C in 3 hours. The product consisted of silvery-gray needle like crystals. A quantitative analysis by Energy Dispersive Spectroscopy (EDS) using a Scanning Electron Microscope (SEM) was performed on several of these crystals which gave an approximate composition of “KPb3,30Bi3,3683.03”. KbeasziflxquTey: A mixture of 0.4g (0.185 mmol) of KzBi8513 and 0.185g (.553 mmol) of PbTe in the ratio 1:3 was transferred into a 9mm quartz tube, which was then flame sealed under vacuum (~10“1 Torr). The tube was heated to 850°C in 10 hours and isothenned there for 48 hours and then cooled slowly to 500°C in 96 hours and finally to 50°C in 5 hours. The product consisted of silvery-gray needle like crystals. A quantitative analysis by Energy Dispersive Spectroscopy (EDS) using 3 Scanning Electron Microscope (SEM) was performed on several of these crystals which gave an approximate composition of “KPb4_6zBi3,95S9_73Te0,27”. NaxSrnsziflxSew: A mixture of 0.03g (0.24 mmol) of Na2Se, 0.2g (1.2 mmol) of SrSe and 0.472g (7.2 mmol) of BiZSe3 in the ratio 1:5:3 were transferred into a graphite tube which was placed in a 13mm quartz tube, which was then flame sealed under vacuum (~104 Torr). The tube was heated to 800°C in 24 hours, held at that temperature for 24 hours and then cooled to 50°C in 25 hours. The product consisted of silvery-gray rod like crystals. Energy Dispersive Spectroscopy (EDS) on several of these crystals gave an approximate composition of “NaSr1,9(,Bi4,6oSe9,6g”. 13 , ‘ c.1119“I ’ Energ.‘ sitimd “e: $33611 “lit 1 ‘1 Differe 311371-ch “ll ‘ 1 gig}: CQSlalS motile contai he detector. T 11611 by co if?! DTA, Ill: ate was c Charge mmllllflll fro 7315mm (COT; PM“. The ter: heater which - 3535321 $139: 1‘13 11le 5., ‘1‘" t. . Q likafllrek C. Physical Measurements Energy Dispersive Spectroscopy: Quantitative microprobe analyses of the compound were performed with a JEOL JSM-64OOV Scanning Electron Microscope equipped with a Tracor Northern Energy Dispersive Spectroscopy (EDS) detector. Data were acquired it sing an accelerating v oltage o f 20 k V and a 3 0 se conds accumulation time. Differential Thermal Analysis: Differential Thermal Analysis (DTA) was performed with a computer-controlled Shimadzu DTA-50 thermal analyzer. Ground single crystals (30-40 mg) were sealed in silica ampoules under vacuum. A silica ampoule containing alumina of equal mass was sealed and placed on the reference side of the detector. The samples were heated to 1000°C at 10°C/min, isothenned for 1 minute followed by cooling at 10°C/min. The reported DTA temperature is the peak temperature. After DTA, the samples were examined with powder X-ray diffiaction. Reproducibility of results was checked with multiple heating / cooling cycles. Charge Transport Measurements: Thermopower was measured using an instrument fi'om MMR Technologies, Inc., Mountain View, CA. The sample and the reference (constantan wire) were mounted on a Seebeck stage with conductive silver paste. The temperature gradient across the sample was built up by a computer controlled heater which is controlled by the MMR Programmable Seebeck Controller 88100. The Seebeck stage was attached to the MMR stage, which provides a given stable temperature for the measurement. The MR K20A Programmable Temperature Controller controls this MMR stage. The voltage across the sample resulting from the temperature gradient was measured. 14 Poudt‘ ifiaetion for sing a CPS position-semi wraparlson 0f theCERlL'S: Single K; 4%} {51.814 feet. The int effectometei 513 sphere of lheShLART reéuction. Th solution \k as c KPb;I Strands PCT WP Puma . Powder X-ray diffraction: The compounds were examined by X-ray powder diffraction for identification and to assess phase purity. Powder patterns were obtained using a CPS 120 INEL diffi'actometer using Cu-Ka radiation and equipped with a position-sensitive detector. The purity and homogeneity of all phases was confirmed by comparison of X-ray powder diffraction to those calculated from single-crystal data using the CERIUS2 software.9 Single-Crystal X-ray Crystallography: Single crystals of KszBisslo, Ko_93Pb3.o4Bi4,34S9_6oTeo,4o and Nao_475Sr2_793Bi4,-,.3Selo were mounted on the tip of a glass fiber. The intensity data were collected at 293 K on a Bruker SMART Platform CCD diffractometer using graphite monochromatized Mo K, (it = 0.71073 A) radiation over a full sphere of reciprocal space. Individual frames were measured using O.3° steps in (o. The SMART software was used for data acquisition and SAINT'0 for data extraction and reduction. The absorption correction was done with SADABS'O, and the structure solution was done with the SHELXTL'O package of crystallographic programs. KszBissm: A full sphere of data was collected with an exposure time of 30 seconds per frame. Structure refinement was straightforward in orthorhombic space group ana. After anisotropic refinement final R values, R1 = 2.75% and wR2 = 6.91%. The fractional atomic coordinates and isotropic displacement parameters are shown in Table 2-2. Ko,93Pb3,uBi4.3489,wTeo,4o: A full sphere of data was collected with an exposure time of 20 seconds per frame. Eighteen crystallographically independent positions (Bi 1-5, Pb 1-4, K 1, S 1-9 and Te 10) were found to sit on a crystallographic mirror plane. Pb(3) & Pb(4) and Bi(1) & K(1) were found to be disordered over a single site. After 15 zisotrOPiC ” rte-mic 000le 520.4? of 30 second: to sit on a cry iational ate :4. anisotropic refinement final R values, R1 = 2.96% and wR2 = 6.06%. The fractional atomic coordinates and isotropic displacement parameters are shown in Table 2-3. Nao,475Srz,mBi4,-,13Selo: A full sphere of date was collected with an exposure time of 30 seconds per frame. Eighteen crystallographically independent positions were found to sit on a crystallographic mirror plane. Bi(l) & Sr(1), Bi(3) & Sr(3), Bi(4) & Sr(4), Sr(5) & Na(5), Sr(6) & Na(6) and Sr(7) & Na(7) were all found to be disordered over a single site. After anisotropic refinement final R values, R1 = 7.00% and wR2 = 12.61%. The fractional atomic coordinates and isotropic displacement parameters are shown in Table 2-4. 