The Spectrum of the Laplacian on Γ\H & the Trace Formula
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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. -
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). -
The Role of the Ramanujan Conjecture in Analytic Number Theory
BULLETIN (New Series) OF THE AMERICAN MATHEMATICAL SOCIETY Volume 50, Number 2, April 2013, Pages 267–320 S 0273-0979(2013)01404-6 Article electronically published on January 14, 2013 THE ROLE OF THE RAMANUJAN CONJECTURE IN ANALYTIC NUMBER THEORY VALENTIN BLOMER AND FARRELL BRUMLEY Dedicated to the 125th birthday of Srinivasa Ramanujan Abstract. We discuss progress towards the Ramanujan conjecture for the group GLn and its relation to various other topics in analytic number theory. Contents 1. Introduction 267 2. Background on Maaß forms 270 3. The Ramanujan conjecture for Maaß forms 276 4. The Ramanujan conjecture for GLn 283 5. Numerical improvements towards the Ramanujan conjecture and applications 290 6. L-functions 294 7. Techniques over Q 298 8. Techniques over number fields 302 9. Perspectives 305 J.-P. Serre’s 1981 letter to J.-M. Deshouillers 307 Acknowledgments 313 About the authors 313 References 313 1. Introduction In a remarkable article [111], published in 1916, Ramanujan considered the func- tion ∞ ∞ Δ(z)=(2π)12e2πiz (1 − e2πinz)24 =(2π)12 τ(n)e2πinz, n=1 n=1 where z ∈ H = {z ∈ C |z>0} is in the upper half-plane. The right hand side is understood as a definition for the arithmetic function τ(n) that nowadays bears Received by the editors June 8, 2012. 2010 Mathematics Subject Classification. Primary 11F70. Key words and phrases. Ramanujan conjecture, L-functions, number fields, non-vanishing, functoriality. The first author was supported by the Volkswagen Foundation and a Starting Grant of the European Research Council. The second author is partially supported by the ANR grant ArShiFo ANR-BLANC-114-2010 and by the Advanced Research Grant 228304 from the European Research Council. -
Modular Forms and Affine Lie Algebras
Modular Forms Theta functions Comparison with the Weyl denominator Modular Forms and Affine Lie Algebras Daniel Bump F TF i 2πi=3 e SF Modular Forms Theta functions Comparison with the Weyl denominator The plan of this course This course will cover the representation theory of a class of Lie algebras called affine Lie algebras. But they are a special case of a more general class of infinite-dimensional Lie algebras called Kac-Moody Lie algebras. Both classes were discovered in the 1970’s, independently by Victor Kac and Robert Moody. Kac at least was motivated by mathematical physics. Most of the material we will cover is in Kac’ book Infinite-dimensional Lie algebras which you should be able to access on-line through the Stanford libraries. In this class we will develop general Kac-Moody theory before specializing to the affine case. Our goal in this first part will be Kac’ generalization of the Weyl character formula to certain infinite-dimensional representations of infinite-dimensional Lie algebras. Modular Forms Theta functions Comparison with the Weyl denominator Affine Lie algebras and modular forms The Kac-Moody theory includes finite-dimensional simple Lie algebras, and many infinite-dimensional classes. The best understood Kac-Moody Lie algebras are the affine Lie algebras and after we have developed the Kac-Moody theory in general we will specialize to the affine case. We will see that the characters of affine Lie algebras are modular forms. We will not reach this topic until later in the course so in today’s introductory lecture we will talk a little about modular forms, without giving complete proofs, to show where we are headed. -
Modular Dedekind Symbols Associated to Fuchsian Groups and Higher-Order Eisenstein Series
