MODULAR. FORMS OF DIMENSION -2 FOR SUBGROUPS OF THE MODULAR GROUP Thesis fiat H10 Dome. of Ph. D. MICWGAH STATE UNEVERSITY John. Roderick Smart 1961 EHEQS This is to certify that the thesis entitled MODULAR FORMS OF DIMENSION -2 FOR SUBGROUPS OF THE MODULAR GROUP presented by John Roderick Smart has been accepted towards fulfillment of the requirements for Ph.D. degree”, Mathematics TOT 2:19 A é/Z/Am Major professor Date May 10, 1961 0-169 MSJ EURNING MATERIIQ: Place in book drop to LJBRAfiJES remove this checkout from _—;‘—- your record. FINES will be charged if book is returned after the date stamped below. -i ABSTRACT MODULAR FORMS OF DIMENSION -2 BELONGING TO SUBGROUPS OF THE MODULAR GROUP by John Roderick Smart Joseph Lehner has given a method for defining Poincare series of dimension -2 on the modular group ['(l) which does not rely on the Hecke method of intro- ducing a convergence factor. The problem considered in this thesis is the following: extend the method to con- gruence subgroups of the modular group; and determine when the method can be extended to arbitrary subgroups of finite index. Let r'be a subgroup of finite index, and let A3100, 3 = 1, 2, --- , 0(l—) be a complete set of inequiv- alent parabolic cusps. AJ el’(l). We assume A3100 = 00 if and only if A3 = I. Let’U’be an abelian character on F-. - R Define e(KJ) szAle JA3) where 7&3 is the least positive _ 7x integer such that A310 JA36 V and we use the notation e(z) = exp[2viz]. ‘We define for integers p {'0 e((u+A.)V z/‘A ) (*) G(Z,/U,A ,F ,p) = i ‘g _:I_L Cid :2 J c=-m sztm “(A3 vc,d)(cz+d) CCG(AJ,F) d6 flogAjgr) John Roderick Smart The sets of integers QT(AJ,T) and OEKC,AJ,K') are so defined that vc,d = (a bl c d) runs over a complete set of matrices in AJT— with different lower row as c runs over é’(AJ,T ) and d runs over ¢3(c,AJ,i ). The double series in (*) is not aboslutely convergent, therefore, we specify that it is to be summed first on d and then on c. With this convention the functions G defined in (*) are regular in‘ki, the upper half plane. In order to show the proper functional equation is satisfied we must prove a Rademacher lemma. By a lattice point for AJK' we mean the lower row (c,d) of a matrix in AJF. Let 0(AJ, l") represent the set of all lattice points for AJF‘. Furthermore, for any positive integer K let C}K(AJ,F') be the set of all lattice points for Aji— contained in the square with sides u = i K, v = 1 K in the u,v-plane. We define a class'Vn of matrices such that every Véilll has the form MUn’X 'X V=1UmwithM€—Wl, U =(l7\[01)andm and n integers. Then the Rademacher lemma implies: e((p+K )vc (ls/Ag: (**) C(zs'U'sAJsr all) 3 11m :‘(UT-J‘ K‘>°° Vc d)(cz+d)2 (c.d)€6‘:(:3.r‘ )M (EKMJJ' )M = i(c¢+¥d,gc +Sd): (c,d)f-0'K(AJ,i-) i that is John Roderick Smart we think of M as acting on the u,v-plane as an affine transformation. Using the Lipschitz formula we derive the Fourier expansion of the functions G. This then shows that they have the prOper behavior at the cusps. All of these results required an estimate of OHcll/2 +8 ) for the Kloosterman sums corresponding to i-and«yt. We use a result of Petersson's which says these sums have the prOper estimate if T.is a congruence subgroup andlv'is identically l on a principal congruence subgroup. The problem we considered was solved in the following generality: whenever the Kloosterman sums have the prOper estimate the method of Lehner can be extended to subgroups of finite index. MODULAR FORMS OF DIMENSION -2 FOR SUBGROUPS OF THE MODULAR GROUP BY John Roderick Smart A THESIS Submitted to Michigan State University in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY Department of Mathematics 1961 5:", a? z/ // /..=’/2 2, 5,, / To Pat ii ACKNOWLEDGEMENTS The author wants to express his sincere thanks to Professor Joseph Lehner for his patient guidance on this and other problems. I want, also, to express my indebtedness to Professor Lehner for his kindness in letting me read portions of his forthcoming book on Automorphic Functions. It most certainly clarified my ideas and the notations which I have used in this paper. I am indebted to two organizations for financial support, the National Science Foundation and the University of Michigan Institute of Science and Tech- nology. Finally, I should like to show appreciation to Professor Hans Rademacher, who showed me his improved method of partial summation for estimating sums like (h.28). This was of utmost service to me. 111 51.. when“ h? "'- 1‘ .1 )AM‘H‘NU4-J TABLE C l ‘11 Section 1. Introduction ............................. 1 Section 2. Preliminaries ............................ 7 Section 3. Convergence and Regularity ............... 17 Section h. The Rademacher Lemma ..................... 29 Section 5. The Functional Equation .................. 55 Section 6. The Fourier Series ....................... 59 Section 7. The Behavior at the Cusps ................ _6h Section 8. Kloosterman Sums, Main Theorem and Examples 70 Section 9. [The Inner Product Formula ................ 91 Bibliography OOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOOO 102 iv m A to L1 Figure 3.1 Figure h.1 Figure h.2 Figure h.3 Figure k.h Figure h.5 Figure h.6 Figure h.7 Figure %.8 OF FIGURES OOOOOOOOOOOOOOOOOO. OOOOOOOOOOCOOOOOOOO COOOOOOOOOCOOOOO... OCOOOOOOOOOOOOOOOOO OOOOOOOOOOOOOOOOOO. OOOOOOOOOOOOOOOOOOO OOOOOOOOOOOOOOOOOOO OOOOOCOOCOOOOOOOOOO 20 31 35 #8 1+9 so 51 52 52 LI ST OF TABLES 1. Table 8.1 Generators and Exponent Sums forl'(6) .... 85 2. Table 8.2 Generators and Exponent Sums for FIR) .... 87 3. Table 8.3 Generators and Exponent Sums for r(8) .... 89 vi 1. Introduction In this section we give a description of the problem considered and the results of our research. The defini- tions and results required for this investigation are given in the next section. Lehner [6] introduced the series °° °° e<- -(p-°L)Vk r) (1.1) r (1:) =2 X ‘m M m__mg flVk,-m"'1‘kt'm”2 (msk)=1 where E is a multiplier system for l—(l) and the dimen- sion -2, o _<, ot< 1, U = (1 1| 0 1), Vk,-m = (* *l.k,-m) €l"(1) and chat ) = 6(U). We use the notation e(z) = exp [2viz]. Furthermore, we write matrices in one line with a bar separating rows. He proved that for u = l, 2, ... Fp(‘C3 is a mbdular form of dimension -2 for the multiplier system Eregular in71L== {z = x+iy: y > 0}. Basic to the proof is an estimation of the Kloosterman sums Ak,“(m) which arise as 0(k1/2+E' ). . t; ' Furthermore, the results depend heavily on a generalization of a lemma due to Rademacher, which -2- allows the rearrangement of certain conditionally conver- gent double series. Lehner derives the Fourier expansion of these functions at the infinite cusp. These coeffi- cients are expressed as an infinite series of the Petersson-Rademacher type, which involve Bessel functions. The functions F“(1:) are not identically zero since they have a pole at It: 100. Our problem can now be stated: (1) extend the methods and results to congruence subgroups of the modular group: (ii) extend the results to arbitrary subgroups of finite index in l—(l). We obtain partial solution of these problems. Let r_be a subgroup of l‘(l) of finite index. Assume -16 I". Let 13100 = p3, J = 1, 2, a be a set of inequivalent parabolic cusps of r.. AJELT'(1) and A1 = I. Suppose 4I=1I(T',-2) is a multiplier system for T’and the dimension -2. Consider the following series: ° ° °“|*"'3’Vc d25/71 ) (1.2) G(z,qr,AJ,f ,p) e Z Z l. c=-oo dz-cn “RASJ'VC’CQ(cud)2 c 6 (is guyr) (13¢ij > where p is a non-zero integer and vc d = (* *1 c d)6 AJF'. 9 The sets Guyr) and fi 2), we could rear- range the series. We would get easily the following results: 1) G(z,W3AJ,V‘.u) is a modular form. That is, it satisfies the functional equation (1.3) G(VZ{V:A33 roll) = ’U(V)(CZ + (1)2 6(29’15A31r :l‘) for each V = (* *\ c d)6 F'. Furthermore, it satisfies the required regularity conditions. 2) We would obtain the Fourier series coefficients given in (6.10). 