16 Irblc 21 C11 XéxSILZrBh°‘S Unethical form formula weigh T. K 1.1 Cash} system Space group L1 L1 Table 2-1. Crystallographic Data for KszBiSSm, Kbe4-2xBi4+xS10-yTey, and NaxSI'4.2XBI4+xSC| 0. Chemical formula Formula weight T, K A. A Crystal system Space group a, A b, A c, A 0., deg 13. deg 7. deg v, A3 Z Pearce. g/cm3 it. mm] Total reflections Unique reflections R(int) No. of parameters Goodness-of-fit on F2 Refinement method R1ll wR2b KszBissm 487.33 293(2) 0.71073 ana 23.92700) 4.1 103(16) 19.315(8) 90 9O 90 1899.6(13) 14 5.964 64.327 21493 2674 0.0452 1 10 1.031 0.0275 0.0691 K0.93Pb3.043i4.3439.6oT60.4o Nao.4753f2.79sBi4.7135610 614.93 293(2) 0.71073 Orthorhombic ana 24.11 1(12) 4.089(2) 19.371(9) 90 90 90 1909.8(16) 11 5.881 54.397 20504 2536 0.0577 114 0.911 8172.56 293(2) 0.71073 ana 24.512(15) 4.247(3) 20.205(13) 90 90 90 2104(2) 1 6.451 64.625 16913 2788 0.1820 117 1.013 Full-matrix least-squares on F2 0.0296 0.0606 0.0700 0.1261 ‘ R1 = z IlFol-chll/ZIFOI- " wR2 = {z [W(Foz-Fc2)2]/ZIW(F02)ZI}”2- 17 Table 2-2. Ator 11:1 IN) for 1 311) 32:31 813) Bil-‘1 31le5) Full or; Kill 511) 3(2) Sill 5(5) 16} Si?) 18) $19) Sill) \ Table 2—2. Atomic coordinates (x 104) and equivalent isotropic displacement parameters (A2x 103) for KszBi5S10. x y z U(eq) Bi(l) 1507(1) 2500 161(1) 17(1) Bi(2) 1716(1) -2500 -1897(1) 15(1) Bi(3) 93(1) -2500 -961(1) 19(1) Bi(4) 2020(1) -2500 4090(1) 14(1) Bi(5) 688(1) -7500 4651(1) 18(1) Pb(l) 428(1) 2500 -2751(1) 18(1) Pb(2) 2865(1) -2500 1 157(1) 29(1) K(1) 1301(1) -2500 2171(2) 18(1) S(l) 885(1) 2500 -1367(2) 19(1) 8(2) 1402(1) -7500 3536(2) 17(1) S(3) -272(1) -2500 -2252(2) 17(1) 8(4) 2219(1) -2500 -326(2) 20(1) S(5) 1409(1) -12500 5211(2) 18(1) S(6) 1235(1) -2500 -3094(2) 17(1) S(7) -35(1) -7500 5893(2) 22(1) 3(8) -699(1) -7500 -564(2) 25(1) 8(9) 2376(1) -7500 -2312(2) 16(1) S(lO) 2046(1) 2500 1321(2) 17(1) U(eq) is defined as one third of the trace of the orthogonalized Uij tensor. 18 rmeJ.AH 113x103) 101 hill n2) as; all Bill 1 8:12) EB) Bit) ho) 51.11 in Rh 8.4} 13 8'6) $8) 319) 16110) islSdefi: Table 2-3. Atomic coordinates (x 104) and equivalent isotropic displacement parameters (AZX 103) for K0.93Pb3.04Bi4.34S9.60TCO.40~ x y z U(eq) Occ. Pb(l) 4899(1) -2500 10957(1) 23(1) Pb(2) 2143(1) -2500 8834(1) 32(1) 0.42601 Pb(3) 5681(1) -2500 14587(4) 19(1) 0.46327 Pb(4) 5701(1) -2500 14725(4) 22(1) 0.53673 K(1) 3706(2) -2500 7802(3) 25(1) 0.87487 Bi(l) 3708(3) -2500 8034(4) 36(2) 0.12513 Bi(2) 3490(1) 2500 9831(1) 20(1) Bi(3) 3271(1) -2500 11889(1) 18(1) Bi(4) 7015(1) -7500 14097(1) 17(1) Bi(5) 4564(1) 2500 12726(1) 25(1) S(l) 4110(1) 2500 11359(2) 21(1) S(2) 6384(1) -2500 1352 1 (2) 17(1) S(3) 5270(1) -2500 12243(2) 23(1) S(4) 2769(2) -2500 10318(2) 24(1) 8(5) 2612(1) -7500 12304(2) 19(1) S(6) 6409(2) -7500 15219(2) 23(1) 8(7) 3758(1) -2500 13073(2) 20(1) S(8) 4283(2) -2500 9426(2) 25(1) S(9) 2971(2) 2500 8670(2) 21(1) Te(10) 4984(1) -2500 15908( 1) 27(1) 0.18924 U(eq) is defined as one third of the trace of the orthogonalized Uij tensor. l9 Table 2-1 : 5 r ‘: IA'X 1 A). i Sal) Sell) 56(3) Soil) Sail 56.5) 3‘17.) 5:9) 56110) L' E“1.115 deC. 1‘1 Table 2-4. Atomic coordinates (x 104) and equivalent isotropic displacement parameters (AZX 103) for Nao.4753f2.79sBi4.7133610- x y z U(eq) Occ. Bi(l) 1513(1) 2500 9824(1) 14(1) 0.89828 Sr(l) 1513(1) 2500 9824(1) 14(1) 0.10172 Bi(2) 1719(1) -2500 11920(1) 16(1) 0.49244 Bi(3) 99(1) -2500 11006(1) 17(1) 0.89034 Sr(3) 99( 1) -2500 1 1006(1) 17(1) 0.10966 Bi(4) 2998(1) -7500 10934( 1) 17(1) 0.93817 Sr(4) 2998(1) -7500 10934(1) 17(1) 0.06183 Bi(5) 4358(1) -12500 10390(1) 23(1) Sr(S) 3708(2) -7500 12897(2) 20(2) 0.79289 Na(5) 3708(2) -7500 12897(2) 20(2) 0.2071 1 Sr(6) 2968(1) -2500 8864(2) 15(1) 0.95836 Na(6) 2968( 1) -2500 8864(2) 15(1) 0.04164 Sr(7) 5423(2) -17500 12283(2) 21(2) 0.77261 Na(7) 5423(2) -17500 12283(2) 21(2) 0.22739 Se(l) 885(1) 2500 11308(2) 15(1) Se(2) 2257(2) -2500 10313(2) 18(1) Se(3) 3613(2) -7500 9789(2) 15(1) Se(4) 2411(2) -7500 12301(2) 15(1) Se(5) 5033(2) -17500 10874(2) 19(1) Se(6) -346(2) -2500 12223(2) 18(1) Se(7) 723(2) -2500 9438(2) 19(1) Se(8) 2018(1) 2500 8628(2) 15(1) Se(9) 3628(2) -12500 11563(2) 19(1) Se(lO) 1244(2) -2500 13116(2) 16(1) U(eq) is defined as one third of the trace of the orthogonalized Uij tensor. 20 D. Results Structure Dt This £116?de mai reels filled cries are git a: Figure 2-1 ocnhedral chalcogenide: 51;". coordin lb? same wa 3’833155331' 1 “ism 2.2 CLamels whj 313 Similar to AIOm while the M 234913) to insult in a bond P 5121 mad b1“ ei :~ l D. Results and discussion Structure Description of KszBissm This compound is isostructural with KBi6.33Slo and has a three dimensional structure made up of NaCl-type blocks and CdIz-type fragments that connect to form tunnels filled with eight-coordinate K+ cations. The bond distances and selected bond angles are given in Tables 2-7 and 2-8. The structural diagram down the b-axis is shown in Figure 2-1. The existence of these types of NaCl- and CdIz-type fragments with Bi in an octahedral coordination site is a very common structural motif found in most bismuth chalcogenides. The two different fragments of NaCl-type and Cdlz-type are joined by eight coordinated Pb atoms (i.e., Pb(2)) which are in a bicapped prismatic geometry, in the same way as Bi is found in KBi6_33Slo 8 and various mineral sulfo salts.'1 The [szBissiol' framework is made of edge-sharing MS6 (M = Bi, Pb) octahedra, as shown in Figure 2.2. An interesting feature is the presence of small triangular shaped empty channels which are lined by Bi(5)-S(7)-Pb(1)-S(6)-Pb(2)-S(5). These types of channels are similar to the KBi6,33Slo structure. Atoms Pb(l) and Bi(5) are present in a slightly distorted octahedral coordination where the M-S (M = Bi, Pb) distances range from 2.820(2) to 2.897(2) A for Pb(l) and 2.749(3) to 2.957(4) A for Bi(5). On the other hand Bi(l), Bi(2), Bi(3) and Bi(4) are present in a highly distorted octahedral coordination with a short bond trans to a long bond. Pb(2) is present in a bicapped prismatic geometry where its coordination sphere is filled by eight sulfur atoms and the bond length ranges fi'om 2.856(2) to 3.310(1) A. 21 ..-I" - 'u‘.l'h'-JA l'lermal Ana Ililerential th eel: 'hermal l decompositior oéohermic Im'sallizati irritated no d Charge Tran Tiennoelectri 1.311111 b)‘ Br mpemture tl lkfiflmz Thermal Analysis of KszBissm Differential thermal analysis was performed on pure KszBiSSm samples to ascertain their thermal behavior. At the end of two heating cycles the compound was checked for decomposition by taking its powder X-ray diffraction pattern. KszBiSSm shows an endothermic (melting) peak at 728°C and on cooling shows an exothermic (recrystallization) peak at 703°C. The powder pattern of the compound after DTA indicated no decomposition. (See Figure 2-3.) Charge Transport Measurement of KszBiSSm Thermoelectric power measurements were carried on polycrystalline oriented ingots (grown by Bridgman technique) '2 of KszBiSSlo. It is a n-type conductor and at room temperature the thennopower has a value of -1 33 uV/K. It shows a linear trend till 400 K. (See Figure 2.4.) 22 figure 2-1. P Figure 2-1. Projection of the structure of KszBisslo down the b-axis. NaCl-type ,. e / Q“ e.. Pooh'fibo of" o 9', ‘ . f s- It? '5“ - e“ 9‘» e‘gRQ‘ - ‘o‘ 23 Figure 2-2. Polyhedral representation of KszBisslo down the b-axis showing the connectivity of the MS; octahedra (M = Bi, Pb). 