Modular Dedekind symbols associated to Fuchsian groups and higher-order Eisenstein series Jay Jorgenson,∗ Cormac O’Sullivan†and Lejla Smajlovi´c May 20, 2018 Abstract Let E(z,s) be the non-holomorphic Eisenstein series for the modular group SL(2, Z). The classical Kro- necker limit formula shows that the second term in the Laurent expansion at s = 1 of E(z,s) is essentially the logarithm of the Dedekind eta function. This eta function is a weight 1/2 modular form and Dedekind expressedits multiplier system in terms of Dedekind sums. Building on work of Goldstein, we extend these results from the modular group to more general Fuchsian groups Γ. The analogue of the eta function has a multiplier system that may be expressed in terms of a map S : Γ → R which we call a modular Dedekind symbol. We obtain detailed properties of these symbols by means of the limit formula. Twisting the usual Eisenstein series with powers of additive homomorphisms from Γ to C produces higher-order Eisenstein series. These series share many of the properties of E(z,s) though they have a more complicated automorphy condition. They satisfy a Kronecker limit formula and produce higher- order Dedekind symbols S∗ :Γ → R. As an application of our general results, we prove that higher-order Dedekind symbols associated to genus one congruence groups Γ0(N) are rational. 1 Introduction 1.1 Kronecker limit functions and Dedekind sums Write elements of the upper half plane H as z = x + iy with y > 0. The non-holomorphic Eisenstein series E (s,z), associated to the full modular group SL(2, Z), may be given as ∞ 1 ys E (z,s) := . -
18.785 Notes
Contents 1 Introduction 4 1.1 What is an automorphic form? . 4 1.2 A rough definition of automorphic forms on Lie groups . 5 1.3 Specializing to G = SL(2; R)....................... 5 1.4 Goals for the course . 7 1.5 Recommended Reading . 7 2 Automorphic forms from elliptic functions 8 2.1 Elliptic Functions . 8 2.2 Constructing elliptic functions . 9 2.3 Examples of Automorphic Forms: Eisenstein Series . 14 2.4 The Fourier expansion of G2k ...................... 17 2.5 The j-function and elliptic curves . 19 3 The geometry of the upper half plane 19 3.1 The topological space ΓnH ........................ 20 3.2 Discrete subgroups of SL(2; R) ..................... 22 3.3 Arithmetic subgroups of SL(2; Q).................... 23 3.4 Linear fractional transformations . 24 3.5 Example: the structure of SL(2; Z)................... 27 3.6 Fundamental domains . 28 3.7 ΓnH∗ as a topological space . 31 3.8 ΓnH∗ as a Riemann surface . 34 3.9 A few basics about compact Riemann surfaces . 35 3.10 The genus of X(Γ) . 37 4 Automorphic Forms for Fuchsian Groups 40 4.1 A general definition of classical automorphic forms . 40 4.2 Dimensions of spaces of modular forms . 42 4.3 The Riemann-Roch theorem . 43 4.4 Proof of dimension formulas . 44 4.5 Modular forms as sections of line bundles . 46 4.6 Poincar´eSeries . 48 4.7 Fourier coefficients of Poincar´eseries . 50 4.8 The Hilbert space of cusp forms . 54 4.9 Basic estimates for Kloosterman sums . 56 4.10 The size of Fourier coefficients for general cusp forms . -
1 Second Facts About Spaces of Modular Forms
April 30, 2:00 pm 1 Second Facts About Spaces of Modular Forms We have repeatedly used facts about the dimensions of the space of modular forms, mostly to give specific examples of and relations between modular forms of a given weight. We now prove these results in this section. Recall that a modular form f of weight 0 is a holomorphic function that is invari- ant under the action of SL(2, Z) and whose domain can be extended to include the point at infinity. Hence, we may regard f as a holomorphic function on the compact Riemann surface G\H∗, where H∗ = H ∪ {∞}. If you haven’t had a course in com- plex analysis, you shouldn’t worry too much about this statement. We’re really just saying that our fundamental domain can be understood as a compact manifold with complex structure. So locally, we look like C and there are compatibility conditions on overlapping local maps. By the maximum modulus principle from complex analysis (see section 3.4 of Ahlfors for example), any such holomorphic function must be constant. We can use this fact, together with the fact that given f1, f2 ∈ M2k, then f1/f2 is a meromorphic function invariant under G (i.e. a weakly modular function of weight 0). Usually, one proves facts about the dimensions of spaces of modular forms using foundational algebraic geometry (the Riemann-Roch theorem, in particular) or the Selberg trace formula (an even more technical result relating differential geometry to harmonic analysis in a beautiful way). These apply to spaces of modular forms for other groups, but as we’re only going to say a few words about such spaces, we won’t delve into either, but rather prove a much simpler result in the spirit of the Riemann-Roch theorem. -
