Perspectives on Mock Modular Forms
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The Five Fundamental Operations of Mathematics: Addition, Subtraction
The five fundamental operations of mathematics: addition, subtraction, multiplication, division, and modular forms Kenneth A. Ribet UC Berkeley Trinity University March 31, 2008 Kenneth A. Ribet Five fundamental operations This talk is about counting, and it’s about solving equations. Counting is a very familiar activity in mathematics. Many universities teach sophomore-level courses on discrete mathematics that turn out to be mostly about counting. For example, we ask our students to find the number of different ways of constituting a bag of a dozen lollipops if there are 5 different flavors. (The answer is 1820, I think.) Kenneth A. Ribet Five fundamental operations Solving equations is even more of a flagship activity for mathematicians. At a mathematics conference at Sundance, Robert Redford told a group of my colleagues “I hope you solve all your equations”! The kind of equations that I like to solve are Diophantine equations. Diophantus of Alexandria (third century AD) was Robert Redford’s kind of mathematician. This “father of algebra” focused on the solution to algebraic equations, especially in contexts where the solutions are constrained to be whole numbers or fractions. Kenneth A. Ribet Five fundamental operations Here’s a typical example. Consider the equation y 2 = x3 + 1. In an algebra or high school class, we might graph this equation in the plane; there’s little challenge. But what if we ask for solutions in integers (i.e., whole numbers)? It is relatively easy to discover the solutions (0; ±1), (−1; 0) and (2; ±3), and Diophantus might have asked if there are any more. -
Arxiv:2003.01675V1 [Math.NT] 3 Mar 2020 of Their Locations
DIVISORS OF MODULAR PARAMETRIZATIONS OF ELLIPTIC CURVES MICHAEL GRIFFIN AND JONATHAN HALES Abstract. The modularity theorem implies that for every elliptic curve E=Q there exist rational maps from the modular curve X0(N) to E, where N is the conductor of E. These maps may be expressed in terms of pairs of modular functions X(z) and Y (z) where X(z) and Y (z) satisfy the Weierstrass equation for E as well as a certain differential equation. Using these two relations, a recursive algorithm can be used to calculate the q - expansions of these parametrizations at any cusp. Using these functions, we determine the divisor of the parametrization and the preimage of rational points on E. We give a sufficient condition for when these preimages correspond to CM points on X0(N). We also examine a connection between the al- gebras generated by these functions for related elliptic curves, and describe sufficient conditions to determine congruences in the q-expansions of these objects. 1. Introduction and statement of results The modularity theorem [2, 12] guarantees that for every elliptic curve E of con- ductor N there exists a weight 2 newform fE of level N with Fourier coefficients in Z. The Eichler integral of fE (see (3)) and the Weierstrass }-function together give a rational map from the modular curve X0(N) to the coordinates of some model of E: This parametrization has singularities wherever the value of the Eichler integral is in the period lattice. Kodgis [6] showed computationally that many of the zeros of the Eichler integral occur at CM points. -
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 + .. -
An Approach to BPS Black Hole Microstate Counting in an N= 2 STU
An approach to BPS black hole microstate counting in an N = 2 STU model G. L. Cardoso, S. Nampuri and D. Polini Center for Mathematical Analysis, Geometry and Dynamical Systems, Department of Mathematics, Instituto Superior T´ecnico, Universidade de Lisboa, Av. Rovisco Pais, 1049-001 Lisboa, Portugal [email protected], [email protected], [email protected] ABSTRACT We consider four-dimensional dyonic single-center BPS black holes in the N = 2 STU model of Sen and Vafa. By working in a region of moduli space where the real part of two of the three complex scalars S; T; U are taken to be large, we evaluate the quantum entropy function for these