3) we would obtain the inner product formula given in (9.2). In order for us to obtain these results we must rearrange conditionally convergent series. In doing so, we must rely on: k) a Rademacher lemma: and 5) a non-trivial estimate on the Kloosterman sums -u- (1,l+) wc(n+/(,p+xj)=ZIE(A31vc,d)e[(n+k)d/c +(p+KJ)a/C;l.3], defié(AJDI—) namely, 8 Wc(n,u) = O(|cll/2 + ) 5’0 where the constant in the C9-symbol does not depend upon n. Our main result is this: ‘1; r'ig a subgroup of finite index ig_l"(l), and i£_the Kloosterman sums have the re: quired estimate then 1), 2) and 3) are obtained. In 598 we give a series of examples of groups l. and multipliers systems’U'for which we are able to prove the validity of the Kloosterman estimate. They include: F = Y’(l) and all six multiplier systems/U'of dimension -2; r'= V'z, the unique subgroup‘of index 2 in i—(l), and all nine multiplier systems: and f‘o(q), q a prime of the form km + l and the multiplier system which depends upon the Legendre symbol. In §>9 we return to these ex- amples and calculate the dimension of the space of cusp forms belonging to these systems. Here we use results of Petersson. The proof that the G of (1.2) satisfies (1.3) depends heavily on our Rademacher-type lemma. Roughly, this lemma states that the series (1.2) can be summed over expanding parallelograms centered at the origin. This is somewhat -5- analogous to the standard way in which one proves the con- vergence of the weierstrass 65-function. To some extent we follow Lehner [6] in proving our Rademacher lemma: however, since in general r.will have more generators than T'(l) we need a more comprehensive lemma. M. I. Knopp has developed other extensions of the original Rademacher lemma ([5] , [5.11): still others are in the process of publication. For the estimate of the Kloosterman sums we rely on the researches of Petersson [ll]. Petersson proves the theorem: if r-is a congruence subgroup and’U’an abelian character on V which is identically l on some principal congruence subgroup T'(N) Cl’, then the Kloosterman sums (1.h) have the required estimate. In § 8 we give an elaboration of his proof so that the interested reader may see the neat way in which the complicated sums (l.h) are reduced to the classical Kloosterman sums. We require the estimate of the sums (l.h) both in the proof of the regularity of the functions G of (1.2) and in the proof of the Rademacher lemma. The above results are not all new. Petersson has obtained them in [11]: however, his method of proof is entirely different from ours. He uses the Hecke idea [h, pp. h68-h76] of introducing a convergence factor ‘cz + dl's, s > 0 into (1.2). He then takes the limit as s -> 0+. Our method of rearranging conditionally conver- -6- gent double series was first suggested by Rademacher [13]. In some senses our method is more natural since it follows the proofs for dimension -r < -2. 2. Preliminaries In this section we give the definitions, notations and results which are needed for this investigation. No attempt has been made to give a reference for every fact which is stated, but rather, to give references for only those results which lie deeper in the theory. Almost all of the results for which no reference is given can be found in Ford's book [2]. We shall be concerned with infinite groups l-of linear fractional transformations where a, b, c and d are rational integers and ad - bc 3 1. These transformations map the upper half plane '7+ = {z : In 2 > 0} onto itself in a one—to-one manner. The groups we are considering will have the further prop- erties: (i) for every point p on the real axis there is a sequence of different substitutions w = Vnz and a point 20 such that the sequence wn = Vnzo accumulates at p: (ii) the same statement does not hold for any point p 574. Groups for which (11) hold are said to be discontinuous in l+-. Groups for which both (i) and (ii) Ihold are called horocyclic groups (they are also called Fuchsian groups of the first kind and Grenzkreisgruppen -7- -8- in the literature). This terminology is not used exclusively for the case in which the region of discon- tinuity is the upper half plane 74 . Let the letters I, U, S, V, M, AJ denote the following two-by-two matrices (written in one line with a vertical bar separating the first row of the matrix from the second) 1 = (1 0| 0 1), U = (1 1| 0 1), (2.1) V = (a b \c d), S = (0 -l ‘1 0), M = («.5 ‘Y 8 ). and AJ = (aJ bJI cJ d3) where all the matrices given above are real unimodular matrices. Further, for any real it , we write (2.2) U“: (1) | o 1). Also, put -v = (-a, -b |-c, -d). With each of the above matrices we can associate a linear transformation, namely (2.3) w = v2 3 41.1.1). Notice that V and -V correspond to the same linear transformation w = Vz. Thus,to any group T— of two-by- two matrices there corresponds a group I: of linear fractional transformations. -1 may or may not belong tol— . However, since our interest lies in the groups of linear fractional transformations we may assume that -9- —I €T—. If it does not then we merely adjoin it to F’ without affecting I" . It follows that F: F/ {1, -1{ . There should be no confusion when we let V stand for the matrix as well as the linear transformation. One uses the same terminology for r-as we did for F': namely, r'is discontinuous or horocyclic if and only if F is. Two points 21 and z2 é‘Ft are said to be congruent or equivalent with respect tol— if there is a V6 VT such that V21 = 22. A fundamental Eggigg for T". R(i—), is a subset of?! which satisfies: (1) R( F) is a non-empty open set: (2) no two distinct points of R(T') are equi- valent: (3) each point of ?+ is equivalent to at least one point of the closure of R(l_). A fundamental region for r'can be chosen so that it is bounded by circular arcs and straight lines called giggg. A Eggggx of a fundamental region is the common and point of two sides. In our case the fixed point of a parabolic element in F' lies on the real axis and is called a parabolic vertex or parabolic cusp. Linear fractional transformations are classified as parabolic, elliptic, hyperbolic or loxodromic. We give the same classification to their matrices. We shall assume that a fundamental region R(l_) has a finite number of sides. This is a restriction on F'. A consequence of this assumption is that the groups we are considering are finitely generated. There is a -10- fundamental region R([_) in which each parabolic cycle consists of a single vertex: we shall always choose this fundamental region. Since there are a finite number of sides there are a finite number of inequivalent parabolic cusps. Let this number be c (l’). The modular group, F'(l), consists of all matrices V = (a b [c d), a,b,c and d rational integers and ad - bc = l. The modular group is a finitely generated zonal horocyclic group discontinuous on ?+ . A discon- tinuous group of real matrices is said to be zonal if it contains a parabolic element fixing 00. The substitutions S and U generate F-(l), and U is the parabolic element fixing 00. A fundamental region for the modular group is the set of all z = x+ iy 67+, y) 0, such that -l/2 < x < 1/2 and lzl > 1. Denote this fundamental region by R(1). R(l) has a finite number of sides. Rankin [1h] proves that if ['* is a subgroup of finite index in.r then T" is horocyclic if and only if F is horocyclic. Further, he proves that a fundamental region for T'* has a finite number of sides if and only if a fundamental region for F'has a finite number of sides. As we stated at the outset we are interested only in sub- groups of the modular group. If we add the condition that the subgroup should be of finite index, then we will know that it is horocyclic and has a fundamental region with a -11- finite number of sides. We reiterate, r-is a subgroup of finite index in the modular group. R( F) is a fundamental region for Fwith a finite number of inequivalent parabolic cusps p3, J = 1, ..., a (l’). We may choose A365 r (1) so that -l J modulo F'. A coset decomposition for r‘(1) modulo F’ will be A 00 = p3. Then the AJ do not belong to the same coset G" 7‘3 r’(1)=U U 1310‘“!- J=1 k=1 where, of course, the integers 7\J depend upon r.. 'AJ is sometimes called the gigth of R([-) at pa. ‘1: is determined as the smallest non-negative integer so 1 that P3 = A31 U 3 AJ E r'. PJ is parabolic and fixes p3. P3 generates the cyclic group of all transformations in l" which fix p1. We now remark that if v is any real two-by-two unimodular matrix and r'is a horocyclic group, than V r‘ v'1 is also a horocyclic group. If, in addition, 1on then r possesses a parabolic element which fixes V- V F'V'l is a zonal horocyclic group. In particular for our choice of f_<: r'(1), we know that Ail. A31 is a zonal horocyclic group for j 8 l, ..., a (r'). A very special class of subgroups of the modular group are the principal congruence subgroups of level X consisting of all those elements in F'(l) for which -12- V -,3 I (mod N), where the symbol 5 denotes element-wise congruence. A congruence subgroup G of level N is a subgroup of [—(1) such that F'(N)CZG = 3301). -13.. where F007) is the complex conjugate of MW), and, further.) (2.6) AMI) = rU(-I) = l. The multiplier system (V (F ,-2) induces a multiplier ar(v r v'l, -2). defined by system on V F' v'l, (U. ' -1 -1 (2.7) (U (M') = flf(M), M' = VMV 63 V F'V . We will be particularly interested in the case in which v = A1. In this case we write (113 a (UTAJ 1‘ A31, -2). Let p3, J = l, ..., a (F) be a cusp of R(l"); we shall assume that p:l = 00 and A1 = I. 7\J was defined to be the a smallest positive integer so that P3 = 11le 3 113 (5r. Write “AJ = 7. (13,1’ ), then this function satisfies (2.8) )3 = Na 1‘) = a (1. aJr 1'1). 