Norm computation and analytic continuation of holomorphic discrete series

Size: px
Start display at page:

Download "Norm computation and analytic continuation of holomorphic discrete series"

Transcription

1 Norm computation and analytic continuation of holomorphic discrete series Ryosuke Nakahama Graduate School of Mathematical Sciences, The University of Tokyo Introduction: Holomorphic discrete series of SU, Let : {w C : w < } Then G : SU, universal covering group acts on O by a b aw + b τ λ fw : cw + d λ f c d cw + d where λ C This action preserves the sesquilinear form f, h λ : λ fwhw w λ dw, π that is, τ λ gf, τ λgh λ f, h λ holds for any g G When Re λ >, this form converges for any polynomial f, h, and therefore τ λ defines a unitary representation of G when λ > This is called the holomorphic discrete series representation On the other hand, if Re λ, this integral diverges for any non-zero function f However, when Re λ > and f m a mw m, we can compute as f λ m m! λ m a m where λ m : λλ + λ + m, because r s λ π λ π w m w n w λ dw π λ δ mn s m s λ ds r m+n e iθm n r λ rdθdr δ mn λ Bm +, λ δ mn Γm + Γλ Γm + λ δ mn m! λ m This expression is available even when Re λ, and positive definite for λ > Therefore τ λ defines a unitary representation of G when λ > This example shows that if once the norm is explicitly computed, we can treat the analytic continuation of the holomorphic discrete series representation

2 Holomorphic discrete series of general Hermitian Lie group Let G be a Hermitian simple Lie group, that is, its maximal compact subgroup K has a non-discrete center We assume that G has a complexification G C We denote their Lie algebras by g, k, g C Then we can take z zk the center of k such that the eigenvalues of adz are +,, We denote the corresponding eigenspace decomposition by g C p + k C p We denote n dim C p +, r rank R G Then there exists a domain p + such that the following diagram commutes G/K G C /K C P p + exp Let τ, V be a holomorphic representation of K C, and let χ be the character of K C such that χexp t z e rt Then we have the following isomorphism Γ O G/K, G K V χ λ O, V where Γ O G/K, G K V χ λ is the space of holomorphic sections, and O, V is the space of V -valued holomorphic functions on G acts on O, V by the form τ λ gfw χµg, w λ τµg, w fg w for g G, w, where µ : G K C is a continuous map satisfying µgh, w µg, hwµh, w µk, w k g, h G, w, k K, w This action preserves the following norm: f λ,τ : c λ τbw π n fw, fw τ χbwλ p dw f O, V where p is an integer determined from g, and B : K C is a continuous map satisfying µg, wbwµg, w Bgw g G, w where is the inverse of the Cartan involution of KC This norm can be zero for any holomorphic function f, but if λ is sufficiently large, this does not occur Ir Example Let J, J I r Ir, and set I r G { g GLr, C : gj t g J, gj J ḡ } Spr, R, Then we have {w Symr, C : I ww is positive definite},

3 and G acts on O, V by A B τ λ fw : detcw + λ τ t Cw + f Aw + BCw + C This preserves f λ,τ : c λ π n τi ww fw, fw τ deti ww λ r+ dw We define another norm on Pp +, V f F,τ : π n fw τ e w dw f Pp +, V, p + where w is a suitable K-invariant norm on p + Let W Pp +, V be an irreducible subspace under the K-action ˆτkf w : τkfk w k K C, f Pp +, V, w p + Then since λ,τ and F,τ are both K-invariant, the ratio of two norms are constant on W The goal of this talk is to calculate this ratio under some conditions Remark Known results For several settings, this is already done by B Ørsted 98 for G SUr, r, scalar type J Faraut and A Korányi 99 for G any Hermitian Lie group, scalar type B Ørsted and G Zhang 994, 995 for G Spr, R, V C r, G SUr, r, V C C r, G SO 4r, V C r S Hwang, Y Liu and G Zhang 4 for G SUn,, V p C n C, q C n C 3 Main result We assume that G is of tube type Then there exists an e p + such that [e, ϑe] zk, [e, [ϑe, e]] e, where ϑ is the Cartan involution of g C Using this, we define c G : Inte πi 4 e ϑe G, L : c G K C, K L : L K We take a maximal abelian subalgebra h k We write the root system by g C, h C p + k C p h C in the usual fashion We define the positive system + g C, h C such that + p + Then there exist roots {γ,, γ r } p + such that, for a irreducible unitary representation V µ of K with lowest weight µ h C, V µ has a K L -invariant vector K L -spherical if and only if µ is of the form µ m γ + + m r γ r, m j Z, m m r 3