24 IkaSBm hnthOI hdiRJle Shihllxl aural) 18186) hfirh9lx2 hfllhl)x2 $0184) lfilh3l BfllSBJXI Afiihl)xl 16118) 1U115) Adlhzlx huluilx 3115(9) Rmihl) Table 2-5. Bond distances (A) for KszBisslo. Bi(l)-S(10) Bi(1)-S(4) x 2 Bi(1)-S(8) x 2 Bi(1)-S(1) Bi(2)-S(6) Bi(2)-S(9) x 2 Bi(2)-8(1) x 2 Bi(2)-S(4) Bi(3)-S(3) Bi(3)-S(8) x 2 Bi(3)-S(1) x 2 Bi(3)-S(8) Bi(4)-8(5) Bi(4)-S(2) x 2 Bi(4)-S(4) x 2 Bi(4)-S(9) Bi(5)-S(2) 2.586(3) 2.830(2) 2.927(3) 3.305(1) 2.583(3) 2.713(2) 3.038(3) 3.264(1) 2.643(3) 2.899(2) 2.903(2) 3.282(1) 2.612(3) 2.748(2) 2.969(2) 3.069(3) 2.749(3) Bi(5)-S(7) x 2 Bi(5)-8(5) x 2 Bi(5)-S(7) Pb(1)-S(3) x 2 Pb(1)-S(6) x 2 Pb(1)-S(7) Pb(1)-S(l) Pb(2)-S(10) x 2 Pb(2)-S(5) x 2 Pb(2)-S(6) x 2 Pb(2)-S(9) Pb(2)-S(4) K(1)-S(10) x 2 K(1)—S(3) x 2 K(1)-S(2) x 2 K(1)-S(9) K(1)-S(8) 2.786(2) 2.894(2) 2.957(4) 2.820(2) 2.897(2) 2.844(3) 2.888(3) 2.856(2) 3.253(1) 3.310(1) 3.012(3) 3.254(1) 3.178(3) 3.211(3) 3.352(3) 3.319(4) 3.423(5) liblc 2-6. Se? 38181115 $31811h5h 1141181115 Sl-IrBllll‘Sll 5441811150 SlIrBllll-Sll 1618131511. StirBilZl-Sl‘j Sill-Billl-Sl 19.181219 19181313“ 5111812 )-S( 5131813 18 soloists. SiirBlij3)-3( 513181013. 5181313”. 311131313 SISI'Bll-I)-S SciBlh-s Wists 51518114}: 113.1814}; 314.1814“ Table 2-6. Selected Angles (deg) for KszBisslo. S(10)-Bi(1)-S(4) S(4)-Bi(1 )-S(4) S(10)-Bi(1)-S(8) S(4)-Bi(1)-S(8) S(4)-Bi(1)-S(8) S(8)-Bi(l)-S(8) S(6)-Bi(2)-S(9) S(9)-Bi(2)-S(9) S(6)-Bi(2)-S(1) S(9)-Bi(2)-S(1) S(9)-Bi(2)-S(1) S(1)-Bi(2)-S(1) S(3)-Bi(3)-S(8) S(8)-Bi(3)-S(8) S(8)-Bi(3)-S(l) S(3)-Bi(3)-S(1) S(8)-Bi(3)-S(1) S(1)-Bi(3)-S(l) S(5)-Bi(4)-S(2) S(2)-Bi(4)-S(2) S(2)-Bi(4)-S(4) S(5)-Bi(4)-S(4) S(2)-Bi(4)-S(4) S(4)-Bi(4)-S(4) 8924(9) 9313(10) 9568(9) 8863(7) 174.80(10) 89.21(10) 8969(8) 98.49(10) 9052(8) 173.33(7) 8818(7) 8515(9) 9193(9) 9029(10) 8978(7) 8772(8) 179.64(10) 90.14(10) 9124(8) 96.8000) 174.60(8) 9160(8) 87.72(7) 8761(9) 26 S(5)-Bi(4)-S(9) S(2)-Bi(4)-S(9) S(4)-Bi(4)-S(9) S(2)-Bi(5)-S(7) S(7)-Bi(5)-S(7) S(7)-Bi(5)-S(5) S(2)-Bi(5)-S(5) S(7)-Bi(5)-S(5) S(5)-Bi(5)-S(5) S(2)-Bi(5)-S(7) S(7)-Bi(5)-S(7) S(5)-Bi(5)-S(7) S(3)-Pb(1)-S(3) S(3)-Pb(1)-S(7) S(3)-Pb(1)-S(1) S(7)-Pb(1)-S(1) S(7)-Pb(1)-S(6) S(3)-Pb(1)-S(6) S(3)-Pb(1)-S(6) S(1)-Pb(1)-S(6) S(6)-Pb(1)-S(6) S(10)-Pb(2)-S(10) S(10)-Pb(2)-S(9) 174.06(9) 8482(8) 9268(8) 9307(9) 95.07(10) 177.39(8) 8551(8) 8720(7) 9050(9) 177.33(9) 8874(8) 9261(8) 93.57(10) 9481(8) 8474(8) 179.3400) 9283(8) 8762(7) 172.16(9) 8763(8) 9037(9) 92.02(10) 76.14(7) Figure 2.3. D 1'26 heating a] m Figure 2.3. DTA diagram of KszBisslo showing the endothermic and exothermic peaks. The heating and cooling rates were 10°C/min. 20~ 10' “\ 9’“ 200 703°C 400 600 800 1 000 Temperature (°C) 27 Figure 2.4. -I3C n4. :4. w 1 1 ‘II o o I AV_.\>.JV m LogohunvPEBCL. 455 160 Figure 2.4. Variable temperature thennopower for a polycrystalline oriented ingot of KszBIsSlo. -130 ' -135 l '140 ' Q 445 . ’ Thennopower S (uVIK) -150 . o -155 ' -160 ' .- - ' ‘ 300 320 340 360 380 400 420 Temperature (K) 28 C” "T'lfl structure I the ("3111311 51-; (~35 herebj metre 1* nitrite 2 pp: and C amels bu' Kill. The nicturalc Att site with 8 Iii-c Pb. l 33.1: 511110 2.3. Phil). '1 tellunr them in Bill) and tustoal Structure Description of K,Pb4.z‘Bi4+,Slo.yTey The idea of using tellurium here was to investigate whether it goes to a different site than sulfur thereby creating a new structure or whether it goes to the same chalcogen site thereby creating a known structure. In our research we ended up in getting a known structure with a small uptake of tellurium in the sulfur site. The compound has a similar structure as KszBisslo where we have a three dimensional network made up of NaCl- type and Cdlz-type fragments. But here unlike KszBisSm these fragments do not form tunnels but instead the K+ cations are disordered with one of the Bi3+ ions (i.e., Bi(l) & K(l)). The bond distances and selected angles are given in Table 2.9 and 2.10. The structural diagram down the b-axis is shown in Figure 2.6. Atoms K(1) and Bi(l) are disordered in the highly coordinated bicapped prismatic site with 87% K and 13% Bi. The other highly coordinated site is occupied by Pb(2) with 43% Pb. In these sites similar to KszBisSlo the metal coordination sphere is filled by eight sulfur atoms. Here the CdIz-type fragments are made of disordered Pb atoms (Pb(3) and Pb(4)) and Te atoms (Te(10)). The lead sites have 46% of Pb(3) and 54% Pb(4) and the tellurium site is a partially filled site with 19% Te(10). Bi(5), Pb(3) and Pb(4) are present in a slightly distorted octahedral coordination. On the other hand Pb(l), Bi(2), Bi(3) and Bi(4) are present in a highly distorted octahedral coordination with a short bond trans to a long bond. 29 - 1 JV.. Figure 2-5. Projection of the structure of Ko.93Pb3_o4Bi4.3489_6oTeo_4o down the b-axis. co ‘0‘ 0" Ge ‘0‘ e‘ .' ... ‘b w. ... 1’ 'O'Wv 03"?” > '05? 2‘? O . .Bi 0": 3:. 30 Figure 2-6. Polyhedral representation of K093Pb1043i434snge040 down the b-axis showing the connectivity of the M86 octahedra (M = Bi, Pb, Bi/K). 31 Table 2-7. Bond distances (A) for Kbe4-2xBi4+xS(o-yTey. Pb(1)«S(3) Pb(l)-S(l) x 2 Pb(1)-S(8) x 2 Pb(l)-S(8) Pb(2)-S(9) x 2 Pb(2)-S(6) x 2 Pb(2)-S(7) x 2 Pb(2)-8(5) Pb(2)-S(4) Pb(3)-S(2) Pb(3)-Te(10) x 2 Pb(3)-S(6) x 2 Pb(3)-Te(10) Pb(4)«S(6) x 2 Pb(4)-Te(10) x 2 Pb(4)—S(2) Pb(4)-Te(10) K(1).S(9) x 2 K(1)-S(3) x 2 K(1)-S(2) x 2 K(1)-S(5) K(1)-S(8) 2.647(4) 2.899(3) 2.936(3) 3.316(1) 2.875(3) 3.267(1) 3.328(1) 3.022(4) 3.247(1) 2.671(7) 2.769(4) 2.960(5) 3.061(7) 2.831(4) 2.899(5) 2.855(7) 2.869(6) 3.186(5) 3.207(4) 3.287(5) 3.322(6) 3.439(7) 32 Bi(1)-S(9) x 2 Bi(1)-S(3) x 2 Bi(l)-S(2) x 2 Bi(1)-S(5) Bi(l)-S(8) Bi(2)-8(1) Bi(2)-S(9) Bi(2)-S(4) x 2 Bi(2)-S(8) x 2 Bi(3)-S(4) Bi(3)-S(7) Bi(3)-8(5) x 2 Bi(3)-8(1) x 2 Bi(4)-S(6) Bi(4)—S(2) x 2 Bi(4)-S(4) x 2 Bi(4)-8(5) Bi(5)-S(3) x 2 Bi(5)-Te(10) Bi(5)-8(1) Bi(5)-S(7) x 2 2.975(6) 3.248(1) 3.648(1) 3.483(1) 3.031(8) 3.316(1) 2.574(4) 2.844(3) 2.907(3) 3.274(1) 2.577(4) 2.712(2) 3.054(3) 2.620(4) 2.782(2) 2.962(3) 3.072(4) 2.820(3) 2.862(3) 2.865(4) 2.900(3) hill 9'91 S391 NEILE Table 2-8. Selected Angles (deg) for Kbe4-2xBi4+xSm-yTey. S(3)—Pb(l)-S(l) S(l)-Pb(1)-S(1) S(3)-Pb(1)-S(8) S(l)-Pb(1)-S(8) S(l)-Pb(1)-S(8) S(8)-Pb(l)-S(8) S(9}Pb(2)-S(9) S(9)-Pb(2)-S(5) S(2)-Pb(3)-Te(10) Te(lO)-Pb(3)-Te(10) S(2)-Pb(3)-S(6) Te(10)-Pb(3)-S(6) Te(10)-Pb(3)-S(6) S(6)-Pb(3)-S(6) S(2)-Pb(3)-Te( 1 0) Te( 1 O)-Pb(3 )-Te( 1 0) S(6).Pb(3)-Te( l O) S(6)-Pb(4)-S(6) S(6)-Pb(4)-S(2) S(5)-Bi(3)-S(1) S(1)-Bi(3)-S(l) S(6)-Bi(4)-S(2) S(2)-Bi(4)—S(4) S(4)-Bi(4)-S(4) S(6)-Bi(4)-S(S) 88.18(9) 89.71(10) 9061(9) 91.01(8) 178.57(10) 88.26(11) 90.66(1 1) 75.89(8) 95.7(2) 95.2(2) 8675(10) 175.2(3) 88.65(7) 87.4(2) 173.9(3) 88.39(10) 88.9(2) 92.48(19) 85.88(10) 173.09(7) 8406(10) 9158(9) 88.97(8) 87.30(10) 174.05(10) 33 S(6)-Pb(4)-Te(lO) S(2)-Pb(4)-Te(10) S(6)-Pb(4)-Te(10) S(2)-Pb(4)-Te(10) Te(lO)-Pb(4)-Te(10) S(6)-Pb(4)-Te(10) Te(10)-Pb(4)-Te(10) S(9)-Bi(l)-S(9) S(9)-Bi(1)-S(8) S(9)-Bi(2)—S(4) S(4)-Bi(2)-S(4) S(9)-Bi(2)-S(8) S(4)-Bi(2)-S(8) S(4)-Bi(2)-S(8) S(8)-Bi(2)-S(8) S(7)-Bi(3)-S(5) S(5)-Bi(3)-S(5) S(7)-Bi(3)-S(l) S(5)-Bi(3)-S(l) S(2)-Bi(4)-S(2) S(6)-Bi(4)-S(4) S(2)-Bi(4)-S(4) S(2)-Bi(4)-S(5) S(4)-Bi(4)-S(5) 95.4(2) 178.2(2) 8869(7) 89.0(2) 89.72(8) 174.6(3) 8968(18) 86.8(2) 84.53(19) 89.59(10) 91 .92(1 1) 94.80(10) 175.49(11) 89.18(8) 89.39(11) 90.16(9) 97.87(1 1) 89.87(9) 89.04(8) 94.60(l l) 91.44(10) 175.26(8) 84.40(8) 92.86(9) Table 1 3.13131 313sz 15111 Table 2-8. (cont’d) S(3)-Bi(5)-S(3) S(3)-Bi(5)-Te(10) S(3)-Bi(5)-S(1) Te(10)-Bi(5)-S(1) 92.96(11) 94.43(8) 85.61(9) 179.94(9) 34 S(3)-Bi(5)-S(7) Te(10)-Bi(S)-S(7) S(l)-Bi(5)-S(7) S(3)-Bi(5)-S(7) S(7)-Bi(5)-S(7) 8830(8) 9235(8) 87.61(9) 172.99(10) 89.6400) 5mm v 1.0-2‘ ,'| .