3' J In particular 7\= X1 7\ (I,l—). Since [(WPJ)! = l, we choose K1 so that Define ((3 = K (13m), then - - -1 (2.10) «3.. «(13.0- «(1, AJFAJ ). In particular let K = K1 = K (1,1’). An automorphic form F(z) on r of dimension -r = -2 belonging to the multiplier system 41’ is a meromorphic -1h- function on? which satisfies the transformation equation (2.11) rm) = (U(V) (cz + (1)2 F(z), for each V a (a b | c d) e I— . One measures the behavior of F(z) by its local variable expansion. Furthermore, F(z) must be meromorphic at each cusp pJ of the funda- mental region R(I_). A local variable for the cusp ‘1 P3 = A: 00 19 8170a by 8(AJa/’AJ). F(z) is meromorphic at pJ if it has an expansion (2.12) F(z) = (ch 4- d3)"2 2? an(F,A3, r)e((n+I(J)AJz/7(J) n= 3 where s is a finite integer. The set of everywhere regular automorphic forms of dimension -2 for r— and/U' forms a complex vector space. By everywhere regular we mean regular on 7+ 4' 8 ‘H U 0), where 6): {A’loorAC—Z F(l) We denote this space by' £’(l_,-2,QI). A subspace of this is the set of all forms which vanish at each cusp of the fundamental region. This is the space of 2232.22523 and is denoted by §+( F ,-2, ’0'). To prove that F(z) is meromorphic at a cusp pJ it is sufficient to show that F(z) approaches a definite limit as z -> pj through values lying entirely within the fundamental region.* ——_ * Lehner, The Fourier coefficients...III, Mich. Math. J., p067. -15- The 1 transform of F(z) is defined to be (2.13) Fv(z) = F(z)| v'1 = (-cz + a)"2 F(v'lz), 1 where V- = (d,-b |-c,a). It follows that Fv(z) belongs to<§7(Vr‘V'1,-2,KU3 where ru' is the multiplier system on VFV'l induced by-v’onl’. Furthermore, (2.1%) Fv(z)l V = F(z). and if A3100 = pJ is a cusp for R(l_), then (2.15) FA (2) = if? an(F,AJ,F')e((n + «3)2/23) J n=s where an(F,AJ, F) is defined in (2.12). We define the following sets of integers :(Ajsr) ={C33V6AJF9 v=(oe\Co)} a oO(c,A,r)={d:3V€Al—, V=(..‘cd)7] s (2.16) J J €(Arl‘) = {dc J3(c,Aj,l—) : d6 [0,c7\]}s QCMJJ‘) = {a :BAVEAJF, v = (a . c J. ae [MN] 3. where [0,c7\] is the closed interval between 0 andich (note that c may be negative), [0,c'hJ] is defined in a similar manner. The following relation is valid 00 (2.17) oo(c.a .r) = U {d +clq : de 00(1) .mi . J gas-m c J -16- which follows from Vc’d = (. . c d)Ei Ajr‘, ce:C’(AJ,F'), dfi d2(Aj.l_) then so is Vc’qu = (. . c,d + cq7\)é AJF. In the course of our investigation Kloosterman sums (2018) Wc(n + K’AJ, [1 + K3) 3 Wc(n,p) (+ K) = E (U(A-1V )e(12:;£lg + _£___1_: ) d6 000(A‘11r) with vc,d = (a b |c d) o for fixed p . In sectinn 8 we shall discuss situations in which we can make such an estimate. We include finally the Lipschitz formula [1,p.206]. If t is a complex variable for which Re(t) > 0 and either 0 < u < l, g > 0 or u = l, g > 1, then 00 8 - - (2.20) $31)... > (m+u)g 1 e(it (m+u)) = E e(nu)(t+ni) 8 (3) m=0 n=-m ‘where i"(g) is the gamma function. Any further introductory material will be dealt with in the course of the text. 3. Convergence and Regularity In this section we prove the uniform convergence of the series introduced in (1.2) on compact subsets of 7% . Thus, these functions are regular in ¥4 . The method follows ($3 of Lehner's paper. Consider the series e((p+ /< )V 2/7\ ) um i I: -r‘ ”—4- c=-m :-m (LE-(A1 Vc,d)(cz+d) C€§(A3,l_) d676(c,Ajsr) where Vc,d = (a b l c d) 6 A31”)- ATM”? and the sets é?(AJ,T‘) and 1I(c,AJ,F') are defined in section 2. We assume u is a non-zero integer. The double series (3.1) does not converge absolutely and for this reason we must define in what order the summation is to be carried out. First, however, we show that while Vc,d is not uniquely determined by the conditions cc mix-1m), dc- flc,AJ,l—), that is, by its lower line 3c,d} , the terms of (3.1) are determined uniquely by these conditions. Let Vé’d be another matrix in Ajl’ with lower line it, 3 , then vc,d = Um v; 6. However, vc,d = 13M, vé'd = AjM', with M, M'ezr‘. Thus 13M = UmAJM', and conse- quently A31 UmAJ = MM"1€ST'. This is a transformation fixing p1, and hence, it must equal P?. In other words -17- -18- k7kj Vé d' Substituting 9 m = k‘hj. This proves that vc,d = this into the term of (3.1) determined by fc,d( , we find It} 8“)” ’3’ch 2/7xj) _ e((..+ «3m 31);“, z/iL) rv(A31 Vc,d)(cz+d)2 - -l 7M’k t 2 (VIA; U c vc,d)(CZ+d) e((u+ KJ)(V;,d 24»): 21V“) 5113):. -1' 2 ’V(A1 U Agrv(A6 Vc’d)(cz+d) k‘x since U Jw = w + k'kj. From (2.9) we see that k7x mun U A3) - UNP’J‘) - out an). Thus the term of (3.1) determined by Ic,di becomes upon simplification 9((l‘+ K3)Vé,d Z/RJ) AI(A31V;’d)(cz+d)2 Now we introduce for the c #’0 the auxiliary series e(( + K )V z/'A ) (302) H(c,z) = i +1 C,d 1 (1,500 was Vc,d)(cz+d)2 65-00(09A31r) which for each c e : (A3, F) is nothing more than the inner sum of (3.1). In the course of our exposition we shall prove that this series converges uniformly on com- pact subsets of 74 . Let the series in (3.1) be understood in the sense of -19- (3.3) 5A3,Ie((“+K)z/7\)+ lim :H(c.z) + 11m H(c,z) K->°°c=-K - K?-->oo¢:_,1 cedf’éajJ) C(CZCAJ.F) where 2 if A A I (30"?) SAJsI 3 { , J l , 0, otherwise. If both of the limits in (3.3) exist simultaneously, we shall define the expression (3.3) to be G(z,rU,AJJ_,p). The objective of this section is to prove that both limits do exist uniformly for z belonging to compact subsets of 7+ . If AJ = I the terms of (3.1) corresponding to c = 0 arise from d =.: 1 because c and d are relatively prime. Thus, there are Just two terms and we can choose Voti:1 =,: I. This will account for the first term of (3.3) when we show that 065013, F) if and only if A1 = 1. Suppose 0 €C(AJ, F); then there is a V (5 A1 F with V = (a b| o d), which implies, a = d = 3; 1. That is, Ube AJF. We can write 1'51 = M'lu'b, M e F and so A3100 2 M’loo. -1 ’1 Then pJ = AJ 00 is equivalent to 00, because MAJ oo = Mid—loo = 00. Because of the way we chose the Ak’ this can happen only if A1 = I. The converse is clear. -20- The following estimate of \cz + dl is essential. (3.5) \cz + dl _>_ (di sin 5 , o < S: arg. z < 17. Kli Fig. 3.1 In Fig. 3.1 we see that lcz + dl is the length of one of the sides of the parallelogram PQRS with vertices + ldl9 : [cl z. For, \cz + d\ = \cz — (-d)\ is the distance from cz to -d. Thus \cz + d\ is the shorter side of PQRS or longer than the shorter side. \d\ sin8| is a leg of a right triangle which has the shorter side of PQRS as hypotenuse. In case 2 lies in the second quadrant we replace 8 by U -8.. The degenerate case is excluded since z 6 H . Also, . 1/2 (3.6) lcz + d5: ((cx + d)2 + c2y2§ ,2(CIY. z = x + 1y. We split H(c,z) into the sum of two series. For c X 0 we have Vz = az + b -21- Let us define for c€Q(Aj,F), c y! 0, (( 4-K) A ) [-( 4-K )/ C(cz+d)]-1 (3.7) H1(c,z)=ie u 3a/c 3 {e n 3 7(3 } as-..) mifvc d)(cz + d) and 6((1H' )8/0 7\ ) (3.8) 112(c,z) = i «1 J -l d=-oorU1Aj Vc,d)(c z + d)2 d e 0(3(c,AJ,F) where vc,d = (a b\ c d). Note that formally R(c,z) = 81(c,z) + 32(c,z). Once convergence of H1 and H2 has been obtained, we will have this result. We obtain estimates of these series which involve c. Expand the second exponential in (3.7) to obtain e(( m )a/c a )(-21r1)m( +« )m (309) H1(c92) = i : +L—J p ...g— . =-m Ina-1’1“!) vc,d)( 7‘30)mm! (czit-d)m d ed)(C.AJ.F) This double series is dominated by f 1217)!” (pi-1| m m mm =-oo mal lei J m! (cz + d! ”+2 de 00’(c.AJ.