Mock Theta Functions and Quantum Modular Forms
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Traces of Reciprocal Singular Moduli, We Require the Theta Functions
TRACES OF RECIPROCAL SINGULAR MODULI CLAUDIA ALFES-NEUMANN AND MARKUS SCHWAGENSCHEIDT Abstract. We show that the generating series of traces of reciprocal singular moduli is a mixed mock modular form of weight 3/2 whose shadow is given by a linear combination of products of unary and binary theta functions. To prove these results, we extend the Kudla-Millson theta lift of Bruinier and Funke to meromorphic modular functions. 1. Introduction and statement of results The special values of the modular j-invariant 1 2 3 j(z)= q− + 744 + 196884q + 21493760q + 864299970q + ... at imaginary quadratic points in the upper half-plane are called singular moduli. By the theory of complex multiplication they are algebraic integers in the ray class fields of certain orders in imaginary quadratic fields. In particular, their traces j(zQ) trj(D)= ΓQ Q + /Γ ∈QXD | | are known to be rational integers. Here + denotes the set of positive definite quadratic QD forms of discriminant D < 0, on which Γ = SL2(Z) acts with finitely many orbits. Further, ΓQ is the stabilizer of Q in Γ = PSL2(Z) and zQ H is the CM point associated to Q. In his seminal paper “Traces of singular moduli”∈ (see [Zag02]) Zagier showed that the generating series 1 D 1 3 4 7 8 q− 2 tr (D)q− = q− 2+248q 492q + 4119q 7256q + ... − − J − − − D<X0 arXiv:1905.07944v2 [math.NT] 2 Apr 2020 of traces of CM values of J = j 744 is a weakly holomorphic modular form of weight − 3/2 for Γ0(4). It follows from this result, by adding a multiple of Zagier’s mock modular Eisenstein series of weight 3/2 (see [Zag75]), that the generating series 1 D 1 4 7 8 q− + 60 tr (D)q− = q− + 60 864q + 3375q 8000q + .. -
Lectures on Modular Forms. Fall 1997/98
Lectures on Modular Forms. Fall 1997/98 Igor V. Dolgachev October 26, 2017 ii Contents 1 Binary Quadratic Forms1 2 Complex Tori 13 3 Theta Functions 25 4 Theta Constants 43 5 Transformations of Theta Functions 53 6 Modular Forms 63 7 The Algebra of Modular Forms 83 8 The Modular Curve 97 9 Absolute Invariant and Cross-Ratio 115 10 The Modular Equation 121 11 Hecke Operators 133 12 Dirichlet Series 147 13 The Shimura-Tanyama-Weil Conjecture 159 iii iv CONTENTS Lecture 1 Binary Quadratic Forms 1.1 The theory of modular form originates from the work of Carl Friedrich Gauss of 1831 in which he gave a geometrical interpretation of some basic no- tions of number theory. Let us start with choosing two non-proportional vectors v = (v1; v2) and w = 2 (w1; w2) in R The set of vectors 2 Λ = Zv + Zw := fm1v + m2w 2 R j m1; m2 2 Zg forms a lattice in R2, i.e., a free subgroup of rank 2 of the additive group of the vector space R2. We picture it as follows: • • • • • • •Gv • ••• •• • w • • • • • • • • Figure 1.1: Lattice in R2 1 2 LECTURE 1. BINARY QUADRATIC FORMS Let v v B(v; w) = 1 2 w1 w2 and v · v v · w G(v; w) = = B(v; w) · tB(v; w): v · w w · w be the Gram matrix of (v; w). The area A(v; w) of the parallelogram formed by the vectors v and w is given by the formula v · v v · w A(v; w)2 = det G(v; w) = (det B(v; w))2 = det : v · w w · w Let x = mv + nw 2 Λ. -
Abelian Solutions of the Soliton Equations and Riemann–Schottky Problems
Russian Math. Surveys 63:6 1011–1022 c 2008 RAS(DoM) and LMS Uspekhi Mat. Nauk 63:6 19–30 DOI 10.1070/RM2008v063n06ABEH004576 Abelian solutions of the soliton equations and Riemann–Schottky problems I. M. Krichever Abstract. The present article is an exposition of the author’s talk at the conference dedicated to the 70th birthday of S. P. Novikov. The talk con- tained the proof of Welters’ conjecture which proposes a solution of the clas- sical Riemann–Schottky problem of characterizing the Jacobians of smooth algebraic curves in terms of the existence of a trisecant of the associated Kummer variety, and a solution of another classical