‘ .wb‘. _ ~14; "18211 Structure Description of N a,Sr4.2,Bi4+,Sem The structure of this compound is very similar to the two previous one but considering only ionic interactions between the alkali and alkaline earth metals with chalcogenides the structure reduces to two dimensional structure having layers of NaCl- type and Cdlz-type fragments joined together. The alkali and alkaline earth metals occupy the sites in b etween these layers. The b 0nd distances and s elected angles are given in Table 2-11 and 2-12. The structural diagram down the b-axis is shown in Figure 2-8. All the three crystallographic sites between the layers are mixed occupied by the alkali and alkaline earth metals. Sr(5) is mixed occupied with Na(S) with 79% Sr(5) and 21% Na(5), Sr(6) is mixed occupied with Na(6) with 96% Sr(6) and 4% Na(6) and Sr(7) is mixed occupied with Na(7) with 77% Sr(7) and 23% Na(7). The BizTe3-type fragment also has mixed occupation, by strontium and bismuth with one site containing only bismuth (i.e., Bi(2)). Bi(l) is mixed occupied with Sr(l) with 90% Bi(l) and 10% Sr(1), Bi(3) is mixed occupied with Sr(3) with 89% Bi(3) and 11% Sr(3) and Bi(4) is mixed occupied with Sr(4) with 94% Bi(4) and 6% Sr(4). Bi(5) is the only atom to be present in a slightly distorted octahedral coordination where the Bi-Se distances range from 2.863(3) to 3.054(3). The remaining atoms Bi(1)/Sr(1), Bi(2), Bi(3)/Sr(1) and Bi(4)/Sr(1) are all present in a highly distorted octahedral coordination. 35 . . ' I 11 1" Figure 2-7. Projection of the structure of Nao.4758r2,793Bi4_7.38e10 down the b-axis. 36 Figure 2-8. Polyhedral representation of Nao,475$r2.793Bi4.7l 38610 down the b-axis showing the connectivity of the M86 octahedra (M = Bi, Bi/Sr). 37 la Table 2-9. Bond distances (A) for NaxSr4-2xBi4+xSelo. Bi(1)/Sr(1)-Se(8) Bi(1)/Sr(1)-Se(1) Bi(1)/Sr(1)-Se(2) x 2 Bi(1)/Sr(l)-Se(7) x 2 Bi(2)-Se(10) Bi(2)-Se(2) Bi(2)-Se(4) x 2 Bi(2)-Se(1) x 2 Bi(3)/Sr(3)-Se(6) Bi(3)/Sr(3)-Se(7) Bi(3)/Sr(3)-Se(1) x 2 Bi(3)/Sr(3)-Se(7) x 2 Bi(4)/Sr(4)-Se(3) Bi(4)/Sr(4)-Se(4) Bi(4)/Sr(4)-Se(9) x 2 Bi(4)/Sr(4)-Se(2) x 2 Bi(5)-Se(5) 2.715(4) 3.371(1) 2.968(3) 2.977(3) 2.682(4) 3.503(1) 2.825(3) 3.196(3) 2.691(4) 3.518(1) 2.931(3) 3.063(3) 2.761(4) 3.113(4) 2.918(3) 3.063(3) 2.958(5) Bi(5)-Se(9) Bi(5)-Se(5) x 2 Bi(5)-Se(3) x 2 Sr(5)/Na(5)-Se(8) x 2 Sr(5)/Na(S)-Se(6) x 2 Sr(5)/Na(5)-Se(9) x 2 Sr(5)/Na(5)-Se(4) Sr(5)/Na(5)-Se(7) Sr(6)/Na(6)-Se(8) x 2 Sr(6)/Na(6)-Se(3) x 2 Sr(6)/Na(6)-Se(10) x 2 Sr(6)/Na(6)-Se(4) Sr(6)/Na(6)-Se(2) Sr(7)/Na(7)-Se(5) Sr(7)/Na(7)-Se(6) x 2 Sr(7)/Na(7)-Se(10) x 2 Sr(7)/Na(7)-Se(1) 2.971(4) 2.863(3) 3.054(3) 3.139(4) 3.153(4) 3.438(5) 3.400(6) 3.410(7) 3.187(4) 3.241(4) 3.245(4) 3.293(6) 3.408(6) 3.002(6) 3.010(4) 3.035(4) 3.065(6) ’1 Table 2-10. Selected Angles (deg) for NaxSr4-2xBi4+xSelo. Se(8)-Bi(l)-Se(2) Se(2)—Bi(l)-Se(2) Se(2)-Bi(1)-Se(7) Se(2)-Bi(l)-Se(7) Se(8)-Bi(l)-Se(7) Se(7)-Bi(1)-Se(7) Se(lO)-Bi(2)-Se(4) Se(4)-Bi(2)-Se(4) Se(4)-Bi(2)-Se(1) Se(lO)-Bi(2)-Se(1) Se(4)-Bi(2)-Se(1) Se(1)-Bi(2)-Se(1) Se(6)-Bi(3)-Se(1) Se(1)-Bi(3)-Se(l) Se(6)-Bi(3)-Se(7) Se(1)-Bi(3)-Se(7) Se(1)~Bi(3)-Se(7) Se(6)-Bi(3)-Se(7) 90.96(10) 91.36(12) 175.42(12) 8864(9) 93.62(1 1) 91.00(12) 90.88(10) 97.48(13) 8942(9) 94.06(10) 171.45(9) 83.27(10) 94.38(10) 92.86(12) 90.00(11) 174.85(12) 8949(9) 90.00(11) 39 Se(7)-Bi(3)-Se(7) Se(3)-Bi(4)-Se(9) Se(9)-Bi(4)-Se(9) Se(3)-Bi(4)-Se(2) Se(9)-Bi(4)-Se(2) Se(9)-Bi(4)-Se(2) Se(2)-Bi(4)-Se(2) Se(3)-Bi(4)-Se(4) Se(9)-Bi(4)-Se(4) Se(2)-Bi(4)-Se(4) Se(5)-Bi(5)-Se(5) Se(5)-Bi(5)-Se(5) Se(5)-Bi(5)-Se(9) Se(5)-Bi(5)-Se(9) Se(5)-Bi(5)-Se(3) Se(5)-Bi(5)-Se(3) Se(5)-Bi(5)-Se(3) Se(9)-Bi(5)-Se(3) Se(3)-Bi(5)-Se(3) 87.80(12) 94.35(11) 9342(13) 88.89(11) 8930(8) 175.59(11) 87.78(11) 174.43(11) 81.86(10) 95.11(10) 95.75(13) 90.21(11) 94.30(11) 173.26(12) 87.65(10) 8802(9) 175.68(10) 87.50(10) 88.13(12) 3.3T ifiA 14, El E. Conclusion The synthesis and structure of three new quaternary bismuth chalcogenides have been presented. Variations in the cosalite structure type are observed whereby replacing the softer Pb2+ with harder Sr2+ collapses the three dimensional character of the cosalite structure to a layered type. The charge—transport properties of K,‘Pb4.2,‘Bi.1+,,Sl0.,Tey and NaxSr¢2xBi4+xSem need to be investigated. Also it would be interesting to do some ion- exchange reactions with NaxSr4-2xBi4+xSem. 4O lel References 1. (a) Kaibe, H.; Tanaka, Y.; Sakata, M.; Nishida, I. J. Phys. Chem. Solids 1989, 50, 945-950. (b) Je on, H .-W.; H a, H .-P.; H yun, D .-B.; S him, J. -D. J. Phys. Chem. Solids 1991, 4, 579-585. (a) Feichtner, J. D.; Roland, G. W. Appl. Opt. 1972, 11, 993-998. (b) Balhnan, A. A.; B yer, R. L.; E imerl, D .; Feigelson, R. S .; Feldman, B. J. ; Goldberg, L. S .; Menyuk, N.; Tang, C. L. Appl. Opt. 1987, 26, 224-227. Takagi, J.; Takeuchi, Y. Acta Crystallogr. 1972, 328, 649-651. Takeuchi, Y.; Takagi, J. Proc. Jpn. Acad. 1974, 50, 76-79. Skowron, A.; Boswell, F. W.; Corbett, J. M.; Taylor, N. J. J. Solid State Chem. 1974, 112, 307-311. (a) Slack, G. A. New Materials and Performance Limits for Thermoelectric Cooling. In CRC Handbook of Thermoelectrics; Rowe, D. M., Ed,; CRC Press: Boca Raton, F1, 1995; pp 407-440. (b) Slack, G. A. Solid State Physics; Ehrenreich, H., Seitz, F., Tumbull, D., Eds.; Academic: New York, 1997; Vol. 34, pl. Choi, K. -S.; Chung, D. -Y.; Mrotzek, A.; Brazis, P.; Kannewurf, C. R.; Uher, C.; Chen, W.; Hogan, T.; Kanatzidis, M.G. Chem. Mater. 2001, 13, 756-764. Kanatzidis, M.G.; McCarthy, T. J.; Tanzer, T. A.; Chen, L. H.; Iordanidis, L. Chem. Mater. 1996, 8, 1465-1474. CERIUSZ, Version 3.8., Molecular Simulations Inc., Cambridge, England, 1999. 10. SAINT v6.45, 1997-2003, SHELXTL v5.1, 1998, Bruker Analytical Xray Systems Inc., Madison, WI 53719, USA. 41 11. (a) Makovicky, E. Eur. .1. Mineral. 