‘—) Using the estimates (3.5) and (3.6) we see for d i 0 |cz+dl -(m+2)$ lc[-(m+2)/2y-(m+2)/2‘d\-(m+2)/2(81n8 )-(m+2)/2’ and if d = O -22- -(m+2) -(m+2) y-(ms-2). [oz + dl s Icl With these results we obtain for our dominating series if gay)" (pi-ll " “:1 m: c2m+2 y2m+2 m=1 d=l + 2: 2: (2n) UNI)" m! kf3m+2572y(m+2)72 d(m+2)72r(31n “mi-272 ‘- ‘°”'2 HAL") {am 2‘? ”‘7' m=O ysin 8 f—r‘ d32 d=1 Therefore, (3.1a) Ipnl(c.z)l 3 (cy)‘2 exp(21r mil/y) -5/2 ' -1 21r| 4-1)] + C lcl (y sin 3) exp[f___I__—y—8Lr;g where C is a sufficiently large constant independent of z. When we say that a series converges absdlutely uniformly we mean that the series of absolute values converges uniformly. We have proved that H1(c,z) converges absolutely uniformly on compact subsets of 7+ , actually for y,2 yo 5 0 and O < ix] 5 x0. Thus, H1(c,z) represents a regular function in74. -23- Note that H2(c,z) of (3.8) correSponds to the missing term m = 0 in (3.9). The dominating series for H2(c,s) is i 1 . da-oo \cz + dli d608'(c,AJ,T') Using the results (3.5) and (3.6) we find if d X 0 lcz + cal"2 5 d-2(sin 5 Y2, and if d = 0 lcz + dl'2 5 c.2 y-Z. Thus, 132‘ 3 (cy)'2 + 2 (a 51:13)“? . d=1 (3011) |H2(C,Z)‘ \< (cy)-2 + unul-z—T o 3 sin 8 We proved that for \x‘ $_xo, y‘z yO > 0 the series H2(c,z) converges absolutely uniformly. H2(c,z) is a regular function in ’H . Now that we have established the conver- gence of H1 and H2 we can assert (see lines following (3.8)) (3012) H(C,Z) = H1(C,Z) + 32(csz)o The estimate (3.11) is not good enough for our purposes since we will want to sum on c. One first proves that the terms of H1 and H2 are uniquely determined by the lower line gc,dfl of vc,d' ‘The proof is almost identical -2u- to the case considered at the outset of this section. We make the choice of the a of Vc d = (a bl c d) unique. We ' k1 saw that V = U 3v' , where V. is another matrix c,d c d ng 9 with lower row and} . That is, a b) (1 k)1>( a' b') _ (a' + ck); at) V = 8 - , c,d c d O l c d c d By choosing k properly we obtain ae [0,c )3], i.e. aeabuyl‘). Now dividing d by c7\ ,d = QC) + d1 where dle (Denim). Then _ ab 3 a * lq7\ .. with ce Earl—L dlewcuyl‘) and ae acmyr). q7\ Using these results and (2.17) e((,u+ Kin/c 2(3) H2(c,z) = Z i -1 7i (1 d1€ dZULJJ’) q=-oo MAJ vc,d1U )(cz+d1+c7\q) e((u+KJ)a/c 15) >4: eC-qk) (cz+d +c7\q)2 2 -1 d eagqu) “I”; Vc,d ) q=-m where we have used 1//U(U(fl ) = e(-q/~1). _The order of summation is immaterial because H2 is absolutely conver- gent. Applying the Lipschitz formula (2.20) to the inner sum of the above series, valid since g = 2, we find, whether K>Ooru= K =0: -25- i e(-QI<) 42-: {'21}: 0° e(QK) q=-oo(cz+d +c 3\ Q) c 7\ q=_m(-1(z/Q\ +d/c>\ )+q1)2 2 if? (n+ K )e((n‘“\ )(z/X ‘ d/c>\ )) n=0 where in (2.20) we identify t = -i(z/7\ + d/cA ). Hence, 6((“4' Kj)a/c x3) _ 2 H2(c,z)={ _1 . 32—23%} . deVOc(AJs r)(U(AJ vC,d) c 7‘ 00 {Z (m x >e(\ ) } . e[ (11+ ((1)8 (hi-K )d 1 -1 {d6 00303. F) ”I”: vc,d) 2 (3.13) = (fig-7:?) (n+ K ‘ e({n+ K 12/ A )' Wc(n,p) n: 0 where we have interchanged the order of summation of the finite sum and the infinite sum and have introduced the Kloosterman sum (2.18). The above interchange of ~26- summation is valid because of the absolute convergence of the double series involved (recall that cacuj, F) is finite for fixed c and 3). At this point we derive an estimate for 32(c,z). The series (3.13) is dominated by 2 . 35.)? E (n+ K) exp(-21r(n+ K)y/7\) |Wc(n,l*)‘. c n=0 Now we use the estimate (2.19) for the Kloosterman sum and the fact that 0 S K.< l to obtain a dominating series 2 .3121. : (n+1) exp(-21r ny/m) CE MIL/2+2 . c n=0 Thus, C E (3.1%) Pawns). S. W i (n+1) exp(-21rny/7\) n=0 -2 .-. cE lcl 3/2 *5 (l - e'ZW/M . This is our desired estimate involving c. It is now easy to see using the estimates (3.10) and (3.1%) that the series : H1(c,z) and i Hz(c,z) cs-oo ca-oo ¢€§(A , r) c€€(AJsr-) egoJ ch converge absolutely uniformly for y‘z yo > 0, ’x“$,xo; we proved that H1 and H2 are regular 1:134 . Hence -27- the above sums are regular in IL . We have, moreover, from (3012) :1 |H(c,z)l g : ‘H1(c,z)‘+ ZR: |H2(c,z) c=l and¢€€(AJsr—) c..10(AJ,r-) C€G(Ajsr) mix (H(c,z)[$ Z]: I31(c,z)l + : IH2(C.2)| 3 c=-K =-K c;.C(AJDr-) C€;(Ajgr—) céé(AJD[—) therefore, the limits in (3.3) exist uniformly for |x{ 3 x0, y'z yo > 0. This completes the proof of the lemma. Lemma 1: The functions G(z,n;,AJ,T-,u) defined in (3.3) are regular in )4 . Furthermore, we have the expressions (3015) Gl(zs/U9A}srsfl) 3 8A 19((IH' K. )z/Z )+: R(csz)s J, cs-oo 06%(A‘1: [— )scflo and (3e16) G(z,/\I,AJ, r3“): SAJ,IC((.L+ K. )a/%) + i 31(C,Z) c=-oo + f H2(c,z) e c€g(AJ,F),c,¥o =-oo Ce £(AJ, r )scylo The three infinite series appearing in (3.15) and (3.16) are absolutely and uniformly convergent in each compact subset of 34 . H(c,z) is defined in (3.2), H1(¢.8) ~28- in (3.7) and 82(c,z) is defined in (3.8). For later considerations we discuss 31(2) defined by the series H1“) = i . i e((|r"/ 0,lx‘ 5 x0; moreover, we get for the sum of the series, 31(2), the estimate (3. 13) I31“)! 5 Cy 2exp(21rlu.4-1| /y) + C(ysin$)1exp[w] Mysingj where the constants are independent of z. h. The Rademacher Lemma We now come to the main tool of this paper, a Rademacher type lemma, which allows us to rearrange certain conditionally convergent double series. In part we follow the method of Lehner [6, § k]. Some preliminary investigations will be required before we can state the lemma. By a lattice point for AJT"we shall mean an ordered pair (c,d) of integers obtained from the lower row of amatrixv =(ab|cd)€A F. Leth.T')be the ed .1 1 set of all lattice points for AJF': (k1) (NAVY) {(c.d): 3 V = (a b \c d)6 Air) . Let ”(K = {w = u + iv: \u\< K, \v) < K) and (M2) Oxurr‘) = 0(AJ,F)fl Xx . Let )n consist of the following matrices M = (on at Y we I' : (h.3) M = 1; (MA) Y=1, ogoi,8 <7\ and 084' 82>O; (M5) Y>1, o 0 as can be seen from the conditions in (H.5) along with 0&5 - {3! = 1. Each V 6 I" has one of the following representations: (k6) v = _+_ U“ MUn)‘ with MEWZ, or, possibly, if S = (0 ~11 l 0) e F 0+.?) v = 1 UM“A so"X . The representation for each V e l- is essentially unique. To prove this result let V = (a bl c d) € V be an arbitrary element. We may suppose c 2 O, for otherwise -V has -c > 0. Now consider U-mX VU‘nx: (a-mc'A *1 c, d-nck ). If c f 0 there are unique choices of m and n so that 0 g a-mc7x < c7\ and 0 g d-nc'A < c7\ . -m7\ vu'n7‘ . If c = r > 1, then o<= a-mc7\ and Let M = U S: d-nc7x satisfy the inequalities of (#35) (neither at or 8 is 0 since (on?!) = (Y,5) = 1): thus, 145W). If c = Y = 1, either both a and d are integral multiples of? or this is not the case. In the first instance a - mc7\ = 0 and d - nc?\ = 0, hence, U'mxv U'n)‘= S = (0 - l \ l 0). This case leads to the representation (h.7). 0n the other hand, if a and d are not both multiples of 7\ , ' M a U-nfl VU'nzem since the inequalities of (MM) are satisfied. Finally, if c = 0 then a = d = _4; 1, hence, v = 3 0M . -31- We can think of Moo J 41(A? wd)(cz+d) d=-oo ea,» «3)a/c ’AJ) K“>°° 4f(A3 Vc,d)(cz+d) (csd)€O-K(Ajs r )M where vc,d = (a b \c d)00 ’U(A31Vc’d)(cz+d)2 (c,d) 6 0K”), r’ )M 63.00 We have shown that the series in the left member of (h.lk) is absolutely uniformly convergent for yIz y0 > 0. Further, for fixed M = (a pl 1 S) 6m the 2:: J H2(c,z) lcl >(d + Y)K series can be made arbitrarily small by choosing K sufficiently large. This is because 0! + Y is definitely positive by our choice of )n , (k.3), (h.h) and (h.§). Moreover, -3h- the sum (Ot+7l)K:'1 c=(01 4- 1)K-1 ‘ (this) Z H2(c.z) = Z, i a“: “we 73)2 j .1 ' .1 ”(83 Vc d)(°2+d) =-(o<+1)x+1 6"” ' c=-(0< +Y)K-l is an absolutely convergent double series for fixed M é7n,and K. This can be seen by using the estimate (3.11) obtained by taking the series of absolute values of terms of H2(c,z) and then performing the finite sum on c. We shall want to rearrange this series, but first some new notation will be introduced. For fixed M<:)n_define the regions-Q1 = 111(u,v) 5331 = $331(usV), i = 1,2, as follows: £1 = {(u,v): (If-00K 5 u < (THOUK, otv - Bu 2, K), 512 = {(u,v): -(°‘+V)K < u < ($00K, 3"? " 5“ 2 K? s .031 = {(u,v): «wax < u g -(x-um, ow - Bu 3 «L _fiz = {(u,v): -(V-d)K < u < 01+X)K, 1v-- Eu 3 -K} , The cases where d = O and M = I merit special attention. Iro<=0setfllan'1=¢. ITMaI,setIl2=—Qz=¢. The regions are given in Fig. k.2, we have used the same choice of M as in Fig. h.l. -35.. “(1' ((stT)Kv(<+%)K) ,/7 ' [/4 //, 4”?“ *‘ Ja/ a __ w - u k” _{11 (~(NK)K,—(8+§)K) Fig. h.2 Define (this) wim = 319-415 , ”1“” = 2: $3315 . (cz+d) (cz+d) 111(c,d) 431(c,d) i = 1,2, where (h.l7) g(C.d) =FU(A;1VC d)e((u+ K3)a/%'Zj) for (c,d)e C9(AJ,r—). The summation conditions indicated in (h.16) mean summation is performed over all lattice points for AJT' which lie in the regionfl.1 or .Il'i, If 0t=OsetW1=Wi=0. IncaseMzIsetw2=w§=o. One could check directly, using the methods of section 3, that these series are absolutely uniformly convergent for y'z,y0 > 0. Their convergence will come out in our development. Notice that the regions .01 and—EL'1(i=1,2) -36- are symmetric with respect to the origin. This implies (ma) W100 = w;i )g(c,d+c?t) = e(dIa/c?t )g(c,d). 97(c,d) is periodic in d with period C7\. . Therefore, it has a finite Fourier expansion ¢(c,d) = Z: Bke(kd/cl ), Bk = llcTA— :43(c,d)e(-kd/c'>\). k c7\) (b.22) “cm where in each case the sums are extended over a complete residue system modulo c'A, say 0, 1, ..., lcl7\ - 1. From the first equation of (k.22) and the definition of Cf (c,d), (ll-.21), we see (M23) g(c,d) = Z Bk euk- mam). k(c7\) From the second equation of (h.22) and the definitions of (70(c,d), (h.21), and g(c,d), (ml?) and (1+.l7a), we obtain \CM -1 (than) Bk - \cz-Ill: d2 J’VUJ Vc’d)e((p.