BPS black holes. In this regime, the subleading corrections point to a microstate counting formula partly based on a Siegel modular form of weight two. This is supplemented by another modular object that takes into account the dependence on Y 0, a complex scalar field belonging to one of the four off-shell vector multiplets of the underlying supergravity theory. We also observe interesting connections to the rational Calogero model and to formal deformation of a Poisson algebra, and suggest a string web picture of our counting proposal. arXiv:1903.07586v2 [hep-th] 20 Aug 2020 August 24, 2020 Contents 1 Introduction1 2 Quantum entropy function for BPS black holes in N = 2 supergravity theories 6 2.1 Generic structure6 2.2 Saddle-point approximation9 3 Quantum entropy function for the N = 2 STU model of Sen and Vafa 10 3.1 The N = 2 STU model with χ = 0 11 3.2 Properties -
Quadratic Forms and Automorphic Forms
Quadratic Forms and Automorphic Forms Jonathan Hanke May 16, 2011 2 Contents 1 Background on Quadratic Forms 11 1.1 Notation and Conventions . 11 1.2 Definitions of Quadratic Forms . 11 1.3 Equivalence of Quadratic Forms . 13 1.4 Direct Sums and Scaling . 13 1.5 The Geometry of Quadratic Spaces . 14 1.6 Quadratic Forms over Local Fields . 16 1.7 The Geometry of Quadratic Lattices – Dual Lattices . 18 1.8 Quadratic Forms over Local (p-adic) Rings of Integers . 19 1.9 Local-Global Results for Quadratic forms . 20 1.10 The Neighbor Method . 22 1.10.1 Constructing p-neighbors . 22 2 Theta functions 25 2.1 Definitions and convergence . 25 2.2 Symmetries of the theta function . 26 2.3 Modular Forms . 28 2.4 Asymptotic Statements about rQ(m) ...................... 31 2.5 The circle method and Siegel’s Formula . 32 2.6 Mass Formulas . 34 2.7 An Example: The sum of 4 squares . 35 2.7.1 Canonical measures for local densities . 36 2.7.2 Computing β1(m) ............................ 36 2.7.3 Understanding βp(m) by counting . 37 2.7.4 Computing βp(m) for all primes p ................... 38 2.7.5 Computing rQ(m) for certain m ..................... 39 3 Quaternions and Clifford Algebras 41 3.1 Definitions . 41 3.2 The Clifford Algebra . 45 3 4 CONTENTS 3.3 Connecting algebra and geometry in the orthogonal group . 47 3.4 The Spin Group . 49 3.5 Spinor Equivalence . 52 4 The Theta Lifting 55 4.1 Classical to Adelic modular forms for GL2 .................. -
A Life Inspired by an Unexpected Genius
Quanta Magazine A Life Inspired by an Unexpected Genius The mathematician Ken Ono believes that the story of Srinivasa Ramanujan — mathematical savant and two-time college dropout — holds valuable lessons for how we find and reward hidden genius. By John Pavlus The mathematician Ken Ono in his office at Emory University in Atlanta. For the first 27 years of his life, the mathematician Ken Ono was a screw-up, a disappointment and a failure. At least, that’s how he saw himself. The youngest son of first-generation Japanese immigrants to the United States, Ono grew up under relentless pressure to achieve academically. His parents set an unusually high bar. Ono’s father, an eminent mathematician who accepted an invitation from J. Robert Oppenheimer to join the Institute for Advanced Study in Princeton, N.J., expected his son to follow in his footsteps. Ono’s mother, meanwhile, was a quintessential “tiger parent,” discouraging any interests unrelated to the steady accumulation of scholarly credentials. This intellectual crucible produced the desired results — Ono studied mathematics and launched a promising academic career — but at great emotional cost. As a teenager, Ono became so desperate https://www.quantamagazine.org/the-mathematician-ken-onos-life-inspired-by-ramanujan-20160519/ May 19, 2016 Quanta Magazine to escape his parents’ expectations that he dropped out of high school. He later earned admission to the University of Chicago but had an apathetic attitude toward his studies, preferring to party with his fraternity brothers. He eventually discovered a genuine enthusiasm for mathematics, became a professor, and started a family, but fear of failure still weighed so heavily on Ono that he attempted suicide while attending an academic conference. -
