Automorphic Forms for Some Even Unimodular Lattices
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Automorphic L-Functions
Proceedings of Symposia in Pure Mathematics Vol. 33 (1979), part 2, pp. 27-61 AUTOMORPHIC L-FUNCTIONS A. BOREL This paper is mainly devoted to the L-functions attached by Langlands [35] to an irreducible admissible automorphic representation re of a reductive group G over a global field k and to local and global problems pertaining to them. In the context of this Institute, it is meant to be complementary to various seminars, in particular to the GL2-seminars, and to stress the general case. We shall therefore start directly with the latter, and refer for background and motivation to other seminars, or to some expository articles on this topic in general [3] or on some aspects of it [7], [14], [15], [23]. The representation re is a tensor product re = @,re, over the places of k, where re, is an irreducible admissible representation of G(k,) [11]. Accordingly the L-func tions associated to re will be Euler products of local factors associated to the 7r:.'s. The definition of those uses the notion of the L-group LG of, or associated to, G. This is the subject matter of Chapter I, whose presentation has been much influ enced by a letter of Deligne to the author. The L-function will then be an Euler product L(s, re, r) assigned to re and to a finite dimensional representation r of LG. (If G = GL"' then the L-group is essentially GLn(C), and we may tacitly take for r the standard representation r n of GLn(C), so that the discussion of GLn can be carried out without any explicit mention of the L-group, as is done in the first six sections of [3].) The local L- ands-factors are defined at all places where G and 1T: are "unramified" in a suitable sense, a condition which excludes at most finitely many places. -
Introduction to L-Functions II: Automorphic L-Functions
Introduction to L-functions II: Automorphic L-functions References: - D. Bump, Automorphic Forms and Repre- sentations. - J. Cogdell, Notes on L-functions for GL(n) - S. Gelbart and F. Shahidi, Analytic Prop- erties of Automorphic L-functions. 1 First lecture: Tate’s thesis, which develop the theory of L- functions for Hecke characters (automorphic forms of GL(1)). These are degree 1 L-functions, and Tate’s thesis gives an elegant proof that they are “nice”. Today: Higher degree L-functions, which are associated to automorphic forms of GL(n) for general n. Goals: (i) Define the L-function L(s, π) associated to an automorphic representation π. (ii) Discuss ways of showing that L(s, π) is “nice”, following the praradigm of Tate’s the- sis. 2 The group G = GL(n) over F F = number field. Some subgroups of G: ∼ (i) Z = Gm = the center of G; (ii) B = Borel subgroup of upper triangular matrices = T · U; (iii) T = maximal torus of of diagonal elements ∼ n = (Gm) ; (iv) U = unipotent radical of B = upper trian- gular unipotent matrices; (v) For each finite v, Kv = GLn(Ov) = maximal compact subgroup. 3 Automorphic Forms on G An automorphic form on G is a function f : G(F )\G(A) −→ C satisfying some smoothness and finiteness con- ditions. The space of such functions is denoted by A(G). The group G(A) acts on A(G) by right trans- lation: (g · f)(h)= f(hg). An irreducible subquotient π of A(G) is an au- tomorphic representation. 4 Cusp Forms Let P = M ·N be any parabolic subgroup of G. -
Genus of Vertex Algebras and Mass Formula
Genus of vertex algebras and mass formula Yuto Moriwaki * Graduate School of Mathematical Science, The University of Tokyo, 3-8-1 Komaba, Meguro-ku, Tokyo 153-8914, Japan Abstract. We introduce the notion of a genus and its mass for vertex algebras. For lattice vertex algebras, their genera are the same as those of lattices, which play an important role in the classification of lattices. We derive a formula relating the mass for vertex algebras to that for lattices, and then give a new characterization of some holomorphic vertex operator algebras. Introduction Vertex operator algebras (VOAs) are algebraic structures that play an important role in two-dimensional conformal field theory. The classification of conformal field theories is an extremely interesting problem, of importance in mathematics, statistical mechanics, and string theory; Mathematically, it is related to the classification of vertex operator algebras, which is a main theme of this work. An important class of vertex operator algebras can be constructed from positive-definite even integral lattices, called lattice vertex algebras [Bo1, LL, FLM]. In this paper, we propose a new method to construct and classify vertex algebras by using a method developed in the study of lattices. A lattice is a finite rank free abelian group equipped with a Z-valued symmetric bilinear form. Two such lattices are equivalent (or in the same genus) if they are isomorphic over the ring of p-adic integers Zp for each prime p and also equivalent over the real number arXiv:2004.01441v2 [math.QA] 5 Mar 2021 field R. Lattices in the same genus are not always isomorphic over Z. -