+ KJ)a/c ’AJH-ki-IOd/cM =0 The summation conditions mean d 6 flcm, l.) and 0 g d < lcl X . However, the above sum is periodic in d with period loll , thus, the finite sum in (M210) is nothing more than the Kloosterman sum of (2.18). (”025) Bk = -l-:ll- wc(-k+ ll sAJsll+ K3). -39.. If we use the extended definition for g(c,d) in (h.16), we can drop the conditions on the summation variables symbolized by the J on the summation sign: that is, we no longer require c Q g(AJJ’) and d6 05(c,AJ,r ). Now insert for g(c,d) in (k.l6) the finite Fourier expan- sion (h.23) to obtain (0‘ ”OK-l lo! 7\ -l - 9((k- Ac )d/9_7‘) (ll-.26) W109 "' Z Z Bk Z (cz+d)2 c==()(-0()K k=o atd-Bczx (LOOK-1 (CM --1 e( (k- KBd/c A) (“027) W (K) = B 2 c=§(:r+ot)K-l ;0 k Z (CZ+d)2 YdPXcZK The dependence of the Bk on c has been suppressed by the notation: however, it is clearly present as is shown in (k.2h).. It is in the above form that we will make our estimate on W1(K). In making our estimate on the inner sums of (h.26) and (h.27), we will want to identify two cases. First, we shall suppose d may take small values and c is bounded away from 0 by a multiple of K, and secondly, c may take on small values and d is bounded away from O by a multiple of K. We are excluding the case that ‘both c and d can take small values. That these two situations, and only these two situations, are realized is a property of the class'MW. The proof of this state- ment is deferred until later. -ho- Define (”028) T(k,C,K) = i 9((k-K)d/C7\.) d=QK (C2 + d) where Q = Q(c) is defined so that QK is the lower limit of summation on the inner most sum (on d) in the equa- tions (h.26) and (b.27) for W1 and W2 respectively. Notice that Q(c) depends upon M. We assume that either: (I) -oo< Q(c) < + 00 with ch> BK, (h.29) R a positive constant: or (II) 0 < Q(c) < + 00. These two situations are not mutually exclusive. In the proof of this lemma we always exclude c = 0; this comes from the fact that the summation variable c in the left member of (%.l3) is not 0. Notice further, that in (I) d #’o since Icl > 1 (for sufficiently large K). and (c,d) = 1. We intend to make an upper estimate for T(c,k,K). This estimate will be carried out in four stages listed below: (I)1 situation (I) with k = 0, (1)2 situation (I) with 1 5 k g ld7\ - 1; (II)1 situation (II) with k = 0, (II)2 situation (II) with 1.3 klg lclh - l. (n.30) In order to carry out this estimation we introduce some preliminary material. Let Sd = E e(o(k-K)t/c7\ ) t=0 -hl- witha=_4_-l. ThenSO=landford21 (10.31) 8d = : e(a(k- K)t/c7\) g 1'e(°(k-’t)(d+l)/c7\) t=0 1 - 9(a(k-K)/c 1) provided It - K i 0. Using the inequality sin n x 2 min. l2x, 2 -2x l for 0 < x < l, we find that for k and K in their ranges (see (h.30)) and k - x i o lSdl _<_ {sin “gull-15 {min[2 l(k-k)/c')\l ,2-2l(k-K)/c7tl]l-1. Thus, $.32) lSdl S loll /2 llk-Kl'l + [M1 - lk- Kl I’ll . This inequality is valid for dlz 1. Under the conditions on k and k the right member of (h.32) exceeds 1, there- fore, this inequality still holds if d = 0. Recall the estimates (3.5) and (3.6) for Icz + dl . Let w=w(z) = min. lsin 5', yl where 0 < S. = arg. z < w . Combining these estimates (1533) lcz+dl 2 ldl sins '2 ldlu) and lcz+dl 2 lcl yz lclm, we conclude that for each 11 with 0 5 7L 5 1 any.) lcz 4- dl 2 Id1 "1 lat) . We continue with the estimation on T(k,c,K). (I)l Suppose we are in case (1)1. Then with 92 = 5/8 we get -hg- (M35) lT(0,c,K)l g i lcz+dl'25_ L52 ldl-b'A lcl'3/1+ d=QK d=QK s :w'2 ldl‘5fl‘lcl'3/l‘ < c lcl'3/1”, =-m C = C(z) is a general positive constant depending on the parameters indicated. (I)2 Suppose we are in case (1)2. In order to use the preliminary material uniformly we decompose the sum T(k,c,K) into two series so that in each case the sum- mation index (1 will be positive. If Q(c) < 0, write T(k,c,K) = T1(k,c,K) + T2(k,c,K) with - T1(k,c,K) = (cz+d)”2 e((k-K)J/c7\) d=QK - K = (oz-d)“2 e(-(k-k)d/c 7x) d=l *‘3 H I and CO T2(k,c,K) = Z (cz+d)-2 8((k'K)d/C7\.) d=QK d‘Z]. T2 In case Q(c) > 0 define T1 = 0. In T1 and T2 we replace the exponential by Sd - Sd-l’ Then -QK T1 = Z (Sd - Sd_1)(cz - d)-2 d=l with Sd defined in (1+.3l) for a = -l. -h3- Thus, _ -I T = S [(cz-d)-2-(cz-d-l)'2] + s (cz-QK)'2 1 d -QK d=l _2 -So(cz-l) Therefore, -QK-l lTll 5.2:: \Sdll'lczwdllcz--d--lll"1llcz-dl"1 +lcz-d-ll'll d=l + lS-QKllcz’QKl-2 * lSollcz - ll-2 Using the estimates (n.32) and (“.3“) with 72.: 1/)+,o,1, lTll S llCIA/b ( lk-«Fl + {Icy} - lk- KlJ-1)l' -QK-l l}: (2 w3 d(d+1)1/‘* lcl7A)-1 + 2w'2 52 l, d=l hence, (1.36) ”1! g llk-Al-l + [ (c1) - \k- ml]'1l' c: Icl’3/‘*. By similar methods an upper estimate of T2 is made. Let Q' = max qu, ll , then with o = 1 in the definition of S d T2 3 : Sd[(¢2+d)-2 - (cz+d+l)'2] d=Q' -Sq._1 (cz+Q'+1)‘2, We see that lT2l S {OCH /2)( lk- Kl-l +[ loll - lk- Kl]'1) } a) l: [ km“ l “*‘ml VII l°z+d|-1+|°z+d+ll "11+ l¢z+Q'+1l-2l. d=Q' -hh- hence, (M37) lT2l < lit-(r1 +[ let) 'lk'Kl1-1}C°lcl-3fl+ . Combining the results of (n.36) and (n.37), (M38) lT(k,c,K)l < c lcl‘3/‘+l “Ml-1 . [ lei) -lk- m-il for the situation (1)2. Now we turn to (II), namely 0 < Q < + co. (II)1 Let the conditions of (II)1 prevail. Then as in (“-35). lT(0.c.K)l < 2:: d'S/u lcl-3/h (n72. d=QK ' Using an integral estimation for the series on d, we find (v.39) lT(o,c,xl < clcl’3/h K-l/h. (II)2 Now turn to case (II)2. Then as before T(k,c,K) = <¥L z;_ Sd [(c2+d)-2 - (cz+d+l)'zj d=QK -sQK_1 (cz + QK)”2 with o = l in the definition of Sd‘ Making the usual upper estimate, q ”(hunk lid/A /2 (ht-«1’1 + I M) - lk-Kl]-1)l l3: n-z d'5/‘+1c(‘7/‘* W-z (an-w a M}. d=QK Thus, (‘+.‘+0) lT;—-(n) C 'where E represents a summation over those c in our -I c decomposition for which (I) holds. E ( ) is defined , II 'by analogy. Then c -h7- -5/‘+ + 26 _ E _ lw1CK)l S :(I)C£lcl + g(II)CE kl 5A*2 K 1A 5 CEZlcl-SA +2E+C£K-1/h if lcl-S/h + 2?; lcl>RK ='°° We place the restriction that o < 2 a < l/h, then, vim = 0061/“ +26) + 0061/”) = 0061”+ ”'25). The constant involved in the (9-symbol involves only p, 5 and z. This shows that W1(K) -> 0 with K ->oo, as promised. To complete the proof we must show how the decom- position (#.h8) can be effected. This will, of course, depend upon the particular MEEXK. Certain cases must be identified and handled separately. Recall the def- inition of TN given in (h.3), (h.h) and (k.5). We assumed that for M = (d Ellis ) all the entries are positive, further, a.and S are not simultaneously 0. We identify six cases: 1) M = I, 2) M 3)M Let M = («.8l‘38 ). The remaining cases have positive (OH-lll 0) with (X > o, (o 4118) with 8> 0. entries and we identify them: 1,) r-oL>o, <§-£s>o, 5) X—do and, finally, 6) 6-q O and 5.- B < 0 is excluded by the fact that «8 - sb’ = 1. We determine the image of ’J7K under M in each of the six cases. From the geometry it will be clear how we can effect the decomposition (%.h8). We refer the reader to either Fig. h.1 or Fig. h.2. 1) Let M = I. ’1. ~35} (— K’L..._._a_.uaaw - --__.. ,_____. ( K» K) J I % K ___._- puma--- hi...” I i (~ch) (m—K) Fig. h.3 In this case W2(K) = 0. Further, in the sum for W1(K), (II) always holds with Q(c) = 1. -hg- 2) SupposeM=(oL,-l\lo)€7nwith o(>0. The transformed region is given below. V l 111 f (-( \+<><)K)KL_ (Cl-00 K,K)F \ _(1‘ ”ix” xi? ‘3) \ U ‘ ~‘i((d+0b(;K) Fig. link We see that for W2(K) situation (II) prevails with Q(c) = 1. We handle W1(K) in the following way (1+0L)K-1 . [x 2] W1(K) = Z T(c,K) + i T(c,K) c=[K/2]+l c=(1-d)K-l to obtain the decomposition (h.k8). In the first sum above (I) holds with R > l/h; in the second sum (II) is satisfied with Q(c) 2 1/2oc . -50- 3) LetM=(o-1(1£)emwith (>0. i V /(K\(§+\)\"\) . , L ~Q .K'/ I. 6 :1)“//// (Kfikflkv // 1 T u /////f //:;14 (hum—M) A “ (9 l-<,-Lg+ 3‘; i0; 334$ Fig. h.5 For this choice of M, W1(K) = 0. We write [-K/28] K-l, wzm = Z mm + Z T(c.K) =-K+1 c=[-K/28]+l to obtain the decomposition (h.h8). In this case for (I) R = 1/28 and for (II) Q(c) > 1/2. -51- u)LetM=((xs|zg )cm with x-a >0 and S - B > O. The configuration of regions is given in Fig. h.6. i V : ‘ «a+r)K,¢d€)K) U _ --_—.—_.—- ._._(_ (~((+d)K‘—(6+S)K) L Fig. h.6. For W1(K) we always have (I) with R = ()’-0<). However, we must decompose W2(K). Write [-K/gg] (IrdeK-l W2(K) = z T(C:K) 4' Z T(C,K) C=-(Y+d)K+l c=[-K/é$]+1 to Obtain (“01*8). The cases 5) and 6) are handled in a manner similar to h). We give their configuration of regions in Fig. h.7 and h.8 respectively. The reader can see how these situations are handled. -52- 5) M=(0(Bl‘(8)67)1with J-(Xo. 52‘ ((Y+o<)K,(£+fs)K) a)K€(S-@)KQ («(1400 K , -(S+g)m Fig. h.7 6) M: (ka]h’8)éWlwith y-ot <0and 5-p°° [— miglvmxcmfi (c,d)E 036A?“ )M Proof: In lemma 1 we proved that (D. G(z.rv.AJ,I’ .n) = 3AM e((p+K)z/1) + :3 H1(C.z) c=-oo 2:“ + H (c,z). J 2 =om Now, lemma 2 gives for M 5 m u e((p+KJ)a/c 7&3) (MSG) H2(c, z) = lim Z 2 K ‘>°° ’\J’(A31Vc,d)(czifd) (c,d)ee’KuyFm Furthermore, we proved that the double series H1(z) of (3.17) which sums to EC, J111(c, z) is absolutely conver- gent. Thus, we may write -(p.