THE CHARACTER GROUP of Q 1. Introduction the Characters of a Finite Abelian Group G Are the Homomorphisms from G to the Unit
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Notes on the Finite Fourier Transform
Notes on the Finite Fourier Transform Peter Woit Department of Mathematics, Columbia University [email protected] April 28, 2020 1 Introduction In this final section of the course we'll discuss a topic which is in some sense much simpler than the cases of Fourier series for functions on S1 and the Fourier transform for functions on R, since it will involve functions on a finite set, and thus just algebra and no need for the complexities of analysis. This topic has important applications in the approximate computation of Fourier series (which we won't cover), and in number theory (which we'll say a little bit about). 2 The group Z(N) What we'll be doing is simplifying the topic of Fourier series by replacing the multiplicative group S1 = fz 2 C : jzj = 1g by the finite subgroup Z(N) = fz 2 C : zN = 1g If we write z = reiθ, then zN = 1 =) rN eiθN = 1 =) r = 1; θN = k2π (k 2 Z) k =) θ = 2π k = 0; 1; 2; ··· ;N − 1 N mod 2π The group Z(N) is thus explicitly given by the set i 2π i2 2π i(N−1) 2π Z(N) = f1; e N ; e N ; ··· ; e N g Geometrically, these are the points on the unit circle one gets by starting at 1 2π and dividing it into N sectors with equal angles N . (Draw a picture, N = 6) The set Z(N) is a group, with 1 identity element 1 (k = 0) inverse 2πi k −1 −2πi k 2πi (N−k) (e N ) = e N = e N multiplication law ik 2π il 2π i(k+l) 2π e N e N = e N One can equally well write this group as the additive group (Z=NZ; +) of inte- gers mod N, with isomorphism Z(N) $ Z=NZ ik 2π e N $ [k]N 1 $ [0]N −ik 2π e N $ −[k]N = [−k]N = [N − k]N 3 Fourier analysis on Z(N) An abstract point of view on the theory of Fourier series is that it is based on exploiting the existence of a particular othonormal basis of functions on the group S1 that are eigenfunctions of the linear transformations given by rotations. -
An Introduction to the Trace Formula
Clay Mathematics Proceedings Volume 4, 2005 An Introduction to the Trace Formula James Arthur Contents Foreword 3 Part I. The Unrefined Trace Formula 7 1. The Selberg trace formula for compact quotient 7 2. Algebraic groups and adeles 11 3. Simple examples 15 4. Noncompact quotient and parabolic subgroups 20 5. Roots and weights 24 6. Statement and discussion of a theorem 29 7. Eisenstein series 31 8. On the proof of the theorem 37 9. Qualitative behaviour of J T (f) 46 10. The coarse geometric expansion 53 11. Weighted orbital integrals 56 12. Cuspidal automorphic data 64 13. A truncation operator 68 14. The coarse spectral expansion 74 15. Weighted characters 81 Part II. Refinements and Applications 89 16. The first problem of refinement 89 17. (G, M)-families 93 18. Localbehaviourofweightedorbitalintegrals 102 19. The fine geometric expansion 109 20. Application of a Paley-Wiener theorem 116 21. The fine spectral expansion 126 22. The problem of invariance 139 23. The invariant trace formula 145 24. AclosedformulaforthetracesofHeckeoperators 157 25. Inner forms of GL(n) 166 Supported in part by NSERC Discovery Grant A3483. c 2005 Clay Mathematics Institute 1 2 JAMES ARTHUR 26. Functoriality and base change for GL(n) 180 27. The problem of stability 192 28. Localspectraltransferandnormalization 204 29. The stable trace formula 216 30. Representationsofclassicalgroups 234 Afterword: beyond endoscopy 251 References 258 Foreword These notes are an attempt to provide an entry into a subject that has not been very accessible. The problems of exposition are twofold. It is important to present motivation and background for the kind of problems that the trace formula is designed to solve. -
Class Numbers of CM Algebraic Tori, CM Abelian Varieties and Components of Unitary Shimura Varieties
CLASS NUMBERS OF CM ALGEBRAIC TORI, CM ABELIAN VARIETIES AND COMPONENTS OF UNITARY SHIMURA VARIETIES JIA-WEI GUO, NAI-HENG SHEU, AND CHIA-FU YU Abstract. We give a formula for the class number of an arbitrary CM algebraic torus over Q. This is proved based on results of Ono and Shyr. As applications, we give formulas for numbers of polarized CM abelian varieties, of connected components of unitary Shimura varieties and of certain polarized abelian varieties over finite fields. We also give a second proof of our main result. 1. Introduction An algebraic torus T over a number field k is a connected linear algebraic group over k such d that T k k¯ isomorphic to (Gm) k k¯ over the algebraic closure k¯ of k for some integer d 1. The class⊗ number, h(T ), of T is by⊗ definition, the cardinality of T (k) T (A )/U , where A≥ \ k,f T k,f is the finite adele ring of k and UT is the maximal open compact subgroup of T (Ak,f ). Asa natural generalization for the class number of a number field, Takashi Ono [18, 19] studied the class numbers of algebraic tori. Let K/k be a finite extension and let RK/k denote the Weil restriction of scalars form K to k, then we have the following exact sequence of tori defined over k 1 R(1) (G ) R (G ) G 1, −→ K/k m,K −→ K/k m,K −→ m,k −→ where R(1) (G ) is the kernel of the norm map N : R (G ) G . -