1993, 5, 545-591. (b) Makovicky, E. Fortschr. Miner. 1981, 59,137-190. (c) Makovicky, E. Neues Jahrbuch Miner. Abh. 1989, 160, 269-297. 12.Kyratsi, T.; Chung, D. -Y.; Choi, K. —-S.; Dyck, J. S.; Chen, W.; Uher, C.; Kanatzidis, M. G. Mat. Res. Soc. Symp. Proc. 2000, 626, 28.8.1. 42 If—JON4I 5‘ t. I.» u ._ id . we . . .. A. r... v. CHAPTER 3 Variation in the K2,5Bi8,58e14 structure type: Synthesis and Structure of Rb.+,Pb3.szi7+,Se.4.yTey and N axBafixBimSeM. A. Introduction Bismuth compounds constitute a great part of the sulfosalt family.1 These naturally occurring minerals present a remarkable structural diversity and complexity. These characteristics are also found in the great number of ternaryz'8 and quatemarys’” bismuth c halcogenides synthesized d uring the last d ecade. T he rich c ompositional and structural variety makes them some of the most adaptable and versatile systems in solid state chemistry. Bismuth atoms both in naturally occurring sulfosalts and in the above mentioned compounds show an amazing flexibility in bonding. Although they usually exhibit a distorted octahedral geometry, however they also adopt variety of other coordination ranging from trigonal pyramidal in B-CsBiSz3, to square pyramidal in szBigSen”, to trigonal prismatic in ALnlixBimSg (A = K, Rb; Ln = La, Ce, Pr, Nd)9 and sometimes the coordination number can range upto nine.2'12 These high-coordination sites (> 6) serves to connect with each other the several NaCl-, BizTe3 and CdIz-type blocks, formed by the BiQ6 (Q = chalcogen) octahedra when combined together by sharing edges. These above mentioned blocks come in different sizes creating even more structural possibilities. Another reason for the structural heterogeneity is the mixed 43 occupancy that bismuth atoms can display with a variety of similar sized ions such as allitali‘la’l4 or alkaline earth metalss, Pb8’ ”’ '5, Sng' '2’ '5 , or lanthanides.9 Examples of the above mentioned structural diversity and complexity can be found in compounds reported earlier from our group such as KBi385,3 KBi(5,3,3Sm,4a a—,B- KzBissels, 2’ M K2.5Bi85S€14l4. KszBissw,l6 Kbe4-2xBi4+xslo-yTey516 I‘IaxSI'4-2xBi4+xS¢10l6 and many more. Our idea to move from ternary systems to quaternary system was that the latter would give a much more complex structure thereby strongly scattering acoustic lattice phonons carrying heat and thus lowering the thermal conductivity. This would lead to better thermoelectric materials. We report here the synthesis and structural characterization of Rb1+be3- 2,,Bi7+,,SeM.yTey and NaxBa5-2xBi6+xSe14 belonging to the K2,5Bi3,5Se14 structure type. B. Experimental Section Reagents: Chemicals were used as obtained: (i) bismuth chunks, 99.999% purity, Cerac, Milwaukee, WI. (ii) selenium shots 99.999% purity, Cerac, Milwaukee, WI. (iii) tellurium chunks 99.999% purity, Cerac, Milwaukee, WI. (iv) lead metal, Cerac, Milwaukee, WI. (v) rubidium metal, 99.8% purity, Alfa Aesar, Ward Hill, MA. (vi) sodium metal, Aldrich, Milwaukee, WI. (vii) barium selenide powder 99.5% purity, -20 mesh, Cerac, Milwaukee, WI. A2Se (A = Na, Rb) was prepared by a stoichiometric reaction of alkali metal and selenium shots in liquid ammonia. Synthesis: All manipulations were carried out under a dry nitrogen atmosphere in 3 Vacuum Atmospheres Dri-Lab glovebox. The purity and homogeneity of the products was verified by comparing the X-ray powder diffraction patterns to those calculated by the crystallographically determined atomic coordinates. Bi;Se3: A mixture of 6.383g (0.045 mol) of bismuth and 3.617g (0.068 mol) of selenium was transferred into a 13mm quartz tube, which was then flame sealed under vacuum (~10‘4 Torr). The tube was heated to 800°C in 10 hours and isothenned there for 10 hours and then cooled down to 50°C in 10 hours. The product was used for further reactions. PbTe: A mixture of 12.378g (0.060 mol) of lead and 7.622g (0.060 mol) of tellurium was transferred into a 13mm carbon coated quartz tube, which was then flame sealed under vacuum (~10‘1 Torr). The tube was heated to 1100°C in 8 hours, held there for 12 hours and then cooled down to 50°C in 24 hours. The product was used for further reactions. szBisSeu: A mixture of 0.871 g (3.50 mmol) of rubidium selenide and 9.129g (0.140 mol) of bismuth selenide was transferred into a 13mm quartz tube, which was then flame sealed under vacuum (~10'4 Torr). The tube was placed under the flame of a natural gas-oxygen torch until the mixture melted, and then the tube was removed from the flame and the molten mixture was allowed to solidify. The procedure was repeated two more times to ensure homogeneity. The product was used for further reactions. Rb1+,Pb3.2,Bi7+,,Se14-yTe,: A mixture of 0.4g (0.140 mmol) of Rb;BigSe13 and 0.047g (0.140 mmol) of lead telluride in the ratio 1:1 was transferred into a 9mm quartz tube, which was then flame sealed under vacuum (~104 Torr). The tube was heated to 850°C in 10 hours and isothenned there for 48 hours and then cooled slowly to 350°C in 45 96 hours and finally to 50°C in 3 hours. The product consisted of silvery-gray needle like crystals. A quantitative analysis by Energy Dispersive Spectroscopy (EDS) using 8 Scanning Electron Microscope (SEM) was performed on several of these crystals which gave an approximate composition of “Rbl.67Pbl,43Bi7_39$e13,31Te0,70”. Na,Ba5.2,,Bi6+,Se14: A mixture of 0.03g (0.240 mmol) of Nazse, 0.286g (1.32 mmol) of barium selenide and 0.472g (0.720 mmol) of bismuth selenide in the ratio 0.5:2.79:3.69 were transferred into a graphite tube which was placed in a 13mm quartz tube, which was then flame sealed under vacuum (~104 Torr). The tube was heated to 800°C in 24 hours and isothenned there for 24 hours and then cooled 50°C in 25 hours. The product consisted of silvery-gray needle like crystals. Energy Dispersive Spectroscopy (EDS) on several of these crystals gave an approximate composition of ‘N3133553Bi7423615.47”. C. Physical Measurements Energy Dispersive Spectroscopy: Quantitative microprobe analyses of the compound were performed with a JEOL JSM-6400V Scanning Electron Microscope equipped with a Tracor Northern Energy Dispersive Spectroscopy (EDS) detector. Data were acquired u sing an accelerating v oltage o f 20 k V and a 3 0 se conds accumulation time. Differential Thermal Analysis: Differential Thermal Analysis (DTA) was performed with a computer-controlled Shimadzu DTA-50 thermal analyzer. Ground single crystals (30-40 mg) were sealed in silica ampoules under vacuum. A silica ampoule containing alumina of equal mass was sealed and placed on the reference side of 46 the detector. The samples were heated to 1000°C at 10°C/min, then isothenned for 1 minute