+K) -1 I e((m/cj)a/C’KJ) §e[+)c 7‘ cud] 3 (#051) H1(2) = 11111 #L——— K ->oo mAilvc’d)(cz+-d)2 (c,d) 591((AJ9 r)” Both the limits in (#.50) and (h.Sl) exist, therefore, we may add them. Using the fact that for c y! o, -51}- V2 == (az+b)/(cz+d) : a/c - l/c(cz + d), we see that “(Mk )V z/7\ ) G(Z,U,Aj,r,p) = lim Z J cod 1 K ->oo 47(A31Vc,d)(cz + d)2 (c,d) fix”? )M where we have incorporated the term correSponding to c O in with the limit. 5. The Functional Equation In this section we prove that the functions G(z,m;AJ,F',p) satisfy the functional equation (2.11). That is, for every V = (a b lc d) (5.1) G(VZ.UrAjrr,u) = rm) (cz + d)2 G(2.’lf,AJ,f—,p). We use the results of the preceeding section; namely, lemma 3 and the representations (h.6) and (H.7) for VEET'. The result (5.1) follows from the special cases: (502) G(U7\ 2945-1339 Fall) 3 “(01) (“Zn/3A..” rail); and forM= (oKBlTS)e'm, (5.3) mummy 1",») mum (6’2 +8 r2 G(z.4r.AJ. It»); finally if, in particular, 3: (o - 1| 1 o)€ I“ , then (5.1+) G(Sz/U‘.AJ.F .u) = ms) 2.2 c\M) IUUJn ) (Yz +7n>x + d)2 G(z,’1r,AJ.r 9P) = 4,7(V) (C2 + d)2 G(29V9A FDP)° j, -55.. -56- If, instead, V = Um SUdk: (a b\!c G) than c = 1 and d = n7\. As above, ax =4;(u“‘7‘5;) (11“7‘2)2 ow z,’V,AJ.r .u) =4)‘(v) (z 4- 11702 G(z,’U’,AJ, rm). There was no loss in generality in assuming c 2,0 since we were dealing with linear fractional transformations rather than matrices. We defer the proof of (5.2) until the next section where we obtain the Fourier expansion of G(z,®CAJ,Y.,p). To deal with (5.3), we have from lemma 3, 11m : e((u+ "1)Vc d z/kj) K “>00 V(A31Vc’d)(cz + d)2 (c,d)c [figuym G(29/U9A39 r 9P) 3 where in that lemma we have taken M = I. Now for any M C- 'm we see upon substitution e((u+’<) dMZ/X ) MHz/1518.1. F...) = lim :0)! ——-Jv fil— K->oo IVc’ndMz-td)2 (c,d)e (9::(115, F) e((u*< J)V Mz/ij) lim mmofmg)? Z ° 6 K'>°° 4/‘(A 'lv: drmc' z+d' ) (c,d)éCKMJJ') 2 -57- where vc,dM = (* * \ c' d') = (* * tac+ Yd, Bo +Sd). If (c,d) runs over C}K(AJ,[-) then (c,d') = (c,d) M runs over K(AJ.f—)M. The terms of the series depend only on the lower row of vc,dM‘ thus, d((l5+a’f _____J)vc ,dz/AL, ,fliAJ 1vc d)(cz+d)2 con/minim) =U(M)(Xz+5)211m Z—-——1 K->oo but by lemma 3 7i e((u+l( )V 25/ Cami, ..n 2.1—: cd 4.. K">°° «MAJ Vc d)(<:z+d)2 rm therefore, G(Mz,/U,A3.r,p) = «mum +5 )2 C(Z,’U’,A3,r,p). Suppose, finally, that S = (0 -l\ l 0)€Ir . Then from lemma 3 with M = I, e((p+fi. )V Sz/A ) 11““ Z ‘4 M 51‘ K->oo an Aglvc , d) (cSz+d ) (c,d)eoxu r) C(3294LAJ, rill) J, 2 e((u+1oo /U'(A31Vc dS)(dz-c)2 (c,d)60 KMJJ‘) -58- As (c,d) runs over O'K(AJ,F ), (-d,c) = (c,d) 5 runs over fixujf )3. But O'K(AJ.F)S = @(AJI ). Thus, Z 3((P+KJ )Vc,dz/AJ) Qf(A31Vc,d)(cz+d)2 ' (Cod)€ §K(A31r ) G(SZ{U3AJ,f—,p) =’UKS) 22 11m K ->oo =’U(S) 22 G(z,/U',A I'M, J, 6. The Fourier Expansion As mentioned in section 5 we must yet prove that ’A 1 (6.1) G(U z,/v,AJ,I”,p) =rU(U )G(z,’lf,AJ,r .p). This is accomplished by expanding G(z,V}AJ,V_,p) in a Fourier series, which, furthermore, will give the behav- ior of G(z,v}AJ,Y',p) at the infinite cusp. We begin with the series I (6.2) H2(z) = ijfizhn) 03'00 ’ 2 2 2 = 3 (2n) /c A (n+x<>wc 0. Each of the functions H2(c,z) is regular in y 2 y0 > 0. Thus, by the Weierstrass double series theorem I (6.3) H2 0. Thus we may rearrange the order of summation in the manner of H2(z). Proceeding from (3.17a) (- '21T1(p.+K))m e((p+KJ)a/c >13) H1(Z)= cm 'xm m: J '1 n+2 2-00 d=-oo «NAJ Vc'd)(cz+d) (6.h) Now, as in H2(z), we can write the inner most sum (on d; see section 3, the development following (3.12)) i——-1———L-— e((p+‘< )a/c R ) { e((p+xj)a/c ’AJ) = Z: -1 =_égv(A31Vc d)(cz+d)n+2 (UMJ vc,d) deficurr) {c-nmz i saw) (chmz q=_°o(-i(z/7( +d/c7\ Mu)”2 g 9((p+«3)a/b‘xj) (_ 2w1)m:2 - Z ’U(A31V (c Mm+2 NM?) 3 . d6 003113.!” ) c,d) 00 a: (Iv-K)!"+1 e((n+K)z/>\ + d/cl D} n=0 where we have used the Lipschitz formula (2.20). Inter- -61- changing orders of summation, valid because of absolute convergence, and introducing the Kloosterman sums, we obtain finally 0° (-2vi)m*2 (n+K)m+1 co. = : e((n+K)z/)\) wc(ngll)o n=0 3 (c70m+2 (m+l): =-oa Introduce the above expression for the inner sum in (6.h): (6.5) 111(2) = i e((n+&)2/?\) n=O m ' (-2"1)2m+2(n+K)m+l(p+KJ)m i wc(nrll) 0n comparing (6.3) and (6.5) one sees that (6.3) corres- ponds to the missing term m = O in (6.5). Thus, on adding (6.3) and (6.5), we obtain cum“. F») = SAJ'IeUp 4402/1) (6.6) t i cn e(n+K)z/7L ) n=0 n+K>O where ‘ i’ i ('2V1)2m+2(n+K)m+1(p+Kj)m C = W (n, ) n c=-ooc p m=0 c2” AW A?(m+1):m: CG é (A3, r) (6.7) 3 Cn(/U'9AJ: r- all) -62- We note in (6.3) and (6.5) that if K.‘ 0 then the coef- ficient co = 0. This is the reason we restrict our sum in (6.6) so that n +I< > O. A simplification of the coefficients c can be n effected if one used the Bessel function [18, p.358] (6.8) J (z) = i "'1’" ‘z/Zfim . 1 m=o m: (M1): The sum on m in (6.7) can be written in the form ') m 2m*1‘¢""' "" 2m+l _ 217 ng-K X1 ('1) (217) ( “:51 “mi-K) ch 44 «3 J? M m:(m+1):(./X;fx’)2m+1 Mam“ - 2 _ (6.9) = - 2" (4‘1“) (2:5)12‘J(21r_f‘“*“1"““’) Icl7x M “A; 1 Icl M A We assumed that p #'0, therefore, p + K3 #'0. Using this expression, we may write the coefficients on in the following form 1/2 1/2 I u+K - un'(u+K')(n+K) .211 3 2:13 2': , _. L cn ’>\ < 7‘ ) (X ) =-o[:' 1Wc(n NHL 7‘3 k ) J When u + H1 < O‘we can replace p +I(J by (p + Kit and then we must also replace J1(z) by 11(2) = 1-131(12) [18, 372], the Bessel function with purely imaginary argument. -63- We now derive (6.1). Replace a by U z = z +?\ in (6.6) cw‘zwmjfim) = 5%,: emu-u )(z+7t m) + i on e((n+K)(z+ 70/1) n30 mm )0 = e(/i)G(z.’U.AJ.r.M =U(U1)G(zr’1fsAjrr-— 99') As 2 ->ioo within the fundamental region R(r), G(z,v,AJ,F ,p) tends to a definite limit, finite or infinite. We see that it p + x > 0 or A: f I this limit is o. If A3 = I and p. 4» I4 < 0 then G(z,’U’,AJ,[—,p) has a pole at 1 oo. 7. The Behavior at the Cusps In order to show that G(z,v3AJ,Y-,p) has the correct behavior at each of the parabolic fixed points of r-, we establish the formula (7.1) G(stsAJsr—sfl)’ B 3 G(Z,’\J!,AJB.B-1r Bop) for each Bti T'(l)(see (2.13) for the definition of IE). a}! =/U(B'1F'B,-2) is the multiplier induced on B’ll' B by 4fa(U(I—,-2). This formula is of interest in its own right. Sincel— is a subgroup of the modular group and B €1"(l), then B'li' B is a subgroup of the modular group. If R( r) is a fundamental region for F then B'1R( r) is a fundamental region for B'lr B. Write R(B’1 r B) = _B'IRH' ). If Mr) is bounded by a finite number of sides consisting of straight lines and circular arcs then so is R(B-1I‘ B). Furthermore, if the parabolic cusps of R(T') are inequivalent, so are the parabolic cusps of R(B’lf' B). If Asloois a cusp of R(T') then (AJB)'loo= B.1 3100 is a cusp of R(B'lr' B). Thus, all the developments of sections 2,3,k,5 and 6 hold for the Poincare series in the right member of (7.1). We shall assume for the moment that (7.1) holds and show that G(z;U;AJ,f—,p) has the proper behavior at the ~6h- ~65- cusps. In section 6 we showed that G(z,’U’,AJ,\— .9) has the proper behavior at z = 1 00. We consider first the remaining cusps of R( 1’). Let Ail 00: pk for 2 g k g a(l-). Then from (7.1) applied to G(z,Nk,AJA;1,rk,p) with B = Ak and FR = AK )- Ail we get (702) G(Z,’Vk,AJA;19 rksfl) I AR 3 G(zrvsAJor—DF)0 "i is the multiplier system on r}: induced by "If on r . ark induces ’Von F . Rewriting (7.2) (Ckz *' dk)-26(AkzsrvkoAJA;1sT—ksl5) = C(zsvsAjsr a“) where Ak = (ak bk, ck dk). As z'-> pk = -dk/ck, Akz --> 1 00. Since G(Akz,’lfk,AjAl;1,r-ksu) = O(‘e(kakz/?\k)( ) with wk=l0sndk;13, wk=1ir Kk=0and 3 )1 k, and if k =1 then wk = u + k3, it follows that G(z,ir,AJ,T-,u) tends exponentially to a definite limit as 2 -> pk. Indeed, if k i 1 each of the terms of the Fourier expansion of G(Akz,’UL,AJA;1, rkm) tends expo- nentially to O as 2 -> pk. Now let p be a parabolic fixed point of T— . Then there is a V = (a bl c d) such that v-1p a pm is one of the cusps of R(f'). The functional equation (5.1) gives G(Vz,’lf,AJ.r,p) =4)'(V)(cz 4- d)2 G(z,’U',AJ,r,u). As a --> pm in a parabolic sector in R(T' ), Vz --> p in a parabolic sector at p. G(z,’U’,AJ, 7,») tends exponentially to a -66- definite limit, therefore, 6(Vzgr,AJ,V'.u) does also. This completes the proof that G(z,¢5AJ,i-,p) has the proper behavior. It remains to establish the formula (7.1). We do this by induction after we have established (703) 6(29’VoA19 Fall), U G(Z,’\J!,AJU,U-1rU,|L), and (70"?) G(z,’U',AJ,r gun) I S 6(294}'9AJS:S-1[—S,|5) for the two generators U = (1 1| 0 l) and S = (0 -ll 1 O) of f'(1). a? is the character on U'll_'U induced by «F on I'. a; is similarly defined. Proof of (7.3): In (3.2) we defined H(c,z); and G(U flu-9A3: Y‘all») 2' iJH(CsUZ) c=’m where H(c,Uz) = iJIi-r(A31Vc,d)(cUz4-d)-2e((pi-KJWc’dUz/KJ). =-oo Now gnarl”) = g(ljum‘lr' U) and 00(c,AJU,U'1|" U) = ic+d2d600'(c,Aj,\—) i. -67- The proof of these facts is almost immediate. Further- more, if IU’ is the multiplier system induced on U'lY’ U ’k c,d+c 4f(A;lvc,d) = a}(u‘1A31vdU) =ar'usju)’ 1v; Md). Also, 7\. = R(AJUsU-1r-U)=7\(AJ.F)=13. and It = R(AJUN'IF U) = K(AJ. F) = «3. Substituting these results into H(c,Uz), R(C.Uz) = Z-_:71"J"((AJU)1Vc dfic)(cz+d+C)'2e((u+KJ)V;,d+c2/7\J) d€£(C,A Ajsr ) Z: 7m '(u U)‘1vd)(cz+d)'2e((p+ «ch’dz/AJ) d6 flC.AJU.U'1I—U) g(cm) since as d runs over ¢7(c,AJ,F') d' = d+c runs over 00(c,AJU,U'1 T' U). Thus, if H(c,Uz) = {g(cm) = (}(z,/\/!,AJU,U"1 \— U,p.). 