Automorphic Forms on Os+2,2(R)+ and Generalized Kac
+ Automorphic forms on Os+2,2(R) and generalized Kac-Moody algebras. Proceedings of the International Congress of Mathematicians, Vol. 1, 2 (Z¨urich, 1994), 744–752, Birkh¨auser,Basel, 1995. Richard E. Borcherds * Department of Mathematics, University of California at Berkeley, CA 94720-3840, USA. e-mail: [email protected] We discuss how modular forms and automorphic forms can be written as infinite products, and how some of these infinite products appear in the theory of generalized Kac-Moody algebras. This paper is based on my talk at the ICM, and is an exposition of [B5]. 1. Product formulas for modular forms. We will start off by listing some apparently random and unrelated facts about modular forms, which will begin to make sense in a page or two. A modular form of level 1 and weight k is a holomorphic function f on the upper half plane {τ ∈ C|=(τ) > 0} such that f((aτ + b)/(cτ + d)) = (cτ + d)kf(τ) ab for cd ∈ SL2(Z) that is “holomorphic at the cusps”. Recall that the ring of modular forms of level 1 is P n P n generated by E4(τ) = 1+240 n>0 σ3(n)q of weight 4 and E6(τ) = 1−504 n>0 σ5(n)q of weight 6, where 2πiτ P k 3 2 q = e and σk(n) = d|n d . There is a well known product formula for ∆(τ) = (E4(τ) − E6(τ) )/1728 Y ∆(τ) = q (1 − qn)24 n>0 due to Jacobi. This suggests that we could try to write other modular forms, for example E4 or E6, as infinite products. -
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 Positive Definite Even Unimodular Lattices
Algebraic automorphic forms and Hilbert-Siegel modular forms Tamotsu Ikeda (Kyoto university) Sep. 17, 2018, at Hakuba 1 Positive definite even unimodular lattices Let F be a totally real number field of degree d. Let n > 0 be an integer such that dn is even. Then, by Minkowski-Hasse theorem, there exists a quadratic space (Vn;Q) of rank 4n with the following properties: (1) (V; Q) is unramified at any non-archimedean place. (2) (V; Q) is positive definite ai any archimedean place. Definition 1. An algebraic automorphic form on the orthogonal group OQ is a locally constant function on OQ(F )nOQ(A). Put 1 (x; y) = (Q(x + y) − Q(x) − Q(y)) x; y 2 V: Q 2 Let L be a o-lattie in V (F ). The dual lattice L∗ is defined by ∗ L = fx 2 Vn(F ) j (x; L)Q ⊂ og: Then L is an integral lattice if and only if L ⊂ L∗. An integral lattice L is called an even lattice if Q(x) ⊂ 2o 8x 2 L: Moreover, an integral lattice L is unimodular if L = L∗. By the assumption (1) and (2), there exists a positive definite even unimodular latice L0 in V (F ). Two integral lattices L1 and L2 are equivalent if there exists an element g 2 OQ(F ) such that g · L1 = L2. Two integral lattices L1 and L2 are in the same genus if there 1 exists an element gv 2 OQ(Fv) such that g · L1;v = L2;v for any finite place v. The set of positive definite even unimodular lattices in V (F ) form a genus. -
Lattice Theory, K3 Surfaces, and the Torelli Theorem
UMass, Reading Seminar in Algebraic Geometry, Lattice theory, K3 surfaces, and the Torelli theorem Luca Schaffler October 4, 2019 1 What is a lattice? Definition 1.1. A lattice is a pair (L; ·), where L is a finitely generated free abelian group and ·: L × L ! Z such that (v; w) 7! v · w is a symmetric bilinear form. • L is even if v2 := v · v is an even number for all v 2 L. • The Gram matrix of L with respect to a basis fe1; : : : ; eng for L is the matrix of intersection (ei · ej)1≤i;j≤n. • The rank of L is defined to be the rank of one of its Gram matrices. • A lattice L is unimodular if the determinant of one of its Gram matrices is ±1. Equivalently, L of maximal rank is unimodular provided the discriminant group ∗ ∗ L =L is trivial (we let L = HomZ(L; Z)). • We can define the signature of L as the signature of one of its Gram matrices. By saying signature (a; b), we mean that a (resp. b) is the number of positive (resp. negative) eigenvalues. If L has signature (a; b), then we say that L is indefinite provided a; b > 0. 2 Example 1.2. U = (Z ; ·) with (v1; v2) · (w1; w2) = v1w2 + v2w1 is called the hyperbolic plane. Check that this is even, unimodular, and of signature (1; 1). 1 8 Example 1.3. E8 = (Z ;B), where 0 −2 1 0 0 0 0 0 0 1 B 1 −2 1 0 0 0 0 0 C B C B 0 1 −2 1 0 0 0 0 C B C B 0 0 1 −2 1 0 0 0 C B = B C : B 0 0 0 1 −2 1 0 1 C B C B 0 0 0 0 1 −2 1 0 C B C @ 0 0 0 0 0 1 −2 0 A 0 0 0 0 1 0 0 −2 This matrix can be reconstructed from the E8 Dynkin diagram. -