followed by cooling at 10°C/minute. The reported DTA temperature is the peak temperature. Afier DTA, the samples were examined with powder X-ray diffiaction. Reproducibility of results was checked with multiple heating / cooling cycles. Charge Transport Measurements: Thermopower was measured using an instrument from MMR Technologies, Inc., Mountain View, CA. The sample and the reference (constantan wire) were mounted on a Seebeck stage with conductive silver paste. The temperature gradient across the sample was built up by a computer controlled heater which is controlled by the MMR Programmable Seebeck Controller SBlOO. The Seebeck stage was attached to the MMR stage, which provides a given stable temperature for the measurement. The MR K20A Programmable Temperature Controller controls this MMR stage. The voltage across the sample resulting from the temperature gradient was measured. Room temperature electrical conductivity was measured by a four probe technique using a Keithley 236 Source Measure Unit. 0.003 inch copper wires were used for the c urrent and v oltage electrodes. M easurements o f the p ellet c toss-sectional area and voltage probe separation were made with a calibrated binocular microscope. Powder X-ray diffraction: The compounds were examined by X-ray powder diffraction for identification and to assess phase purity. Powder patterns were obtained using a CPS 120 INEL diffractometer using Cu-Ka radiation and equipped with a position-sensitive detector. The purity and homogeneity of all phases was confirmed by comparison of X-ray powder diffraction to those calculated from single-crystal data using the CERIUS2 software.17 47 Single-Crystal X-ray Crystallography: Intensity data were collected at 293 K on a Bruker SMART Platform CCD diffractometer using graphite monochromatized Mo Kg (2. = 0.71073A) radiation over a full sphere of reciprocal space. Individual frames were measured using 0.3° steps in (o. The SMART software was used for data acquisition and SAINT ‘8 for data extraction and reduction. The absorption correction was done with SADABS'S, and the structure solution was done with the SHELXTL18 package of crystallographic programs. RbL-nPb1,298i38e13,42Te059: A full sphere of data was collected with an exposure time of 45 seconds per frame. The crystallographic data is shown in Table 3-1. Twenty five crystallographically independent positions were found to sit on a crystallographic mirror plane. Pbl & Rb2, Pb2, Rb3 & Pb3, Te2 & Se2 and Te14 & Se14 were all found to be disordered over a single site. Afier anisotropic refinement final R values, R1 = 5.17% and wR2 = 11.75%. The fractional coordinates and isotropic displacement parameters along with occupancies for disordered atoms are shown in table 3-2. NalBa2,7gBi-;37Se.4: A hemisphere of data was collected with an exposure time of 30 seconds per frame. The crystallographic data is shown in Table 3-1. Twenty seven crystallographically independent positions were found to sit on a crystallographic mirror plane. Bi6 & Na6, Bi7 &Na7, Bi8 & Na8 and 8e15, Se16 & Se17 were all found to be disordered over a single site. After anisotropic refinement final R values, R1 = 5.29% and wR2 = 10.78%. The fractional coordinates and isotropic displacement parameters along with occupancies for disordered atoms are shown in table 3-3. 48 Table 3-1. Crystallographic Data for Rb]+be3-2xBi7+xSe14-yTey and NaxBa5-2xBi6+xSe14. Chemical formula Formula weight T, K L A Crystal system Space group a, A b, A c, A (1, deg 13. deg 7. deg v, A3 Z Pcalcd. g/cm3 H. mm“ Total reflections Unique reflections Rant) No. of parameters Goodness-of-fit on F2 Refinement method R1a wR2b RbI .73Pb129Bi8Sel342T6059 798.10 293(2) 0.71073 P2(1)/m 17.610(11) 4.213(3) 21.398(13) 90 109.348(9) 90 1497.9(16) 8 7.078 73.827 16731 3890 0.0860 151 1.009 0.0517 0.1175 N8133279Bi7373614 3554.62 293(2) 0.71073 Monoclinic P2(1)/m 17.407(6) 4.3165(15) 21.747(7) 90 98.768(6) 90 1614.9(10) 2 7.310 64.326 14160 4245 0.1181 171 1.294 F ull-matrix least-squares on F2 0.0529 0.1078 ‘ R1 = z IlFol-chll/ZIFOI- " sz = {z 1w(F.2-F£)21/21w(F.2)21}”2. 49 Table 3-2. Atomic coordinates ( x 104) and equivalent isotropic displacement parameters (Azx 103) for Rb1.73Pb1,29B138e1 3_42Te0,59 x y z U(eq) Occ Rb(l) 4216(2) 2500 3546(2) 29(1) Bi(l) 5215(1) 2500 913(1) 21(1) Bi(2) 7203(1) -2500 632(1) 28(1) Bi(3) 3367(1) -2500 1387(1) 24(1) Bi(4) 8913(1) -12500 4290(1) 21(1) Bi(5) 8756(1) -7500 6155(1) 21(1) Bi(6) 9180(1) -7500 2701(1) 24(1) Bi(7) 9083(1) -7500 135(1) 23(1) Bi(8) 6659(1) -12500 4816(1) 21(1) Pb(l) 6679(2) -l7500 3101(2) 33(1) 0.69871 Rb(2) 6617(7) -17500 2855(8) 13(2) 0.30129 Pb(2) 1663(5) -7500 2104(9) 34(2) 0.40436 Rb(3) 1375(7) -7500 1933(6) 12(2) 0.43145 Pb(3) 1645(9) -7500 1895(17) 31(5) 0.18427 Se(l) 8305(2) -7500 1262(2) 22(1) Te(2) 4512(2) 2500 1958(2) 22(1) 0.08409 Se(2) 4512(2) 2500 1958(2) 22(1) 0.91591 Se(3) 7872(2) -7500 4486(2) 21(1) Se(4) 9716(2) -7500 7457(2) 21(1) Se(S) 10173(2) -12500 842(2) 22(1) Se(6) 8124(2) -12500 2952(2) 21(1) Se(7) 4210(2) -12500 4916(2) 19(1) Se(8) 7811(2) -12500 6372(2) 22(1) Se(9) 4010(2) -2500 150(2) 19(1) Se(10) 10068(2) -17500 4147(2) 17(1) Se(11) 7896(2) -2500 -595(2) 28(1) Se(12) 2833(2) -2500 2435(2) 25(1) Se(13) 5794(2) -12500 3480(2) 29(1) 50 Table 3-2. (cont’d) x y z U(eq) Occ Te(14) 6333(2) -2500 1600(2) 21(1) 0.20309 Se(14) 6333(2) ~2500 1600(2) 21(1) 0.79691 U(eq) is defined as one third of the trace of the orthogonalized Uij tensor. 51 Table 3-3. Atomic coordinates (x 104) and equivalent isotropic displacement parameters (Azx 103) for NajBa2_79Bi7.378e.4. x y z U(eq) ’ Occ. Bi(l) 3225(1) 7500 4771(1) 12(1) Bi(2) 4553(1) -2500 11723(1) 17(1) Bi(3) 1894(1) 2500 6034(1) 16(1) Bi(4) 696(1) -2500 14326(1) 20(1) Bi(5) 3929(1) 2500 9695(1) 25(1) Bi(6) 2483(1) 2500 1 11 17(1) 22(1) 0.68214 Na(6) 2483(1) 2500 11117(1) 22(1) 0.31786 Bi(7) -503(1) 2500 12842(1) 19( 1) 0.53889 Na(7) -503( 1) 2500 12842(1) 19(1) 0.46111 Bi(8) 1809(2) 7500 9440(1) 40(1) 0.70179 Na(8) 1809(2) 7500 9440(1) 40(1) 0.29821 Bi(9) 362(1) -2500 10936(1) 42(1) Ba(l) 2159(1) 2500 12982(1) 14(1) Ba(2) 3153(1) 7500 7776(1) 13(1) 38(3) 5043(1) 7500 6315(1) 14(1) Se(l) 3262(2) -2500 10420(2) 18(1) Se(2) 2962(2) 7500 6200(2) 15(1) Se(3) 1884(2) 2500 4510(2) 15(1) Se(4) 5360(2) -7 500 10983(2) 20(1) Se(5) 3742(2) -7500 12192(2) 15(1) Se(6) 2641(2) 2500 8826(2) 18(1) Se(7) 1824(2) -2500 1 1 766(2) 26(1) Se(8) 4274(2) 2500 51 12(2) 13(1) Se(9) 1734(2) 2500 7265(2) 16(1) Se(10) 3500(2) 7500 3572(2) 12(1) Se(l l) 5663(2) -2500 12737(2) 11(1) Se(12) 1075(2) 2500 10143(2) 21(1) Se(13) 720(2) -2500 13069(2) 18(1) 52 Table 3-3. (cont’d.) x Y Z U(eq) Occ Se( 14) 531(2) -2500 5778(2) 14( 1) Se(15) -399(l6) -7500 1 1481 (6) 47(6) 0.68043 Se(16) -606(18) -6200(110) 1 1513(13) 24(10) 0.24310 Se(l 7) -70(50) -7500 1 1540(20) 45(17) 0.16378 U(eq) is defined as one third of the trace of the orthogonalized Uij tensor. 