problem of algebraic geometry, that of characterizing the Prym varieties of unramified covers. Contents 1. Introduction 1011 2. Welters’ trisecant conjecture 1014 3. The problem of characterization of Prym varieties 1017 4. Abelian solutions of the soliton equations 1018 Bibliography 1020 1. Introduction The famous Novikov conjecture which asserts that the Jacobians of smooth alge- braic curves are precisely those indecomposable principally polarized Abelian vari- eties whose theta-functions provide explicit solutions of the Kadomtsev–Petviashvili (KP) equation, fundamentally changed the relations between the classical algebraic geometry of Riemann surfaces and the theory of soliton equations. It turns out that the finite-gap, or algebro-geometric, theory of integration of non-linear equa- tions developed in the mid-1970s can provide a powerful tool for approaching the fundamental problems of the geometry of Abelian varieties. The basic tool of the general construction proposed by the author [1], [2]which g+k 1 establishes a correspondence between algebro-geometric data Γ,Pα,zα,S − (Γ) and solutions of some soliton equation, is the notion of Baker–Akhiezer{ function.} Here Γis a smooth algebraic curve of genus g with marked points Pα, in whose g+k 1 neighborhoods we fix local coordinates zα, and S − (Γ) is a symmetric prod- uct of the curve. -
Mirror Symmetry of Abelian Variety and Multi Theta Functions
1 Mirror symmetry of Abelian variety and Multi Theta functions by Kenji FUKAYA (深谷賢治) Department of Mathematics, Faculty of Science, Kyoto University, Kitashirakawa, Sakyo-ku, Kyoto Japan Table of contents § 0 Introduction. § 1 Moduli spaces of Lagrangian submanifolds and construction of a mirror torus. § 2 Construction of a sheaf from an affine Lagrangian submanifold. § 3 Sheaf cohomology and Floer cohomology 1 (Construction of a homomorphism). § 4 Isogeny. § 5 Sheaf cohomology and Floer cohomology 2 (Proof of isomorphism). § 6 Extension and Floer cohomology 1 (0 th cohomology). § 7 Moduli space of holomorphic vector bundles on a mirror torus. § 8 Nontransversal or disconnected Lagrangian submanifolds. ∞ § 9 Multi Theta series 1 (Definition and A formulae.) § 10 Multi Theta series 2 (Calculation of the coefficients.) § 11 Extension and Floer cohomology 2 (Higher cohomology). § 12 Resolution and Lagrangian surgery. 2 § 0 Introduction In this paper, we study mirror symmetry of complex and symplectic tori as an example of homological mirror symmetry conjecture of Kontsevich [24], [25] between symplectic and complex manifolds. We discussed mirror symmetry of tori in [12] emphasizing its “noncom- mutative” generalization. In this paper, we concentrate on the case of a commutative (usual) torus. Our result is a generalization of one by Polishchuk and Zaslow [42], [41], who studied the case of elliptic curve. The main results of this paper establish a dictionary of mirror symmetry between symplectic geometry and complex geometry in the case of tori of arbitrary dimension. We wrote this dictionary in the introduction of [12]. We present the argument in a way so that it suggests a possibility of its generalization. -
Arxiv:1906.07410V4 [Math.NT] 29 Sep 2020 Ainlpwrof Power Rational Ftetidodrmc Ht Function Theta Mock Applications
MOCK MODULAR EISENSTEIN SERIES WITH NEBENTYPUS MICHAEL H. MERTENS, KEN ONO, AND LARRY ROLEN In celebration of Bruce Berndt’s 80th birthday Abstract. By the theory of Eisenstein series, generating functions of various divisor functions arise as modular forms. It is natural to ask whether further divisor functions arise systematically in the theory of mock modular forms. We establish, using the method of Zagier and Zwegers on holomorphic projection, that this is indeed the case for certain (twisted) “small divisors” summatory functions sm σψ (n). More precisely, in terms of the weight 2 quasimodular Eisenstein series E2(τ) and a generic Shimura theta function θψ(τ), we show that there is a constant αψ for which ∞ E + · E2(τ) 1 sm n ψ (τ) := αψ + X σψ (n)q θψ(τ) θψ(τ) n=1 is a half integral weight (polar) mock modular form. These include generating functions for combinato- rial objects such as the Andrews spt-function and the “consecutive parts” partition function. Finally, in analogy with Serre’s result that the weight 2 Eisenstein series is a p-adic modular form, we show that these forms possess canonical congruences with modular forms. 