3 -l c="m C€;(AJU, U rU) Proof of (7.k). From the definition of the operator -68- S and from lemma 3 with M = I, we see G(z.¢r.AJ,T'.p)|s . 5:13:00: ri'xi'lv d)(cSz+d) 2e((u.+ xjwc dSZ/A ) (c, d)€€9K(AJ,r ) . = 3 - - ' = Let vdrc vc'ds (b, a|d, c). vd,-c€ AJVS AJS s’1r 3. Thus, (d,-c)eO(AJ.F) s and - -1 Moreover, M(A31Vc,d) = q}'(s'1A31vc c, S) = 13((AJS)-1V;'_ ) and R(AJSfi’lr‘ s) = 13 ., &(As,s'1r S) = «3. Therefore, 2’2 Lim ZfiAslvc,d)(cSz+d)'2 e((u+IiJ)Vc’dSz/3\J) K ->oo (C,d)€0 (Ajtr) 11m Zrufiszrlv d)(cz+d)‘ Zeuw «ch d2M) K->OO (c,d)eO (A s,s‘1r‘ S) J N .- G(Z.€U’,AJS,S 1 r‘ 3.»). This last equality follows from lemma 3 with M = I. Since 8 and U generate F'(l), we can write any B b 1 a a b em) in the form B = s 10 s ”U “, a1 2 Leo 2 0. -69- b1 2 l and bn‘Z 0. Now we need to know that F(z) v1v2 = (F(z)‘ vl)\v2. Let N' be the multiplier system on V? 1' v1 induced by ”VOn F , «P be the multiplier system on (V1V2)-1Y' V1V2 induced by ’V’ on Vilr’vl, and let nffl'be the multiplier system on (v1v2)'1r' Vlv2 induced by’U'on F'. Then 4f =/U' (7.1) is now proved by induction from (7.3). (7.h) and the above mentioned facts. 8. Kloosterman Sums, Main Theorem, and Examples We introduced Kloosterman sums associated with our modular forms of dimension -2 belonging to r-and the multiplier system /lr=’lF(F,-2) in (2.18). At the same time we assumed that for fixed 9 {'0 these sums could l1/2 +E‘) be estimated as O( \c . With this assumption we have proved the following theorem. THEOREM 1: Let [_be a subgroup of finite index in the modular group (“(1) and let Qr=flf()",-2) be a multiplier system for(— and the dimension -2. Let A3100 = p: be a cusp of the fundamental region of F (A3100 3 00 if and only if A3 = I). Then e( (“+KJ )vc’dz/RJ) (8.1) G(z,W,AJ,r oil) = i c=-oo =-oo /U(A31Vc,d)(02+d)2 “(3”)“? ) dEo<9(c.AJ.l’) is a modular form of dimension -2 for r and the multiplier system «1T=Qf(f-.-2)s provided the Kloosterman sum (8.2) Wc(n+K.AJ,p+’£J) = Eluslvmyd(n+K)/c?«+(p+KJVol.1) dEfié(AJOI—) can be estimated as O ( (ell/2 +E ) for fixed p. ;{ O. The series in (8.1) is not aboslutely convergent; we under- stand that the summation is to be performed in the order -70- -71- f a) -1 oo 11m 2 °'° + 11111 E 00. K ->oo K'->ool-—- c=0 d=-oo c=-K d=-oo effgflAJ’I-fl) deflcrA1sr) (366(Ajrr ) dfflcsAJsr) The sets 5 (A1,? ),0‘~9(c,AJ,r ) and ”6::(A3’r) are defined in (2.16). Furthermore, G(z{U;AJ,[-,p) has the Fourier expansion (8.3) SAJ'I 9((IH’K)Z/7\) + Z cn(V.AJ.r.p)e((n+K)z/7t ) n+K>0 where ' w ‘13 n+Kg ”C(nrfl) kn “+K3‘nIX ‘8'”) “““(ALWTJ Z TJ1(T°-F{XJ T) n+K>0 where we use the positive square root. J1(z) is the Bessel function defined in (6.8). In regard to the estimates of the Kloosterman sums Petersson[11] has proved the following theorem. Theorem (Peterson): Let F'be a congruence subgroup of the modular group, wran.abelian character for F‘, and suppose there is a principal congruence subgroup T'(N) such that Hmc F and 1f=4f( r‘,-2) is identically l on Y'(N). Then the Kloosterman sum (8.2) has the estimate 8. (9(lcl1/2 + ) for fixed u #'0. The constant in the C7-symbol depends upon 4F,r—,p and E.but is independent of n. -72- We shall give Petersson's proof of this result. The material given in thelnext few pages is an elaboration of pages l6, l7 and 18 of [11]. The proof proceeds by showing how to reduce the sum (8.2) to a sum of original Kloosterman sums. Then the results of Salie [l5] and Weil [17] for these sums are applied to give the final result. ("(N) is normal in F‘. Suppose V has the coset decomposition (8.5) =U Ks I‘m), K e (— s=1 s where 1!: [F’:)—(N)]. Then V (8.6) A r = U A j 831 JKs rm). We state a lemma. Lemma 1+: 0(AK ,l’m» and 0(A3Ks' (’01)) are either 3K m’ disjoint or identical; they are identical if and only if -113 Km = PJKSM where n is an integer, PJ = AJ U A:j and M E F(N). Finally, for ceéu r) J, (8.7) flcmjf) = U1 Ole. AK K.Y‘(N)). s- n . z n - J Proof. Suppose first, Km PJ KSM then AJKm - U AJKSM. If (c, d)€(7(AJKs M, ( (N))= C9(A3Ks ,('(N)) then there is a V\J. Therefore, we can write -75.. loll EWCCn.,'») = g Z d: 6681::ij ) g\¢Db_ 1 (8.9) "' (H (“A A) Va, 8’ “(WWW/ck ((MKJVc a3) - J 00% 84.1") N (cl = Waglvm) e([g(n+/( )d+gj(u+/(J)]/cN) d=1 . d6 @(C, A37r) where we have used the periodicity in d and that g?t = N and gJ 8:] = N. Now using the decomposition 16(c,AJ,T ) gt = U 08(c,A K F(N)) and the fact that these latter sets s=l 38' are pairwise disjoint, u" N|c( 8Wc(nw)= 2; dzg’vmglvcm) e([g(n+/()d+gj(u+/ U1 U2 T U2 2 0 e(“/“) 1 1 2 T2 U2 0 2 e(B/h) 2 - x T3 U2U1U2 2 0 e( /h) r5 ”2U1U2Uil 2 o e(B/h) -88- We see that the’U’=“*(T‘(2),-2) determined by 1) Cl: 0, 2) (i=0, (8.35) 3) O(=’+, 1+)0K= h, B B B B o u 0 u will be identically 1 on ['(h). From the data given in Table 8.3 we see that, in addition to the above multiplier systems, the multiplier systems determined by 5) mi: 0, (8'36) 7) O(= O, are identically l on T'(8). 'UD'CD'UD B 2 2 6 6 Petersson's theorem applies to these cases. We shall return to these examples at the end of the next section. -89- Table 8.3 Generators and exponent sums for r(8) Generators Representation t1 (1)1 00(1) for F(8) in terms of T1 (01) (U2) X1 Ti 1+ O eé) x2 Tzrlrglrll o o 1 x3 Thrlrglril o o 1 XL, : T1T2T1T31 1. t o 961;: ) xs grlrurlrgl u E o 3 e63) E 1 -1 i : x6 ETSTITS T1 o i o a 1 x7 :TlTsTngl u g o : e63) x8 r3 0 1. fig.) x9 'rhrz'rglrll -2 § 0 ' e(-°f;) x10 rsrzrglril | -2 g h i e(-‘E'+ 3) x11 TngTil ' o g h g e(3) x12 rlrurzrgl 2 g o g e63) x13 «_Tl'rsrz'rgl ; 2 u 3 e(?;‘ + 3) x1“ ér3ril % 0 § 0 1 x15 §r1r3 E h 3 0 e63) x16 Tur3rglri I o g o 1 x17 r5r3rglril o 1 o 1 -90- Table 8.3 continued Generators!Representation 1'1 C01 ’W(X1) for i"(8) in terms of T1 (01) (U2) -1 h N -1 g_ X19 TITMTBTM H O e(2) -l -1 X20 T1T5T3 T5 0 0 l -1 -1 a X21 TzTth T1 -2 0 e(- g) 2 X22 Th 0 0 1 x r r T’lr'l -2 o (- a) 23 s h 2 1 e E -1 o< 2 -l X25 TlTth . 0 0 l -1 g X26 jTlTSTuTZ g 2 0 6(a) 1 -1 -1 z _ - x E X27 {TZTSTM T1 E 2 h e( K + 2) -1 -1 1 g X28 THT5T2 T1 i -2 0 3(k) 2 9 E 2 -1 3 E -1 3 N E -1 g x X32 TlTkTST2 2 O 1 e(:) ;_ -1 -1 g 1 x33 ,T2T3T2 T1 0 5 o 1 9. The Inner Product Formula The set of all cusp forms g? F,-2,1r) is a finite dimensional vector space. Petersson [10] introduced an inner product (9.1) (F(z), 6(2); R(i”)) = ,{i F(z) 5??) dx dy R(T‘) on this Space. The integral is a Lebesgue integral, and R( r) is a fundamental region for F'. The integral is known to converge and be independent of R([—) [10, pp. h9h-h96]. The object of this section is to establish the inner product formula: 111130313143: For .1 _>_ 1, F(z) 5V F,-2,1r), we have a (F,A ,F )K2 (9.2) (F(z). G(z.’2r.A Y3»); MD) 2 41—4—1— 3, [Hr(p+KJ) where a“(F,AJ,f—) is the p-th coefficient in expansion of F(z) at the cusp A3100 = pJ (see(2.12)). We start with Lemma 5: If F(z)€é§+(T-,-2{U) then for y 2 yO > O (9.3) F(z) =O(exp[-2wy/7\]) where 0):.K if H.) 0, otherwise a): 1. Proof: F(z) has the expansion in (2.12) with AJ = I where s + K > 0 since F(z) is a cusp form. This Fourier -91- -92- series converges absolutely uniformly in y 2 yO > O. The result follows. Let R( F) be a fundamental region for I’ which is connected and lies in the strip E< x < 2 +1 where E is a cusp Ailoo. This fundamental region is to be bounded by a finite number of straight lines and circular arcs. Each parabolic cycle is to consist of a single element. We begin the proof of (9.2) with A = I; let 3 (9A) J = (cu/151$”), F(z); R). -1 For each p = A 00, J = 2, 3, ..., a(I‘) let R = R J J .1 p3 be a parabolic sector of R at p3; We suppose the sectors are chosen small enough so that, for j #’k, Raf) Rk =,¢. Let R1 = R - 3C} RJ. We are now able to write (905) '1‘: (C(zr/UaIrx—tll)’ F(Z); R3): :11} J3 Jfl where RJ indicates the set over which the functions are integrated. We now introduce two results of Petersson [10]. If G315 an "admissible" region, then for V = (a b \c d) a real unimodular matrix (9.6) f, (F(z)\V) (G(z)\V)dxdy = J F(z) 6(2) dx dy; v 10.3 63 -93... and for L € V. (9.7) J, .F(z)'G(z) dx dy = J’F(z) G(z) dx dy. LCB 8 Suffice it to say that R, R1,... RT are "admissible" regions. We now apply (9.6) to Jk, 2 g k g o, with V = Ail. (9.8) Jk f {mm/11.1.1311) \ Ail} { F(z)‘ affix dy AkRk if 0(2'WiC’A121' rkrl-l) F(Z)\ A121 d1 dy AkRk The last equality comes from (7.1); (L = Ak F Ail. We now use the representation 0 ’U’ '1 F - (90/) 6(29 k’Ak, kg“) " H(C,Z)o “may. FR) This converges absolutely uniformly for y 2 yo > O. The parabolic sector Rk is mapped by Ak onto a strip ’1; = i2 = x + iy: ék < x (:1: +7\k, y >7Zk > O }. Introduce (9.9) into (9.8) and interchange summation and integration; thus, (9.10) Jk = 2::3 ‘{ HCc,z)‘F(z)\ Ail dx dy . -9h- We now justify this interchange of integration and sum- mation. We see from (3.10), (3.12), (3.1%) and lemma 5 ifcflo H(c,z)F(z))A£1k< C(Yk)exp[-2wwy/k]{(L/02Y2)exp[2fl(u+l)/V +(Q/IclS/2 y sing )exp[2n(p+l)/V ysinS ] +(C5/ [cl 3/2-E)(1 - exp[- 2fiy/13Y2 Recall that 8: erg. 2; since gk < x (ER +>‘~k, y >21: > O, we see that sin): is bounded away from 0. If c - O ‘ H(o.z) F(z)! A31 < C(Qk) exp[-2 (p+lt+UJ)/A.]