53 D. Results and discussion Structure Description of Rb.+,,Pb3.2,,Bi-;.,,Se.4.,Tey The compound is isostructural to K25Bi358e14 ‘ and possesses a complex 3D anionic framework which is very similar to that of B- K2Bi88e13l (see Figure 3-1.). The main difference being the presence of only NaCl- and BizTe3-type fi‘agments in case of Rbl4,.Pb3.2,.Bi7+,,Se14.y'l‘ey whereas the presence of additional CdIz-type fragments in case of B- KzBlgsfil3. These different types of fragments are common in other multinary bismuth chalcogenides such as Cs3Bi7Se1219 and KBi(,-,33810.4a The BizTe3-type fragments in Rbp.,,Pb3.2,.Bi7+,.Se.4.yTey are arranged side by side to form layers. The NaCl-type fiagments connect these layers which run p erpendicular to the c -axis, to b uild a three dimensional framework with tunnels which are filled by the alkali (Rb+) cations. The NaCl-type fragments in Rb]..,,Pb3.2,,Bi7+,,Se14.,Tey are three bismuth octahedra wide whereas the BizTe3-type fragments are five bismuth octahedra wide. The latter is an important structural difference with the B- KzBigseU structure where these fi'agments are three Bi octahedra wide. Among the Rb+ cations in Rb]+be3-2xBi7+xSe14-yTey, Rb( 1) is fully occupied by Rb+ while Rb(2) is disordered with Pb( 1) and Rb(3) is disordered with Pb(2) and Pb(3) (see figure 3-1). The Rb(2) site contains 70% Pb and 30% Rb while the Rb(3) site contains 43% of Rb, 40% of Pb(2) and 18% of Pb(3). There are two eight coordinate sites. One is occupied by Pb(l) and Rb(2) in a distorted bicapped trigonal prismatic coordination by Se(6), Se(6)’, Se(13), Se(13)’, Te14/Se(14), Te(14)/Se(14)’, Se(3) and Te(2)/Se(2) (the atoms primed outside parentheses are the symmetrically equivalent ones). Pb(l) is disordered with Rb(2) at 0.499(1)A. The other site has Rb(3), Pb(2) and Pb(3) 54 atoms in a similar kind of coordination. The prism is defined by Se(4), Se(5), Se(12) and their symmetry equivalent atoms while the capping atoms are Se(8) and Se(ll). Here Rb(3) is disordered with Pb(2) and Pb(3) at a distance of 0.518(3) and 0.51(2)A respectively. These high-coordinate sites serve to stitch together the layers formed by BizTe3-type fi'agments. Two of the chalcogenide sites in the BizTe3-type fragments close to Pb(1)/Rb(1) disordered site has mixed occupancy. The Se(2) site contains 92% of Se(2) and 8% of Te(2). The Se(14) site contains 80% of Se(14) and 20% of Te( 14). Apart from Bi(6) all the bismuth atoms in both types of fragments are present in a highly distorted octahedral coordination with a short bond trans to a long bond. In contrast Bi(6) is in a slightly distorted octahedral coordination where the Bi-Se distances range fi'om 2.953(4) to 2.974(3) (see Table 3-4. & 3-5.). This site also serves as the second joining point for the two types of fragments. 55 Figure 3-1. Projection of the structure of Rbmngl,29BigSe1342Te059 down the b-axis. 56 RR R Ft 5: 2h EB Table 3-4. Bond distances (A) for Rb],73Pb1,nglgsCI3,42T6059. Rb(l )~Se(12) Rb(1)-Se(13) Rb(1)-Se(7) Rb(l)-Te(2)/Se(2) Rb(1)-Se(7) Rb(1)-Se(8) Rb(2)-Se(13) Rb(2)-Te(14)/Se(14) Rb(2)-Se(6) Rb(2)-Se(3) Rb(2)-Te(2)/Se(2) Rb(3)-Pb(3) Rb(3)-Pb(2) Rb(3)-Se(12) x 2 Rb(3)-Se(5) x 2 Rb(3)-Se(4) x 2 Rb(3)-Se(8) Rb(3)-Se(11) Bi(1)-Te(14)/Se(14) x 2 Bi(1)-Se(9)x 2 Bi(1)-Te(2)/Se(2) Bi(1)-Se(9) Bi(2)-Se(1) x 2 Bi(2)-Se(9) x 2 Bi(2)-Te(14)/Se(14) 3.491(4) 3.527(4) 3.532(5) 3.603(5) 3.613(4) 3.632(5) 3.099(10) 3.319(13) 3.341(9) 3.457(16) 3.565(12) 0.51(2) 0.518(3) 3.219(10) 3.331(10) 3.390(10) 3.428(13) 3.505(13) 2.925(3) 3.051(3) 2.893(4) 3.016(4) 2.879(3) 3.071(3) 2.955(4) Bi(2)-Se(1 1) Bi(3)-Te(2)/Se(2) x 2 Bi(3)-Se(11) x 2 Bi(3)-Se(9) Bi(3)-Se(12) Bi(4)-Se(3) x 2 Bi(4)-Se(10) x 2 Bi(4)-Se(6) Bi(4)-Se(10) Bi(5)-Se(8) x 2 Bi(5)-Se(10) x 2 Bi(5)-Se(4) Bi(5)-Se(3) Bi(6)-Se(4) x 2 Bi(6)-Se(6) x 2 Bi(6)-Se(1) Bi(6)-Se(10) Bi(7)-Se(5) x 2 Bi(7)-Se(11) x 2 Bi(7)-36(1) Bi(7)-Se(5) Bi(8)-Se(7) x 2 Bi(8)-Se(3) x 2 57 3.241(5) 2.892(3) 3.124(3) 3.206(4) 2.702(4) 2.913(3) 3.013(3) 2.736(4) 3.231(4) 2.817(3) 3.167(3) 2.740(4) 3.389(1) 2.961(3) 2.974(3) 2.953(4) 2.968(4) 2.914(3) 3.013(3) 3.142(4) 2.811(4) 2.773(2) 3.240(3) Table 3-4. (Cont’d) Bi(8)-Se(13) Bi(8)-Se(8) Pb(1)-Se(13)x 2 Pb(1)-Se(6) x 2 Pb(1)s6(3) Pb(1)-Rb(2) 2.759(4) 3.275(1) 2.892(3) 3.398(2) 3.012(5) 0.499(1) Pb(2)-Se(12) x 2 Pb(2)-Se(8) Pb(3)-Pb(2) Pb(3)-Se(12) x 2 Pb(3)-Se(1 1) 58 2.867(6) 3.079(18) 0.439(1) 2.923(11) 314(4) Table 3-5. SCIGCICd Angles (deg) fOI' Rb1_73Pb.,29Bi38e.3_42Te0,59. Te(2)-Bi(1)-Te(14) Te(14)-Bi(l)-Te(14) Te(2)-Bi(1)-Se(9) Te(14)-Bi(1)-Se(9) Te(2)-Bi(1)-Se(9) Te(14)-Bi(l)-Se(9) Te(2)-Bi(1)-Se(9) Te(14)-Bi(1)-Se(9) Se(9)-Bi(l)—Se(9) Se(9)-Bi(1)-Se(9) Se(1)-Bi(2)-Se(1) Se(1)-Bi(2)-Te(14) Se(1)-Bi(2)—Se(9) Se(1)-Bi(2)-Se(9) Te(14)-Bi(2)-Se(9) Se(9)-Bi(2)-Se(9) Se(1)-Bi(2)-Se(1 1) Te(14)-Bi(2)-Se(1 1) Se(9)-Bi(2)-Se(1 1) Se(12)-Bi(3)-Te(2) Te(2)-Bi(3)-Se(2) Se(12)-Bi(3)-Se(1 1) Te(2)-Bi(3)-Se(1 1) Te(2)-Bi(3)-Se(l 1) Se(12)-Bi(3)-Se(1 1) Se(l 1)«Bi(3)—Se(1 1) Se(12)-Bi(3)-Se(9) 9008(9) 92.13(10) 178.57(10) 8893(9) 9078(9) 9027(7) 9078(9) 177.45(8) 9026(9) 87.32(10) 9405(12) 9560(9) 175.08(10) 8958(8) 8733(9) 86.61(10) 9015(9) 171.55(10) 8652(9) 92.02(10) 93.51(12) 93.98(10) 172.65(11) 9054(8) 93.98(10) 84.80(10) 179.68(11) Te(2)-Bi(3)-Se(9) Se(l 1)-Bi(3 )-Se(9) Se(6)-Bi(4)-Se(3) Se(3)-Bi(4)-Se(3) Se(6)-Bi(4)-Se(10) Se(3)-Bi(4)-Se(10) Se(3)-Bi(4)-Se(10) Se(10)-Bi(4)-Se(10) Se(6)-Bi(4)-Se(10) Se(3)-Bi(4)-Se(10) Se( 1 0)-Bi(4)-Se( 10) Se(4)-Bi(5)-Se(8) Se(8)-Bi(5)-Se(8) Se(4)-Bi(5)-Se(10) Se(8)-Bi(5)-Se(10) Se(8)-Bi(5)-Se(10) Se(8)—Bi(5)-Se(10) Se(10)-Bi(5)-Se(10) Se(1)-Bi(6)-Se(4) Se(4)-Bi(6)-Se(4) Se(1)-Bi(6)-Se( 10) Se(4)-Bi(6)-Se(10) Se(1)-Bi(6)-Se(6) Se(4)-Bi(6)-Se(6) Se(4)-Bi(6)-Se(6) Se(1)-Bi(6)-Se(6) 59 87.76(9) 8626(10) 9146(10) 92.63(1 1) 91.12(9) 176.76(10) 8927(8) 8871(10) 176.96(10) 9064(9) 8671(9) 91 .78(10) 96.79(1 1) 8898(9) 8991(8) 173.23(7) 173.23(7) 8837(9) 9091(9) 9070(1 1) 179.69(10) 8887(9) 9270(9) 176.39(12) 8943(8) 9270(9) Table 3-5. (Cont’d) Se(10)-Bi(6)-Se(6) Se(6)-Bi(6)-Se(6) Se(5)-Bi(7)-Se(5) Se(5)-Bi(7)-Se(5) Se(5)-Bi(7)-Se(1 1) Se(5)-Bi(7)-Se(1 1) Se(5)-Bi(7)-Se(1 1) s60 1)-Bi(7)-Se(1 1) Se(5)-Bi(7)-Se(1) Se(5)-Bi(7)-Se(1) Se(l 1)-Bi(7)-Se( 1) Se(13)-Bi(8)-Se(7) Se(7)-Bi(8)-Se(7) 8752(9) 9020(1 1) 89.82(10) 9259(12) 91.65(10) 177.58(9) 8933(8) 88.71(11) 178.16(11) 8890(9) 89.67(10) 93.5200) 98.86(11) Se(13)-Bi(8)-Se(3) Se(7)-Bi(8)-Se(3) Se(7)-Bi(8)-Se(3) Se(3)-Bi(8)-Se(3) Se(13)-Pb(1)-Se(13) Se(13)-Pb(1)-Se(3) Rb(3)-Pb(2)-Se(12) Se(12)-Pb(2)-Se(12) Rb(3)-Pb(2)-Se(8) Se(12)-Pb(2)-Se(8) Se(12)-Pb(3)-Se(12) Se(12)-Pb(3)-Se(l