1. Introduction and statement of results In the theory of mock theta functions and its applications to combinatorics as developed by Andrews, Hickerson, Watson, and many others, various formulas for q-series representations have played an important role. For instance, the generating function R(ζ; q) for partitions organized by their ranks is given by: n n n2 n (3 +1) m n q 1 ζ ( 1) q 2 R(ζ; q) := N(m,n)ζ q = −1 = − − n , (ζq; q)n(ζ q; q)n (q; q)∞ 1 ζq n≥0 n≥0 n∈Z − mX∈Z X X where N(m,n) is the number of partitions of n of rank m and (a; q) := n−1(1 aqj) is the usual n j=0 − q-Pochhammer symbol. -
Theta Function Review G = 1 Case
The genus 1 case - review Theta Function Review g = 1 case We recall the main de¯nitions of theta functions in the 1-dim'l case: De¯nition 0 Let· ¿ 2¸C such that Im¿ > 0: For "; " real numbers and z 2 C then: " £ (z;¿) = "0 n ¡ ¢ ¡ ¢ ¡ ¢ ³ ´o P 1 " " ² t ²0 l²Z2 exp2¼i 2 l + 2 ¿ l + 2 + l + 2 z + 2 The series· is uniformly¸ and absolutely convergent on compact subsets " C £ H: are called Theta characteristics "0 The genus 1 case - review Theta Function Properties Review for g = 1 case the following properties of theta functions can be obtained by manipulation of the series : · ¸ · ¸ " + 2m " 1. £ (z;¿) = exp¼i f"eg £ (z;¿) and e; m 2 Z "0 + 2e "0 · ¸ · ¸ " " 2. £ (z;¿) = £ (¡z;¿) ¡"0 "0 · ¸ " 3. £ (z + n + m¿; ¿) = "0 n o · ¸ t t 0 " exp 2¼i n "¡m " ¡ mz ¡ m2¿ £ (z;¿) 2 "0 The genus 1 case - review Remarks on the properties of Theta functions g=1 1. Property number 3 describes the transformation properties of theta functions under an element of the lattice L¿ generated by f1;¿g. 2. The same property implies that that the zeros of theta functions are well de¯ned on the torus given· ¸ by C=L¿ : In fact there is only a " unique such 0 for each £ (z;¿): "0 · ¸ · ¸ "i γj 3. Let 0 ; i = 1:::k and 0 ; j = 1:::l and "i γj 2 3 Q "i k θ4 5(z;¿) ³P ´ ³P ´ i=1 "0 k 0 l 0 2 i 3 "i + " ¿ ¡ γj + γ ¿ 2 L¿ Then i=1 i j=1 j Q l 4 γj 5 j=1 θ 0 (z;¿) γj is a meromorphic function on the elliptic curve de¯ned by C=L¿ : The genus 1 case - review Analytic vs. -
Theta Function Identities
JOURNAL OF MATHEMATICAL ANALYSIS AND APPLICATIONS 147, 97-121 (1990) Theta Function Identities RONALD J. EVANS Deparlment of Mathematics, University of California, San Diego, La Jolla, California 92093 Submitted by Bruce C. Berndt Received June 3. 1988 1. INTR~D~JcTI~N By 1986, all but one of the identities in the 21 chapters of Ramanujan’s Second Notebook [lo] had been proved; see Berndt’s books [Z-4]. The remaining identity, which we will prove in Theorem 5.1 below, is [ 10, Chap. 20, Entry 8(i)] 1 1 1 V2(Z/P) (1.1) G,(z) G&l + G&J G&J + G&l G,(z) = 4 + dz) ’ where q(z) is the classical eta function given by (2.5) and 2 f( _ q2miP, - q1 - WP) G,(z) = G,,,(z) = (- 1)” qm(3m-p)‘(2p) f(-qm,p, -q,-m,p) 9 (1.2) with q = exp(2niz), p = 13, and Cl(k2+k)/2 (k2pkV2 B . (1.3) k=--13 The author is grateful to Bruce Berndt for bringing (1.1) to his attention. The quotients G,(z) in (1.2) for odd p have been the subject of interest- ing investigations by Ramanujan and others. Ramanujan [ 11, p. 2071 explicitly wrote down a version of the famous quintuple product identity, f(-s’, +)J-(-~*q3, -w?+qfF~, -A2q9) (1.4) f(-43 -Q2) f(-Aq3, -Pq6) ’ which yields as a special case a formula for q(z) G,(z) as a linear combina- tion of two theta functions; see (1.7). In Chapter 16 of his Second 97 0022-247X/90 $3.00 Copyright % 1993 by Academc Press, Inc. -