. Therefore, 00 2:: .[ \H(°’z) F(Z)‘ Ail} dY < + 00, c ’Lk and this completes the Justification of interchange of summation and integration. H(c,z) is the series Z’fiflfivcmflcz ” d)‘2e((p *“)Vc,dz/7\ )° d€fi(C9A-lsr—k) Recall that K = «(1, F) = M11121, [1) and 1:1(A121, rk). This series is absolutely uniformly convergent for yEB yo) 0. Introduce this expression into the terms of -95.. (9.10) and interchange orders of summation and integration. We obtain (9.11) -._ e((p+fl)vc dZ/W) ._ J = y ' F(z)\ -ldxdy. R Z L. ’lfkhikvc’d)(cz+d)‘2 Ak ce as “1531; 5(A;1.I"k) acmklxk) We understand that the summation in (9.11) is to be car- ried out in the same manner as indicated in Theorem 1. We now justify the interchange of summation and integration on d. We see from lemma 5 and (3.5) that irdgo “(1”ch dz/X ) exp[-21rwy/1] flr(z)]ak1 < C(7k) ‘cz + d[ 2 Mk(Akv d)(cz+d)2 5 ch)(1/d2) exp[-21rduy/7\ ]. Therefore, Z [w e((u+K)Vc dZ/W) QR Vk(Ak1V C d)(cz+d)2 < CQk) {I + 2:.1/d2} foo exp[-21rw y/A ]dy 7 d k < + 00. -96- In the terms of the series (9.11) we make the change of variable w = Ach d z. The Jacobian of the transforma- .9 tion is , -h Since F(z)\ AQ1€'C:(rk.-2{Uk) F(ngdAilw)lA;1 =’“R(ngdAil)(-(cdk+ack)w+(cbk+aak))2F(w)\A;1 On computing one finds that 1 - -1 (ch,d Ak "4- (1).-2 = {-ckw 4' ak)2(-(Cdk+ack)W+(0bk+aak))-20 Therefore, substituting these results into the terms of (9.11), we find they become J, 6((p+KJA£1W/7\)(“Ckw + ak)'2'F(z)l Ail dudv. Akvc,dAkRk Once again we make a change of variables. Let z = Ailw then the above integral becomes I e((u+K)Z//\) F(z) dx dy . Vc,dAkRk We have used the fact that the Jacobian is lckz + dk) -h s and the identity (ckz + akrzmikz) \ A121 (ckz+ak)’2(ckakz + dk)-2 F(z) F(z) -97- Thus, (9.12) Jk = Z Z I e((p+K)z/7\) F(z) dx dy. c d vc,dAkRk c and d are summed over the same sets as in (9.11) and summation is carried out in the manner of Theorem 1. -1 We mentioned that vc’de 1’ 1k so that Vc,dAk€ V . As (c,d) runs over @(Ailfk), (c,d)Ak runs over 0 (I,\'-). Let 02 be a complete set of matrices in r with different lower row. We shall make an appropriate choice of the upper row. Let [Ux'] denote the cyclic group generated by fil . Then (9.13) V = "J [U1] v . e<2 Let (9.11.) 08: V902 VRH') . dfiis a fundamental region for [U?\]. We suppose that -1 vc,d€ T'Ak is chosen so that Vc,dAk 6 C2 . Define 03k = u Vc,dAk€Q R for k = 1,2, .00, O 0 Then, Vc,d Ak k by the completed additivity of the integral, we see from (9.12) (9.15) Jk = d!- 6((p+k)z/?\)‘§(z) dxdy . k -98- O H- Furthermore, U @k = W. Thus, from (9.5) we se k=1 that (9.16) J = [8((314402/7‘.) F(z) dxdy . 667 ThestripJ ={z=x+iy: §0‘( isa fundamental region for [U1]. Due to the way we chose R( F), there is a determination of the V's€ 01 so that 00:1! . We shall use this determination. Define 00'(y0.y1) £2606 :yO < y < y1% then J = lim J(yo,yl) = lim f e((u+K)a/7t )F-(z)dxdy. y1 ">°° y1 "‘>°° (76(y0.y1) yO ->O yo ->O By the lemma of this section I - C(y0)7\1 ‘ F(z)e((u+’<)Z/A )(dxdy < 2noo, the integral tends to a limit J(yo,oo). Introduce the Fourier expansion for F(z) and interchange orders of summation and integration: mom) = Z 3n(F.I.V)[e((n+K)z/a )e((u+K)z/1)dxdy n+K>O OWYONO) The interchange of order is justified by the Fourier series converging absolutely uniformly in y'z yO > 0. Consider -99- f e( (n+K)z/)\ )e((p+/<)z/?~) dx dy w‘YODW) 00 $4.) I exp[-21r(n+K+p.)y/ 7( ]dyf exp[ 21ri(p.-n)x/’A ]dx Yo g = 2'2 exp[-hw(p+k)yO/z_] S . hfl(p+K) p,n 5“ n is the Kronecker symbol. Thus, ._ F 2 8“(F:I: )% J(y0.oo) = exp[-hw(h++<)yo/h 1. hV(p+K) Now let y0->O. Since (F, G: R) = ( G, F: R) the result (9.2) follows for Aj = I. Consider ) J(A (F9 6(29M9A3, r3“); R(r ))o 3 Then by (9.6) MAJ) = < WEI: t(znmjm .p)lA31: R(I‘Jn .. -1 . " ( F‘AJ 3 G(zsqrjrlp[31u)9 R(rj))o = ‘ = = F; r = , Now 13 MAJJ’) MIA’J) and n3 (13, > K(I,rj) Thus, from (2.15) and the case already proved -100- 2 afl(F’Aj, r) x3 -1 . - (F A3 : G(Z.VJ.I.FJ.|1), R( rj)) " This completes the proof of the inner product formula. The following well known result is an immediate consequence of the inner product formula. Theorem: The vector space Spanned by the Poincare series G(Z,V,A39rgfl)g [L = 1, 2, .0. equals 5+(r, ’2,V)o We return to the examples we considered at the end of section 8. P- EXAMPLE 1. I = r (1): there are six characters on T-(l). In only one instance is the dimension of the space 5% r(l),-2,’U‘) positive. Petersson [12, p. 189] gives a formula for calculating the dimension of £7+. Using his formula, we find that when Qf(S) = -1 and QT(US) = e(-l/3) is the character defined on the generators S and US of R1), the dimension of 5+(1),-2,V) is 1. This proves that in this instance not all the functions G(z,U3I,I",p) with p > O are identically 0. However, for the remaining five characters on ('(1) and for p > O, we have G(Z,‘U,I,r ,“) = 0. EXAMPLE 2. T =T"2 = [SU, US]. There are nine characters on (‘2. As in example 1, there is only one character for which dim {‘1 (12,-2.1)") is positive. If ”1"(SU) = e(-1/3) = g(US) then the dimension is l. -101- EXAMPLE 3. In the case I‘d—0m), (NV) = ('3): v = (a b] c d), q a prime of the form h m + l, Hecke [h, p. 815] gives the dimension of g*(i’0(q),-2,U). The first prime for which this dimension is positive is q = 29, in which case the dimension is 2. EXAMPLE 1+. If I” = F(z) and’U’ is the multiplier system determined by 4I(U1) = e(l/2), ’U(U2) = e(1/h). then the dimension of the space é§+( F(2),-2,1I) is 1. In the other seven cases considered the dimension is O. BIBLIOGRAPHY l. L. E. Dickson, Studies 19 the Theory of Numbers, Univ. of Chicago Press, 1930. 1.1. T. Estermann, Beweis eines Sates von Kloosterman, Hamb. Abh. 7(1930), 82-98. 2. L. R. Ford, Automorphic Functions, Second edition, New York, 1951. 2.1. R. C. Gunning, Lectures gn_Modular Forms, Lecture Notes, Math. Dept. Princeton Univ., 1958. 3. M. Hall, Jr., The Theory of Groups, New York, 1959. 3.1. G. Hardy, Ramanujan, Twelve Lectures on Subjects Suggested by His Life and Work, Cambridge, l9h0. h. E. Hecke, Mathematische Werke, GSttingen, 1959. 5. M. I. Knopp. Fourier series 9; automorphic forms 9: non-negative dimension, Illinois J. Math. 5(1961), 18"“‘20 5.1. , Automorphic forms of non-negative dgmen- sion and_e§ponentia1'sums, Michigan Math. J. 7(1960) ‘- s.“ 257-287. 6- J - Lehner: 9.9. 14.99.11.191‘ f. 9.3.28 .0! negative dimensies. Michigan Math. J. 6(1959), 71-88. -102- 7. 10. 11. 12. 13. 19. 15. 16. -103- J. H. van Lint, On the multiplier system of the Riemann-Dedekind function 71 , Neder. Akad. Wetensch. Indago Math. 20(1958), 522-5270 W. Maak, Fastperiodische Funktionen aufgdgr Modul- gruppe, Math. Scand. 3 (1955), hh - #8. W. Magnus, Discrete Groups, N. Y. U. Inst. of Math. Sci.,l952. H. Petersson, Metrisung der Automorphen Formen und der Theorie der Poincaréschen‘Re1hen, Math. Ann. - -4. '“ 117(1990). lt53 - 537- . fiber Modulfunktionen End Partgtionen' probleme, Abh. D. Akad. Wiss. Berlin, 2, 195k, 1 - 59. , Automorphe Formen als metrischei1n- var1anten 1, Math Nachr. 1(l9h8), 158 - 212. H. Rademacher, The Fourier series and the functional -..II‘ equation of the absolute modular invariant J(‘C), Amer. J. Math. 61 (1939), 237 - 298. R. A. Rankin, On horocyclic groups, Proc. London Math. Soc. (3) h (195%). 219 - 23%. / H H. Salie, Uber d1e Kloosgermanschen Summon S(u,v;q), Math. Zelt. 3“ (1932)’ 91 - 1090 E. C. Titchmarsh, The Theory of Functions, Second Edition, Oxford Univ. Press, 1952. -1ou- 17. A. Weil, On some exponential sums, Proc. Nat. Acad. Sci. U. S. A. 3% (1998), 20% - 207. 18. E. T. Whittaker, and G. N. Watson, Course of Modern Analysis, Fourth Edition, Cambridge, 1958. l I I, I! I'll Ill ll I'll III II I I l‘ Illlll' l I I! I! l '1 I i I I II II I I I III- II! IIHIINHIHHIIWH 174 9660 3 1293 03