Some Applications of the Fourier Transform in Algebraic Coding Theory
Contemporary Mathematics Some Applications of the Fourier Transform in Algebraic Coding Theory Jay A. Wood In memory of Shoshichi Kobayashi, 1932{2012 Abstract. This expository article describes two uses of the Fourier transform that are of interest in algebraic coding theory: the MacWilliams identities and the decomposition of a semi-simple group algebra of a finite group into a direct sum of matrix rings. Introduction Because much of the material covered in my lectures at the ASReCoM CIMPA research school has already appeared in print ([18], an earlier research school spon- sored by CIMPA), the organizers requested that I discuss more broadly the role of the Fourier transform in coding theory. I have chosen to discuss two aspects of the Fourier transform of particular interest to me: the well-known use of the complex Fourier transform in proving the MacWilliams identities, and the less-well-known use of the Fourier transform as a way of understanding the decomposition of a semi-simple group algebra into a sum of matrix rings. In the latter, the Fourier transform essentially acts as a change of basis matrix. I make no claims of originality; the content is discussed in various forms in such sources as [1,4, 15, 16 ], to whose authors I express my thanks. The material is organized into three parts: the theory over the complex numbers needed to prove the MacWilliams identities, the theory over general fields relevant to decomposing group algebras, and examples over finite fields. Each part is further divided into numbered sections. Personal Remark. This article is dedicated to the memory of Professor Shoshichi Kobayashi, my doctoral advisor, who died 29 August 2012. -
Chapter 2 C -Algebras
Chapter 2 C∗-algebras This chapter is mainly based on the first chapters of the book [Mur90]. Material bor- rowed from other references will be specified. 2.1 Banach algebras Definition 2.1.1. A Banach algebra C is a complex vector space endowed with an associative multiplication and with a norm k · k which satisfy for any A; B; C 2 C and α 2 C (i) (αA)B = α(AB) = A(αB), (ii) A(B + C) = AB + AC and (A + B)C = AC + BC, (iii) kABk ≤ kAkkBk (submultiplicativity) (iv) C is complete with the norm k · k. One says that C is abelian or commutative if AB = BA for all A; B 2 C . One also says that C is unital if 1 2 C , i.e. if there exists an element 1 2 C with k1k = 1 such that 1B = B = B1 for all B 2 C . A subalgebra J of C is a vector subspace which is stable for the multiplication. If J is norm closed, it is a Banach algebra in itself. Examples 2.1.2. (i) C, Mn(C), B(H), K (H) are Banach algebras, where Mn(C) denotes the set of n × n-matrices over C. All except K (H) are unital, and K (H) is unital if H is finite dimensional. (ii) If Ω is a locally compact topological space, C0(Ω) and Cb(Ω) are abelian Banach algebras, where Cb(Ω) denotes the set of all bounded and continuous complex func- tions from Ω to C, and C0(Ω) denotes the subset of Cb(Ω) of functions f which vanish at infinity, i.e. -
Adams Operations and Symmetries of Representation Categories Arxiv
Adams operations and symmetries of representation categories Ehud Meir and Markus Szymik May 2019 Abstract: Adams operations are the natural transformations of the representation ring func- tor on the category of finite groups, and they are one way to describe the usual λ–ring structure on these rings. From the representation-theoretical point of view, they codify some of the symmetric monoidal structure of the representation category. We show that the monoidal structure on the category alone, regardless of the particular symmetry, deter- mines all the odd Adams operations. On the other hand, we give examples to show that monoidal equivalences do not have to preserve the second Adams operations and to show that monoidal equivalences that preserve the second Adams operations do not have to be symmetric. Along the way, we classify all possible symmetries and all monoidal auto- equivalences of representation categories of finite groups. MSC: 18D10, 19A22, 20C15 Keywords: Representation rings, Adams operations, λ–rings, symmetric monoidal cate- gories 1 Introduction Every finite group G can be reconstructed from the category Rep(G) of its finite-dimensional representations if one considers this category as a symmetric monoidal category. This follows from more general results of Deligne [DM82, Prop. 2.8], [Del90]. If one considers the repre- sentation category Rep(G) as a monoidal category alone, without its canonical symmetry, then it does not determine the group G. See Davydov [Dav01] and Etingof–Gelaki [EG01] for such arXiv:1704.03389v3 [math.RT] 3 Jun 2019 isocategorical groups. Examples go back to Fischer [Fis88]. The representation ring R(G) of a finite group G is a λ–ring. -