Computing with Algebraic Automorphic Forms
Computing with algebraic automorphic forms David Loeffler Abstract These are the notes of a five-lecture course presented at the Computations with modular forms summer school, aimed at graduate students in number theory and related areas. Sections 1–4 give a sketch of the theory of reductive algebraic groups over Q, and of Gross’s purely algebraic definition of automorphic forms in the special case when G(R) is compact. Sections 5–9 describe how these automor- phic forms can be explicitly computed, concentrating on the case of definite unitary groups; and sections 10 and 11 describe how to relate the results of these computa- tions to Galois representations, and present some examples where the corresponding Galois representations can be identified, giving illustrations of various instances of Langlands’ functoriality conjectures. 1 A user’s guide to reductive groups Let F be a field. An algebraic group over F is a group object in the category of alge- braic varieties over F. More concretely, it is an algebraic variety G over F together with: • a “multiplication” map G × G ! G, • an “inversion” map G ! G, • an “identity”, a distinguished point of G(F). These are required to satisfy the obvious analogues of the usual group axioms. Then G(A) is a group, for any F-algebra A. It’s clear that we can define a morphism of algebraic groups over F in an obvious way, giving us a category of algebraic groups over F. Some important examples of algebraic groups include: Mathematics Institute, University of Warwick, Coventry CV4 7AL, UK, e-mail: d.a. -
Arxiv:2001.07094V3 [Math.NT] 10 May 2021 Aeo Nirdcbeplnma)Alclgoa Principl a Local-Global Conditions, a Local Polynomial) I Are Irreducible Mcmullen 20]
ISOMETRIES OF LATTICES AND HASSE PRINCIPLES EVA BAYER-FLUCKIGER Abstract. We give necessary and sufficient conditions for an integral polynomial without linear factors to be the characteristic polynomial of an isometry of some even, unimodular lattice of given signature. This gives rise to Hasse principle questions, which we answer in a more general setting. As an application, we prove a Hasse principle for signatures of knots. 0. Introduction In [GM 02], Gross and McMullen give necessary conditions for a monic, irreducible polynomial to be the characteristic polynomial of an isometry of some even, unimodular lattice of prescribed signature. They speculate that these conditions may be sufficient; this is proved in [BT 20]. It turns out that the conditions of Gross and McMullen are local conditions, and that (in the case of an irreducible polynomial) a local-global principle holds. More generally, if F Z[X] is a monic polynomial without linear factors, the conditions of Gross∈ and McMullen are still necessary. Moreover, they are also sufficient everywhere locally (see Theorem 25.6). However, when F is reducible, the local-global principle no longer holds in general, as shown by the following example Example. Let F be the polynomial (X6 + X5 + X4 + X3 + X2 + X + 1)2(X6 X5 + X4 X3 + X2 X + 1)2, arXiv:2001.07094v3 [math.NT] 10 May 2021 − − − and let L be an even, unimodular, positive definite lattice of rank 24. The lattice L has an isometry with characteristic polynomial F everywhere locally, but not globally (see Example 25.17). In particular, the Leech lattice has no isometry with characteristic polynomial F , in spite of having such an isometry everywhere locally. -
Arxiv:1203.1428V2 [Math.NT]