Mock Moonshine by Prof. Kishore Marathe City University of New
Mock Moonshine by Prof. Kishore Marathe City University of New York, Brooklyn College International Conference on Recebt Developments in String Theory Congressi Stefano Franscini - Monte Verita, Switzerland July 21 to 25, 2014 ====================== 1 Thirty years ago some very surprising relations between the Fourier coefficients of the Jacobi Hauptmodul or the J-function and represen- tations of the largest finite simple sporadic group, the Monster were discovered. Precise formulation of these relations is now called the ’Monstrous Moonshine’. It has given rise to a large body of new mathematics. The moonshine correspondence has been extended to other groups revealing unexpected relations to conformal field theory, gravity and string theory in physics and to Ramanujan’s mock theta functions and its extensions in mathe- matics. We call these results which have been discoverd in the last 30 years ’ Mock Moon- shine’. We will survey some recent develop- ments related to Mock Moonshine and indicate directions for future research. 2 List of Topics 1. Some Historical Remarks 2. Modular objects 3. Monstrous Moonshine Conjectures 4. Monstrous Moonshine and Vertex Algebras 5. Moonshine for other groups 6. Mock Moonshine and Field Theories 3 The following historical material is taken from [4]. Recall that a group is called simple if it has no proper non-trivial normal subgroup. Thus an abelian group is simple if and only if it is isomorphic to one of the groups Zp, for p a prime number. This is the simplest example of an infinite family of finite simple groups. An- other infinite family of finite simple groups is the family of alternating groups An,n> 4 that we study in the first course in algebra. -
Fermat, Taniyama–Shimura–Weil and Andrew Wiles, Part I
Fermat, Taniyama–Shimura–Weil and Andrew Wiles, Part I John Rognes University of Oslo, Norway May 13th 2016 The Norwegian Academy of Science and Letters has decided to award the Abel Prize for 2016 to Sir Andrew J. Wiles, University of Oxford for his stunning proof of Fermat’s Last Theorem by way of the modularity conjecture for semistable elliptic curves, opening a new era in number theory. Sir Andrew J. Wiles Sketch proof of Fermat’s Last Theorem: I Frey (1984): A solution ap + bp = cp to Fermat’s equation gives an elliptic curve y 2 = x(x − ap)(x + bp) : I Ribet (1986): The Frey curve does not come from a modular form. I Wiles (1994): Every elliptic curve comes from a modular form. I Hence no solution to Fermat’s equation exists. Point counts and Fourier expansions: Elliptic curve Hasse–Witt ( L6 -function Mellin Modular form Modularity: Elliptic curve ◦ ( ? L6 -function Modular form Wiles’ Modularity Theorem: Semistable elliptic curve defined over Q Wiles ◦ ) 5 L-function Weight 2 modular form Wiles’ Modularity Theorem: Semistable elliptic curve over Q of conductor N ) Wiles ◦ 5L-function Weight 2 modular form of level N Frey Curve (and a special case of Wiles’ theorem): Solution to Fermat’s equation Frey Semistable elliptic curve over Q with peculiar properties ) Wiles ◦ 5 L-function Weight 2 modular form with peculiar properties (A special case of) Ribet’s theorem: Solution to Fermat’s equation Frey Semistable elliptic curve over Q with peculiar properties * Wiles ◦ 4 L-function Weight 2 modular form with peculiar properties O Ribet Weight 2 modular form of level 2 Contradiction: Solution to Fermat’s equation Frey Semistable elliptic curve over Q with peculiar properties * Wiles ◦ 4 L-function Weight 2 modular form with peculiar properties O Ribet Weight 2 modular form of level 2 o Does not exist Blaise Pascal (1623–1662) Je n’ai fait celle-ci plus longue que parce que je n’ai pas eu le loisir de la faire plus courte. -
Modular Forms, the Ramanujan Conjecture and the Jacquet-Langlands Correspondence