l) 60 87.21(10) 171.04(7) 9000(8) 81.1 1(9) 93.5004) 89.3503) 129.1(7) 946(3) 128.9(18) 784(4) 922(5) 894(7) Structure Description of NaxBasszm,Se14 The structure of this compound is very similar to Rb,,Pb5.2,,Bi(,+,.Se14.,Tey structure. In the previous compound lead replaces the bismuth atoms in the high-coordinate sites. In NayBasquifixSeM moving from lead to barium the trend remains the same but the bonding becomes more ionic. Barium too, replaces the high-coordinate bismuth sites but due to its more ionic nature the resultant structure is different fi'om the previous one. Here too, only NaCl- and BizTe3-type fragments exist and the former fi'agment is three bismuth octahedra wide while the latter is five bismuth octahedra wide which is a point of su'uctural difference with the B-KzBlgSCl 3 structure. The NaCl-type fragments connect the layers formed by BizTeg-type fragments to generate a three dimensional fi'amework with tunnels which are filled by the alkaline earth (Ba2+) cations. Among the alkaline earth (Ba2+) cations, Ba(l) and Ba(2) occupy the bismuth high-coordinate sites while Ba(3) occupies the tunnels (see figure 3-2). All these three sites are fully occupied. Ba(1,2) is present in a bicapped trigonal prism like coordination with eight Se atoms in the range between 3.293(3) —— 3.464(4)A for Ba(l) and between 3.295(3) — 3.443(5)A for Ba(2). The coordination environment of Ba(3) is a little different and can be described as a distorted tricapped trigonal prism. The prism is defined by Se(8), Se(10), Se(l 1) and their symmetry-equivalent atoms, while the capping atoms are Se(2), Se(5) and Se(8). The alkali (Na+) cations have mixed occupancy over three sites with Bi(6, 7, 8). The Bi(6) site contains 68% of Bi and 32% of Na, the Bi(7) site contains 54% of Bi and 46% of Na and the Bi(8) site contains 70% of Bi and 30% of Na. The Bi(7) mixed site is present in the NaCl fragment whereas the other two mixed sites are present in the B12TC3 fragment. This disorder can be attributed to very similar 61 ionic sizes of Na+ and Bi3+ in octahedral coordination (n.1,,+ = 1.16A, r1313+ = 1.17A).20 Bi(1-5) are present in a highly distorted octahedral coordination with a short bond trans to a long bond. The other interesting feature of this structure is the disordered selenium site containing three selenium atoms, Se(15), Se(16) and Se(17) which also makes up the coordination sphere for the mixed site of Bi(7)/Na(7) and Bi(8)/Na(8). For bond lengths and selected angles see Table 3-6. & 3-7. Thermal Analysis of NaxBaM,Bi6+,Se14 Differential thermal analysis was performed on pure NaxBa5-2xBi6+xSe14 to ascertain its thermal behavior. At the end of two heating cycles the compound was checked for decomposition by taking its powder X-ray diffraction pattern. NaxBa5- 2xBi6+xSe14 show an endothermic (melting) peak at 819°C and on cooling shows an exothermic (recrystallization) peak at 788°C (see Figure 3-3.). The powder pattern of the compound after DTA indicated no decomposition. Charge Transport Measurement of NaxBayszififie” Thermoelectric power measurements were carried on polycrystalline oriented ingots (grown by Bridgman technique) 2' of NaxBa5-2xBi6+xSe14. It is a n-type conductor and at room temperature the thennopower has a value of -24.22 uV/K. It shows a linear trend till 400 K. (See Figure 34). Electrical conductivity measurements were carried on polycrystalline oriented ingots along the needle axis and at room temperature value of 183.61 S/cm was obtained. 62 Figure 3-2. Projection of the structure of NalBa2,7gBi7_37Sel4 down the b-axis. 63 Table 3.6. Bond distances (A) for NalBa2,79Bi7_37Se14. Bi(1)-Se(10) Bi(1)-Se(8) x 2 Bi(1)-Se(3) x 2 Bi(1)-Se(2) Bi(2)-Se(l 1) Bi(2)-Se(5) x 2 Bi(2)-Se(4) x 2 Bi(2)-86(1) Bi(3)-Se(9) Bi(3)-Se(2) x 2 Bi(3)-Se(14) x 2 Bi(3)-Se(3) Bi(4)-Se(13) Bi(4)-Se(3) x 2 Bi(4)-Se(14) x 2 Bi(4)-Se(14) Bi(5)-Se(6) Bi(5)-Se(4) x 2 Bi(5)-Se(1) x 2 Bi(5)-Se(4) Bi(6)/Na(6)-Se(7) x 2 Bi(6)/Na(6)-Se(1) x 2 Bi(6)/Na(6)-Se(5) Bi(6)/Na(6)-Se(12) 2.722(4) 2.851(3) 3.167(3) 3.208(4) 2.701(4) 2.851(2) 3.147(3) 3.337(1) 2.733(4) 2.836(3) 3.193(3) 3.313(1) 2.740(4) 2.974(3) 3.020(3) 3.215(4) 2.704(4) 2.987(3) 3.008(3) 3.453(1) 2.908(3) 3.070(3) 2.950(5) 2.984(5) Bi(7)/Na(7)-Se(16) x 2 Bi(7)/Na(7)-Se(13) x 2 Bi(7)/Na(7)-Se(9) x 2 Bi(7)/Na(7)-Se(15) Bi(7)/Na(7)-Se(14) Bi(7)/Na(7)-Se(17) Bi(8)/Na(8)-Se(16) x 2 Bi(8)/Na(8)-Se(15) Bi(8)/Na(8)-Se(1 7) Bi(8)/Na(8)-Se(6) x 2 Bi(8)/Na(8)-Se(12) x 2 Bi(8)/Na(8)-Se(l) Bi(9)-Se(17) x 2 Bi(9)-Se(16) x 2 Bi(9)-Se(15) x 2 Bi(9)-Se(7) Bi(9)-Se(12) x 2 Bi(9)-Se(12) Ba(1)-Se(10) x 2 Ba(1)-Se(13) x 2 Ba(1)-Se(7) x 2 Ba(1)-Se(3) Ba(1)-Se(5) Ba(2)-Se(1 1) x 2 Ba(2)-Se(9) x 2 64 292(3) 3.019(3) 3.025(3) 2.992(12) 3.009(5) 305(4) 277(3) 292(2) 3.429(1 1) 3.022(3) 3.036(3) 3.049(5) 269(3) 276(3) 2.880(14) 2.887(5) 3.135(3) 3.159(5) 3.293(3) 3.334(3) 3.395(4) 3.427(4) 3.464(4) 3.295(3) 3.340(3) Table 3-6. (cont’d) Ba(2)-Se(6) x 2 Ba(2)-Se(2) Ba(2)-Se(4) Ba(3)-Se(10) x 2 3.359(3) 3.395(4) 3.443(5) 3.310(3) Ba(3)-Se(11) x 2 Ba(3)-Se(8) Ba(3)-Se(8) x 2 Ba(3)-Se(2) Ba(3)-Se(5) 65 3.345(3) 3.488(4) 3.497(4) 3.593(4) 3.594(5) Table 3-7. Selected Angles (deg) for NalBa2,79Bi7,37Se14. Se(10)-Bi(l)-Se(8) Se(8)-Bi(1)-Se(8) Se(10)-Bi(1)-Se(3) Se(8)-Bi(1)-Se(3) Se(8)-Bi(1)-Se(3) Se(3)-Bi(l)-Se(3) Se(10)-Bi(1)-Se(2) Se(8)-Bi(1)-Se(2) Se(3)-Bi(1)-Se(2) Se(10)-Bi(1)-Ba(3) Se(8)-Bi(1)-Ba(3) Se(3)-Bi(1)-Ba(3) Se(2)-Bi(1)-Ba(3) Se(11)-Bi(2)-Se(5) Se(5)-Bi(2)-Se(5) Se(l 1)-Bi(2)-Se(4) Se(5)-Bi(2)-Se(4) Se(5)-Bi(2)-Se(4) Se(4)-Bi(2)-Se(4) Se(9)-Bi(3)-Se(2) Se(2)-Bi(3)-Se(2) Se(9)-Bi(3)-Se(14) Se(2)-Bi(3)-Se(14) Se(2)-Bi(3)-Se(14) Se(14)-Bi(3)-Se(14) Se(13)~Bi(4)-Se(3) Se(3)-Bi(4)-Se(3) 9284(9) 9839(12) 9345(9) 171.16(9) 8750(7) 85.9300) 178.09(1 1) 8592(9) 8794(9) 122.58(9) 5485(7) 125.60(7) 5551(7) 9224(10) 9839(1 1) 95.64(10) 170.290 1) 8699(7) 86.60(10) 92.2000) 99.1002) 8925(9) 172.78(9) 8790(7) 85.05(10) 9104(10) 93.06(11) Se(13)-Bi(4)-Se(14) Se(3)-Bi(4)-Se(14) Se(3)-Bi(4)-Se(14) Se(14)-Bi(4)-Se(14) Se(13)-Bi(4)-Se(14) Se(3)-Bi(4)-Se(14) Se(14)-Bi(4)-Se(14) Se(6)-Bi(5)-Se(4) Se(4)-Bi(5)-Se(4) Se(6)-Bi(5)-Se(1) Se(4)-Bi(S)-Se(1) Se(4)-Bi(5)-Se(1) Se(1)-Bi(5)-Se(1) Se(7)-Bi(6)-Se(7) Se(7)-Bi(6)-Se(5) Se(7)-Bi(6)-Se(12) Se(5)-Bi(6)-Se(12) Se(7)-Bi(6)-Se(1) Se(7)-Bi(6)-Se( 1) Se(5)-Bi(6)-Se(1) Se(12)-Bi(6)-Se(1) Se(1)-Bi(6)-Se(1) Se(16)-Bi(7)-Se(16) Se(16)-Bi(7)-Se(15) Se(16)-Bi(7)-Se(14) Se(l 5)-Bi(7)-Se( 14) Se(16)-Bi(7)-Se(13) 66 9249(10) 176.3702) 87.74(7) 9124(1 1) 175.7902) 9186(9) 8457(9) 9095(0) 9252(11) 9122(10) 177.7903) 8784(7) 91.7101) 9582(13) 85.20(12) 90.1402) 173.0303) 176.3900) 8740(8) 9345(10) 9151(11) 89.34(11) 22(2) 13.100) 168.1(10) 177.5(5) 103.6(10) Table 3-7. 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