SOME APPLICATIONS OF NUMBER THEORY TO 3-MANIFOLD THEORY MEHMET HALUK S¸ENGUN¨ Contents 1. Introduction 1 2. Quaternion Algebras 2 3. Hyperbolic Spaces 3 3.1. Hyperbolic 2-space 4 3.2. Hyperbolic 3-space 4 4. Arithmetic Lattices 5 5. Automorphic Forms 6 5.1. Forms on 6 H2 5.2. Forms on 3 7 Hs r 5.3. Forms on 3 2 9 5.4. Jacquet-LanglandsH × H Correspondence 10 6. HeckeOperatorsontheCohomology 10 7. Cohomology and Automorphic Forms 11 7.1. Jacquet-Langlands Revisited: The Mystery 13 8. Volumes of Arithmetic Hyperbolic 3-Manifolds 13 9. Betti Numbers of Arithmetic Hyperbolic 3-Manifolds 15 9.1. Bianchi groups 15 9.2. General Results 16 10. Rational Homology 3-Spheres 17 arXiv:1203.1428v2 [math.NT] 16 Oct 2013 11. Fibrations of Arithmetic Hyperbolic 3-Manifolds 18 References 20 1. Introduction These are the extended notes of a talk I gave at the Geometric Topology Seminar of the Max Planck Institute for Mathematics in Bonn on January 30th, 2012. My goal was to familiarize the topologists with the basics of arithmetic hyperbolic 3- manifolds and sketch some interesting results in the theory of 3-manifolds (such as Labesse-Schwermer [29], Calegari-Dunfield [8], Dunfield-Ramakrishnan [12]) that are 1 2 MEHMET HALUK S¸ENGUN¨ obtained by exploiting the connections with number theory and automorphic forms. The overall intention was to stimulate interaction between the number theorists and the topologists present at the Institute. These notes are merely expository. I assumed that the audience had only a min- imal background in number theory and I tried to give detailed citations referring the reader to sources. -
Notes on 4-Manifolds
ALGEBRAIC SURFACES AND FOUR-MANIFOLDS PHILIP ENGEL Contents 1. Structures on manifolds 1 2. Sheaves, bundles, and connections 4 3. Cohomology 8 4. Characteristic classes 12 5. The Riemann-Roch theorem and its generalizations 16 6. The Hodge theorems 19 7. Introduction to algebraic surfaces 25 8. Blow-ups and blow-downs 30 9. Spin and Spinc groups 33 10. Spin bundles and Dirac operators 38 11. Rokhlin's theorem 42 12. Freedman's theorems 45 13. Classification of unimodular lattices 49 4 14. An exotic R 49 15. The Seiberg-Witten equations 49 1. Structures on manifolds Definition 1.1. A topological or C0-manifold of dimension n is a Hausdorff n topological space X, which admits local charts to φU : U ! R . It follows that the transition functions −1 tUV := φV ◦ φU : φU (U \ V ) ! φV (U \ V ) are homeomorphisms. Definition 1.2. By requiring tUV to respect extra geometric structures on n R , we produce many other classes of manifolds. In increasing order of restrictiveness, we say X is additionally a (1) PL manifold if tUV are piecewise-linear. k 1 k (2) C - or C -manifold if tUV 2 C are k-differentiable or smooth. (3) real-analytic manifold if tUV are real-analytic. (4) complex-analytic manifold if tUV is holomorphic: i.e. has a complex- n n=2 linear differential with respect the identification R = C . 1 2 PHILIP ENGEL (5) projective variety if there is a homeomorphism X ! V (f1; : : : ; fm) ⊂ N CP to a smooth vanishing locus of homogenous polynomials. N N+1 ∗ CP := (C n f0g)= ∼ with x ∼ λx for all λ 2 C : There is a natural notion of isomorphism for each class of manifold/variety, by declaring that a homeomorphism f : X ! Y defines an isomorphism if it preserves the given structure. -
L-Functions and Automorphic Representations*
L-Functions and Automorphic Representations* R. P. Langlands Introduction. There are at least three different problems with which one is confronted in the study of L-functions: the analytic continuation and functional equation; the location of the zeroes; and in some cases, the determination of the values at special points. The first may be the easiest. It is certainly the only one with which I have been closely involved. There are two kinds of L-functions, and they will be described below: motivic L-functions which generalize the Artin L-functions and are defined purely arithmetically, and automorphic L-functions, defined by data which are largely transcendental. Within the automorphic L-functions a special class can be singled out, the class of standard L-functions, which generalize the Hecke L-functions and for which the analytic continuation and functional equation can be proved directly. For the other L-functions the analytic continuation is not so easily effected. However all evidence indicates that there are fewer L-functions than the definitions suggest, and that every L-function, motivic or automorphic, is equal to a standard L-function. Such equalities are often deep, and are called reciprocity laws, for historical reasons. Once a reciprocity law can be proved for an L-function, analytic continuation follows, and so, for those who believe in the validity of the reciprocity laws, they and not analytic continuation are the focus of attention, but very few such laws have been established. The automorphic L-functions are defined representation-theoretically, and it should be no surprise that harmonic analysis can be applied to some effect in the study of reciprocity laws.