Appendix: Modular forms, the Ramanujan conjecture and the Jacquet-Langlands correspondence Jonathan D. Rogawski1) The theory developed in Chapter 7 relies on a fundamental result (Theorem 7 .1.1) asserting that the space L2(f\50(3) x PGLz(Op)) decomposes as a direct sum of tempered, irreducible representations (see definition below). Here 50(3) is the compact Lie group of 3 x 3 orthogonal matrices of determinant one, and r is a discrete group defined by a definite quaternion algebra D over 0 which is split at p. The embedding of r in 50(3) X PGLz(Op) is defined by identifying 50(3) and PGLz(Op) with the groups of real and p-adic points of the projective group D*/0*. Although this temperedness result can be viewed as a combinatorial state ment about the action of the Heckeoperators on the Bruhat-Tits tree associated to PGLz(Op). it is not possible at present to prove it directly. Instead, it is deduced as a corollary of two other results. The first is the Ramanujan-Petersson conjec ture for holomorphic modular forms, proved by P. Deligne [D]. The second is the Jacquet-Langlands correspondence for cuspidal representations of GL(2) and multiplicative groups of quaternion algebras [JL]. The proofs of these two results involve essentially disjoint sets of techniques. Deligne's theorem is proved using the Riemann hypothesis for varieties over finite fields (also proved by Deligne) and thus relies on characteristic p algebraic geometry. By contrast, the Jacquet Langlands Theorem is analytic in nature. The main tool in its proof is the Seiberg trace formula. -
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. -
Congruences Between Modular Forms
CONGRUENCES BETWEEN MODULAR FORMS FRANK CALEGARI Contents 1. Basics 1 1.1. Introduction 1 1.2. What is a modular form? 4 1.3. The q-expansion priniciple 14 1.4. Hecke operators 14 1.5. The Frobenius morphism 18 1.6. The Hasse invariant 18 1.7. The Cartier operator on curves 19 1.8. Lifting the Hasse invariant 20 2. p-adic modular forms 20 2.1. p-adic modular forms: The Serre approach 20 2.2. The ordinary projection 24 2.3. Why p-adic modular forms are not good enough 25 3. The canonical subgroup 26 3.1. Canonical subgroups for general p 28 3.2. The curves Xrig[r] 29 3.3. The reason everything works 31 3.4. Overconvergent p-adic modular forms 33 3.5. Compact operators and spectral expansions 33 3.6. Classical Forms 35 3.7. The characteristic power series 36 3.8. The Spectral conjecture 36 3.9. The invariant pairing 38 3.10. A special case of the spectral conjecture 39 3.11. Some heuristics 40 4. Examples 41 4.1. An example: N = 1 and p = 2; the Watson approach 41 4.2. An example: N = 1 and p = 2; the Coleman approach 42 4.3. An example: the coefficients of c(n) modulo powers of p 43 4.4. An example: convergence slower than O(pn) 44 4.5. Forms of half integral weight 45 4.6. An example: congruences for p(n) modulo powers of p 45 4.7. An example: congruences for the partition function modulo powers of 5 47 4.8. -
25 Modular Forms and L-Series
18.783 Elliptic Curves Spring 2015 Lecture #25 05/12/2015 25 Modular forms and L-series As we will show in the next lecture, Fermat's Last Theorem is a direct consequence of the following theorem [11, 12]. Theorem 25.1 (Taylor-Wiles). Every semistable elliptic curve E=Q is modular. In fact, as a result of subsequent work [3], we now have the stronger result, proving what was previously known as the modularity conjecture (or Taniyama-Shimura-Weil conjecture). Theorem 25.2 (Breuil-Conrad-Diamond-Taylor). Every elliptic curve E=Q is modular. Our goal in this lecture is to explain what it means for an elliptic curve over Q to be modular (we will also define the term semistable). This requires us to delve briefly into the theory of modular forms. Our goal in doing so is simply to understand the definitions and the terminology; we will omit all but the most straight-forward proofs. 25.1 Modular forms Definition 25.3. A holomorphic function f : H ! C is a weak modular form of weight k for a congruence subgroup Γ if f(γτ) = (cτ + d)kf(τ) a b for all γ = c d 2 Γ. The j-function j(τ) is a weak modular form of weight 0 for SL2(Z), and j(Nτ) is a weak modular form of weight 0 for Γ0(N). For an example of a weak modular form of positive weight, recall the Eisenstein series X0 1 X0 1 G (τ) := G ([1; τ]) := = ; k k !k (m + nτ)k !2[1,τ] m;n2Z 1 which, for k ≥ 3, is a weak modular form of weight k for SL2(Z).