An Addition Formula for the Jacobian Theta Function and Its Applications
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Advances in Mathematics 212 (2007) 389–406 www.elsevier.com/locate/aim An addition formula for the Jacobian theta function and its applications Zhi-Guo Liu 1 East China Normal University, Department of Mathematics, Shanghai 200062, People’s Republic of China Received 13 July 2005; accepted 17 October 2006 Available online 28 November 2006 Communicated by Alain Lascoux Abstract In this paper, we prove an addition formula for the Jacobian theta function using the theory of elliptic functions. It turns out to be a fundamental identity in the theory of theta functions and elliptic function, and unifies many important results about theta functions and elliptic functions. From this identity we can derive the Ramanujan cubic theta function identity, Winquist’s identity, a theta function identities with five parameters, and many other interesting theta function identities; and all of which are as striking as Winquist’s identity. This identity allows us to give a new proof of the addition formula for the Weierstrass sigma function. A new identity about the Ramanujan cubic elliptic function is given. The proofs are self contained and elementary. © 2006 Elsevier Inc. All rights reserved. MSC: 11F11; 11F12; 11F27; 33E05 Keywords: Weierstrass sigma function; Addition formula; Elliptic functions; Jacobi’s theta function; Winquist’s identity; Ramanujan’s cubic theta function theory E-mail addresses: [email protected], [email protected]. 1 The author was supported in part by the National Science Foundation of China. 0001-8708/$ – see front matter © 2006 Elsevier Inc. -
P-Adic Analysis and Mock Modular Forms
P -ADIC ANALYSIS AND MOCK MODULAR FORMS A DISSERTATION SUBMITTED TO THE GRADUATE DIVISION OF THE UNIVERSITY OF HAWAI`I IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF DOCTOR OF PHILOSOPHY IN MATHEMATICS AUGUST 2010 By Zachary A. Kent Dissertation Committee: Pavel Guerzhoy, Chairperson Christopher Allday Ron Brown Karl Heinz Dovermann Theresa Greaney Abstract A mock modular form f + is the holomorphic part of a harmonic Maass form f. The non-holomorphic part of f is a period integral of a cusp form g, which we call the shadow of f +. The study of mock modular forms and mock theta functions is one of the most active areas in number theory with important works by Bringmann, Ono, Zagier, Zwegers, among many others. The theory has many wide-ranging applica- tions: additive number theory, elliptic curves, mathematical physics, representation theory, and many others. We consider arithmetic properties of mock modular forms in three different set- tings: zeros of a certain family of modular forms, coupling the Fourier coefficients of mock modular forms and their shadows, and critical values of modular L-functions. For a prime p > 3, we consider j-zeros of a certain family of modular forms called Eisenstein series. When the weight of the Eisenstein series is p − 1, the j-zeros are j-invariants of elliptic curves with supersingular reduction modulo p. We lift these j-zeros to a p-adic field, and show that when the weights of two Eisenstein series are p-adically close, then there are j-zeros of both series that are p-adically close. -
Transformation Groups for Soliton Equations V —
Publ. RIMS, Kyoto Univ. 18 (1982), 1111-1119 Quasi- Periodic Solutions of the Orthogonal KP Equation — Transformation Groups for Soliton Equations V — By Etsuro DATE*, Michio JIMBO?, Masaki KASHIWARAI and Tetsuji MiWAf § 0. Introduction In this note we study quasi-periodic solutions of the BKP hierarchy in- troduced in [1]. Our main result is the Theorem in Section 2, which states that quasi-periodic T-functions for the BKP hierarchy are the theta functions on the Prym varieties of algebraic curves admitting involutions with two fixed points. The rational and soliton solutions of the BKP hierarchy were studied in part IV [2] together with its operator formalism. We also showed that the BKP hierarchy is the compatibility condition for the following system of linear equations for w(x), x = (xl9 x3, .T5,...)