Notes on the Chern-Character Maakestad H* Department of Mathematics, NTNU, Trondheim, Norway
Theory an ie d L A p d p Maakestad, J Generalized Lie Theory Appl 2017, 11:1 e l z i i c l a a t Journal of Generalized Lie r DOI: 10.4172/1736-4337.1000253 i o e n n s e G ISSN: 1736-4337 Theory and Applications Research Article Open Access Notes on the Chern-Character Maakestad H* Department of Mathematics, NTNU, Trondheim, Norway Abstract Notes for some talks given at the seminar on characteristic classes at NTNU in autumn 2006. In the note a proof of the existence of a Chern-character from complex K-theory to any cohomology Lie theory with values in graded Q-algebras equipped with a theory of characteristic classes is given. It respects the Adams and Steenrod operations. Keywords: Chern-character; Chern-classes; Euler classes; Singular H* : Top→−Q algebras cohomology; De Rham-cohomology; Complex K-theory; Adams operations; Steenrod operations from the category of topological spaces to the category of graded commutative Q-algebras with respect to continuous maps of topological Introduction spaces. We say the theory satisfy the projective bundle property if the The aim of this note is to give an axiomatic and elementary following axioms are satisfied: For any rankn complex continuous treatment of Chern-characters of vectorbundles with values in a vectorbundle E over a compact space B There is an Euler class. class of cohomology-theories arising in topology and algebra. Given ∈ 2 uE H (P(E)) (1) a theory of Chern-classes for complex vectorbundles with values in → singular cohomology one gets in a natural way a Chern-character from Where π:P(E) B is the projective bundle associated to E. -
GROUP REPRESENTATIONS and CHARACTER THEORY Contents 1
GROUP REPRESENTATIONS AND CHARACTER THEORY DAVID KANG Abstract. In this paper, we provide an introduction to the representation theory of finite groups. We begin by defining representations, G-linear maps, and other essential concepts before moving quickly towards initial results on irreducibility and Schur's Lemma. We then consider characters, class func- tions, and show that the character of a representation uniquely determines it up to isomorphism. Orthogonality relations are introduced shortly afterwards. Finally, we construct the character tables for a few familiar groups. Contents 1. Introduction 1 2. Preliminaries 1 3. Group Representations 2 4. Maschke's Theorem and Complete Reducibility 4 5. Schur's Lemma and Decomposition 5 6. Character Theory 7 7. Character Tables for S4 and Z3 12 Acknowledgments 13 References 14 1. Introduction The primary motivation for the study of group representations is to simplify the study of groups. Representation theory offers a powerful approach to the study of groups because it reduces many group theoretic problems to basic linear algebra calculations. To this end, we assume that the reader is already quite familiar with linear algebra and has had some exposure to group theory. With this said, we begin with a preliminary section on group theory. 2. Preliminaries Definition 2.1. A group is a set G with a binary operation satisfying (1) 8 g; h; i 2 G; (gh)i = g(hi)(associativity) (2) 9 1 2 G such that 1g = g1 = g; 8g 2 G (identity) (3) 8 g 2 G; 9 g−1 such that gg−1 = g−1g = 1 (inverses) Definition 2.2. -
On the Characters of ¿-Solvable Groups
ON THE CHARACTERSOF ¿-SOLVABLEGROUPS BY P. FONGO) Introduction. In the theory of group characters, modular representation theory has explained some of the regularities in the behavior of the irreducible characters of a finite group; not unexpectedly, the theory in turn poses new problems of its own. These problems, which are asked by Brauer in [4], seem to lie deep. In this paper we look at the situation for solvable groups. We can answer some of the questions in [4] for these groups, and in doing so, obtain new properties for their characters. Finite solvable groups have recently been the object of much investigation by group theorists, especially with the end of relating the structure of such groups to their Sylow /»-subgroups. Our work does not lie quite in this direction, although we have one result tying up arith- metic properties of the characters to the structure of certain /»-subgroups. Since the prime number p is always fixed, we can actually work in the more general class of /»-solvable groups, and shall do so. Let © be a finite group of order g = pago, where p is a fixed prime number, a is an integer ^0, and ip, go) = 1. In the modular theory, the main results of which are in [2; 3; 5; 9], the characters of the irreducible complex-valued representations of ©, or as we shall say, the irreducible characters of ®, are partitioned into disjoint sets, these sets being the so-called blocks of © for the prime p. Each block B has attached to it a /»-subgroup 35 of © determined up to conjugates in @, the defect group of the block B. -