Elliptic Curves and Modular Forms
ALGANT Master Thesis - July 2018 Elliptic Curves and Modular Forms Candidate Francesco Bruzzesi Advisor Prof. Dr. Marc N. Levine Universit´adegli Studi di Milano Universit¨atDuisburg{Essen Introduction The thesis has the aim to study the Eichler-Shimura construction associating elliptic curves to weight-2 modular forms for Γ0(N): this is the perfect topic to combine and develop further results from three courses I took in the first semester of the academic year 2017-18 at Universit¨atDuisburg-Essen (namely the courses of modular forms, abelian varieties and complex multiplication). Chapter 1 gives a brief overview on the algebraic geometry results and tools we will need along the whole thesis. Chapter 2 introduces and develops the theory of elliptic curves, firstly as an algebraic curve over a generic field, and then focusing on the fields of complex and rational numbers, in particular for the latter case we will be able to define an L-function associated to an elliptic curve. As we move to Chapter 3 we shift our focus to the theory of modular forms. We first treat elementary results and their consequences, then we seehow it is possible to define the canonical model of the modular curve X0(N) over Q, and the integrality property of the j-invariant. Chapter 4 concerns Hecke operators: Shimura's book [Shi73 Chapter 3] introduces the Hecke ring and its properties in full generality, on the other hand the other two main references for the chapter [DS06 Chapter 5] and [Kna93 Chapters XIII & IX] do not introduce the Hecke ring at all, and its attributes (such as commutativity for the case of interests) are proved by explicit computation. -
The Modularity Theorem
R. van Dobben de Bruyn The Modularity Theorem Bachelor's thesis, June 21, 2011 Supervisors: Dr R.M. van Luijk, Dr C. Salgado Mathematisch Instituut, Universiteit Leiden Contents Introduction4 1 Elliptic Curves6 1.1 Definitions and Examples......................6 1.2 Minimal Weierstrass Form...................... 11 1.3 Reduction Modulo Primes...................... 14 1.4 The Frey Curve and Fermat's Last Theorem............ 15 2 Modular Forms 18 2.1 Definitions............................... 18 2.2 Eisenstein Series and the Discriminant............... 21 2.3 The Ring of Modular Forms..................... 25 2.4 Congruence Subgroups........................ 28 3 The Modularity Theorem 36 3.1 Statement of the Theorem...................... 36 3.2 Fermat's Last Theorem....................... 36 References 39 2 Introduction One of the longest standing open problems in mathematics was Fermat's Last Theorem, asserting that the equation an + bn = cn does not have any nontrivial (i.e. with abc 6= 0) integral solutions when n is larger than 2. The proof, which was completed in 1995 by Wiles and Taylor, relied heavily on the Modularity Theorem, relating elliptic curves over Q to modular forms. The Modularity Theorem has many different forms, some of which are stated in an analytic way using Riemann surfaces, while others are stated in a more algebraic way, using for instance L-series or Galois representations. This text will present an elegant, elementary formulation of the theorem, using nothing more than some basic vocabulary of both elliptic curves and modular forms. For elliptic curves E over Q, we will examine the reduction E~ of E modulo any prime p, thus introducing the quantity ~ ap(E) = p + 1 − #E(Fp): We will also give an almost complete description of the conductor NE associated to an elliptic curve E, and compute it for the curve used in the proof of Fermat's Last Theorem. -