^ (1) ^7=B'W' '='.3,5,... where 5, is a linear ordinary differential operator with respect to XL without constant term. dl l~2 dm One of the specific properties of the BKP hierarchy is the fact that squares of T-functions for the BKP hierarchy are T-functions for the KP hierarchy with x2j- = 0. Now we explain why the Prym varieties and the theta functions on them ap- pear in our present study. Received November 20, 1981. Faculty of General Education, Kyoto University, Kyoto 606, Japan. Research Institute for Mathematical Sciences, Kyoto University, Kyoto 606, Japan. 1112 ETSURO DATE, MICHIO JIMBO, MASAKI KASHIWARA AND TETSUJI MIWA One derivation is given through the examination of the geometrical prop- erties of the wave functions associated with soliton solutions. -
2D Theta Functions and Crystallization Among Bravais Lattices Laurent Bétermin
2D Theta Functions and Crystallization among Bravais Lattices Laurent Bétermin To cite this version: Laurent Bétermin. 2D Theta Functions and Crystallization among Bravais Lattices. 2015. hal- 01116262v2 HAL Id: hal-01116262 https://hal.archives-ouvertes.fr/hal-01116262v2 Preprint submitted on 9 Apr 2015 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Distributed under a Creative Commons Attribution - NonCommercial| 4.0 International License 2D Theta Functions and Crystallization among Bravais Lattices Laurent B´etermin∗ Universit´eParis-Est Cr´eteil LAMA - CNRS UMR 8050 61, Avenue du G´en´eral de Gaulle, 94010 Cr´eteil, France April 9, 2015 Abstract In this paper, we study minimization problems among Bravais lattices for finite energy per point. We prove – as claimed by Cohn and Kumar – that if a function is completely monotonic, then the triangular lattice minimizes energy per particle among Bravais lattices with density fixed for any density. Furthermore we give an example of convex decreasing positive potential for which triangular lattice is not a minimizer for some densities. We use the Montgomery method presented in our previous work to prove minimality of triangular lattice among Bravais lattices at high density for some general potentials. -
The Riemann Zeta Function and Its Functional Equation (And a Review of the Gamma Function and Poisson Summation)
Math 259: Introduction to Analytic Number Theory The Riemann zeta function and its functional equation (and a review of the Gamma function and Poisson summation) Recall Euler's identity: 1 1 1 s 0 cps1 [ζ(s) :=] n− = p− = s : (1) X Y X Y 1 p− n=1 p prime @cp=1 A p prime − We showed that this holds as an identity between absolutely convergent sums and products for real s > 1. Riemann's insight was to consider (1) as an identity between functions of a complex variable s. We follow the curious but nearly universal convention of writing the real and imaginary parts of s as σ and t, so s = σ + it: s σ We already observed that for all real n > 0 we have n− = n− , because j j s σ it log n n− = exp( s log n) = n− e − and eit log n has absolute value 1; and that both sides of (1) converge absolutely in the half-plane σ > 1, and are equal there either by analytic continuation from the real ray t = 0 or by the same proof we used for the real case. Riemann showed that the function ζ(s) extends from that half-plane to a meromorphic function on all of C (the \Riemann zeta function"), analytic except for a simple pole at s = 1. The continuation to σ > 0 is readily obtained from our formula n+1 n+1 1 1 s s 1 s s ζ(s) = n− Z x− dx = Z (n− x− ) dx; − s 1 X − X − − n=1 n n=1 n since for x [n; n + 1] (n 1) and σ > 0 we have 2 ≥ x s s 1 s 1 σ n− x− = s Z y− − dy s n− − j − j ≤ j j n so the formula for ζ(s) (1=(s 1)) is a sum of analytic functions converging absolutely in compact subsets− of− σ + it : σ > 0 and thus gives an analytic function there.