Introduction to Fourier Methods
Appendix L Introduction to Fourier Methods L.1. The Circle Group and its Characters We will denote by S the unit circle in the complex plane: S = {(x, y) ∈ R2 | x2 + y2 =1} = {(cos θ, sin θ) ∈ R2 | 0 ≤ θ< 2π} = {z ∈ C | |z| =1} = {eiθ | 0 ≤ θ< 2π}. We note that S is a group under multiplication, i.e., if z1 and z2 are in S then so is z1z2. and if z = x + yi ∈ S thenz ¯ = x − yi also is in S with zz¯ =zz ¯ =1, soz ¯ = z−1 = 1/z. In particular then, given any function f defined on S, and any z0 in S, we can define another function fz0 on S (called f translated by z0), by fz0 (z) = f(zz0). The set of piecewise continuous complex-valued functions on S will be denoted by H(S). The map κ : t 7→ eit is a continuous group homomorphism of the additive group of real numbers, R, onto S, and so it induces a homeomorphism and group isomorphism [t] 7→ eit of the compact quotient group K := R/2πZ with S. Here [t] ∈ K of course denotes the coset of the real number t, i.e., the set of all real numbers s that differ from t by an integer multiple of 2π, and we note that we can always choose a unique representative of [t] in [0, 2π). K is an additive model for S, and this makes it more convenient for some purposes. A function on K is clearly the “same thing” as a 2π-periodic function on R. -
L-Functions and Non-Abelian Class Field Theory, from Artin to Langlands
L-functions and non-abelian class field theory, from Artin to Langlands James W. Cogdell∗ Introduction Emil Artin spent the first 15 years of his career in Hamburg. Andr´eWeil charac- terized this period of Artin's career as a \love affair with the zeta function" [77]. Claude Chevalley, in his obituary of Artin [14], pointed out that Artin's use of zeta functions was to discover exact algebraic facts as opposed to estimates or approxi- mate evaluations. In particular, it seems clear to me that during this period Artin was quite interested in using the Artin L-functions as a tool for finding a non- abelian class field theory, expressed as the desire to extend results from relative abelian extensions to general extensions of number fields. Artin introduced his L-functions attached to characters of the Galois group in 1923 in hopes of developing a non-abelian class field theory. Instead, through them he was led to formulate and prove the Artin Reciprocity Law - the crowning achievement of abelian class field theory. But Artin never lost interest in pursuing a non-abelian class field theory. At the Princeton University Bicentennial Conference on the Problems of Mathematics held in 1946 \Artin stated that `My own belief is that we know it already, though no one will believe me { that whatever can be said about non-Abelian class field theory follows from what we know now, since it depends on the behavior of the broad field over the intermediate fields { and there are sufficiently many Abelian cases.' The critical thing is learning how to pass from a prime in an intermediate field to a prime in a large field. -
Beyond Endoscopy for the Relative Trace Formula II: Global Theory
BEYOND ENDOSCOPY FOR THE RELATIVE TRACE FORMULA II: GLOBAL THEORY YIANNIS SAKELLARIDIS Abstract. For the group G = PGL2 we perform a comparison between two relative trace formulas: on one hand, the relative trace formula of Jacquet for the quotient T \G/T , where T is a non-trivial torus, and on the other the Kuznetsov trace formula (involving Whittaker periods), applied to non-standard test functions. This gives a new proof of the celebrated result of Waldspurger on toric periods, and suggests a new way of comparing trace formulas, with some analogies to Langlands’ “Beyond Endoscopy” program. Contents 1. Introduction. 1 Part 1. Poisson summation 18 2. Generalities and the baby case. 18 3. Direct proof in the baby case 31 4. Poisson summation for the relative trace formula 41 Part 2. Spectral analysis. 54 5. Main theorems of spectral decomposition 54 6. Completion of proofs 67 7. The formula of Waldspurger 85 Appendix A. Families of locally multiplicative functions 96 Appendix B. F-representations 104 arXiv:1402.3524v3 [math.NT] 9 Mar 2017 References 107 1. Introduction. 1.1. The result of Waldspurger. The celebrated result of Waldspurger [Wal85], relating periods of cusp forms on GL2 over a nonsplit torus (against a character of the torus, but here we will restrict ourselves to the trivial character) with the central special value of the corresponding quadratic base 2010 Mathematics Subject Classification. 11F70. Key words and phrases. relative trace formula, beyond endoscopy, periods, L-functions, Waldspurger’s formula. 1 2 YIANNIS SAKELLARIDIS change L-function, was reproven by Jacquet [Jac86] using the relative trace formula.