One-Dimensional Semirelativistic Hamiltonian with Multiple Dirac Delta Potentials
PHYSICAL REVIEW D 95, 045004 (2017) One-dimensional semirelativistic Hamiltonian with multiple Dirac delta potentials Fatih Erman* Department of Mathematics, İzmir Institute of Technology, Urla 35430, İzmir, Turkey † Manuel Gadella Departamento de Física Teórica, Atómica y Óptica and IMUVA, Universidad de Valladolid, Campus Miguel Delibes, Paseo Belén 7, 47011 Valladolid, Spain ‡ Haydar Uncu Department of Physics, Adnan Menderes University, 09100 Aydın, Turkey (Received 18 August 2016; published 17 February 2017) In this paper, we consider the one-dimensional semirelativistic Schrödinger equation for a particle interacting with N Dirac delta potentials. Using the heat kernel techniques, we establish a resolvent formula in terms of an N × N matrix, called the principal matrix. This matrix essentially includes all the information about the spectrum of the problem. We study the bound state spectrum by working out the eigenvalues of the principal matrix. With the help of the Feynman-Hellmann theorem, we analyze how the bound state energies change with respect to the parameters in the model. We also prove that there are at most N bound states and explicitly derive the bound state wave function. The bound state problem for the two-center case is particularly investigated. We show that the ground state energy is bounded below, and there exists a self- adjoint Hamiltonian associated with the resolvent formula. Moreover, we prove that the ground state is nondegenerate. The scattering problem for N centers is analyzed by exactly solving the semirelativistic Lippmann-Schwinger equation. The reflection and the transmission coefficients are numerically and asymptotically computed for the two-center case. We observe the so-called threshold anomaly for two symmetrically located centers. -
Bound States in the Continuum in One-Dimensional Qubit Arrays
DIPARTIMENTO INTERATENEO DI FISICA "M. MERLIN" Dottorato di ricerca in Fisica - Ciclo XXXII Settore Scientifico Disciplinare FIS/02 Bound states in the continuum in one-dimensional qubit arrays Dottorando: Domenico Pomarico Supervisori: Ch.mo Prof. Saverio Pascazio Dott. Francesco V. Pepe Coordinatore: Ch.mo Prof. Giuseppe Iaselli ESAME FINALE 2020 Contents Introduction1 I Friedrichs-Lee model simulators3 1 The Friedrichs-Lee model5 1.1 Unstable vacua............................6 1.2 Minimal coupling........................... 10 1.2.1 Canonical quantization................... 12 1.3 Dipole Hamiltonian and Rotating waves.............. 15 1.4 Waveguide QED in a nutshell.................... 19 1.4.1 Quasi-1D free field and interaction Hamiltonian..... 20 2 The resolvent formalism 23 2.1 Resolvent operator.......................... 23 2.2 Schrödinger equation......................... 25 2.3 Survival amplitude.......................... 26 2.4 Fermi golden rule........................... 28 2.5 Diagrammatics and Self-energy................... 30 2.6 Projection of the resolvent in a subspace.............. 33 3 Single emitter decay 35 3.1 Selection rules............................. 35 3.1.1 Approximations summary................. 37 3.2 Spontaneous photon emission.................... 39 3.2.1 Analytical continuation................... 42 3.2.2 Weisskopf-Wigner approximation............. 44 3.2.3 Plasmonic eigenstates.................... 46 iii iv Contents II Emitters pair: bound states and their dissociation 49 4 Entangled bound states generation 51 4.1 Resonant bound states in the continuum.............. 52 4.1.1 Entanglement by relaxation................. 55 4.1.2 Energy density........................ 57 4.1.3 Atomic population...................... 57 4.2 Time evolution and bound state stability.............. 59 4.3 Off-resonant bound states...................... 64 4.4 Extension to generic dispersion relations.............. 69 5 Correlated photon emission by two excited atoms in a waveguide 71 5.1 The two-excitation sector......................