4 Let a l : h l Then a l is spanned by {γ al,, γ r al } For a representation V of K C, we denote by V the complex conjugate representation of V with respect to the real form L For s s,, s r C r and m m,, m r Z r, we write s m : s j d j j where d is the integer satisfying n r + d rr Now we state the main theorem Theorem 3 Let τ, V be an irreducible finite dimensional complex representation of K C with restricted lowest weight k γ k r al γ r We assume τ KL still remains irreducible Let W Pp +, V be a K-irreducible subspace If all the K L -spherical irreducible subspaces in W V have the same lowest weight n γ n r γ r, then for any f W, f λ,τ f F,τ holds under the suitable choice of c λ λ k λ n m j λ + k n k Example 3 Let G Spr, R Then we have K Ur, L GLr, R, K L Or, and a l h We identify h R r such that m,, m r R r is a lowest weight of a representation of K if and only if m m r, m j Z Then we have γ j e j We set V : V,,,,, k C r Then this remains irreducible when restrected }{{} k to K L, and V V holds We have Pp +, V V m V,,,,, }{{} m m r k m j Z m m r m j Z i < <i k V m+ei i k where e i i k is the vector whose i j -component is and otherwise, and V ν {} if ν is not dominant V m+ei i k V is decomposed as V m+ei i k V j < <j k V m+ei i k +e j j k, but since V ν is K L -spherical if and only if ν Z r, the only K L -spherical subspace in V m+ei i k V is V m+ei i k Therefore, for f V m+ei i k, we have Thus the norm f λ,τ ek f F,τ ek λ e k λ m+ei i k f λ,τ ek m m r m j Z i < <i k λ + e k m+ei i k e k λ ek λ m+ei i k f m+ei i k F,τ ek 4

5 is continued meromorphically, and for k r it becomes a unitary representation if and only if { k λ, k +,, r } r,, and when λ l l k,, r the corresponding representation space is H λ, V m m l i < <i k l m l+ m r m j Z Remark 33 Our result can be applied for G Spr, R, V k C r G SO 4r, V S k C r, S k C r V m+ei i i k G SUr, r, V W C, C W W : any irreducible representation of Ur G Spin, s, V C V k,,k,±k k Z G Spin, s +, V C V,, spin representation 4 Proof for G Spr, R case In this section we prove the theorem for G Spr, R case In this case we have K Ur, L GLr, R, K L Or, p + Symr, C, {w Symr, C : I ww is positive definite} Let τ, V be an irreducible unitary representation of K, and let W Pp +, V be a K-irreducible subspace under the action ˆτkf w : τkfk w t k k K C, f Pp +, V, w p + For f W we compute the ratio c λ f τi ww λ,τ π f n fw, fw τ deti ww λ r+ dw F,τ π n fw τ e trww dw p + under the condition V has the lowest weight k k,, k r V KL V Or still remains irreducible All the K L Or-spherical irreducible subspaces in W V W V have the same lowest weight n n,, n r 5

6 We set f λ,τ / f F,τ : R W,λ, and compute this ratio As a preparation, we set b t b b B : GLr, R : b jj >, j,, r, b r b r b rr : {x Symr, R : positive definite} Then we have a bijection t B, b b t b Also, for x and s s,, s r C r, we set s x : x s s x s s3 r x s r s r r x s r where k x : detx ij i,j k For example, for b b ij t B we have s b t b b s bs bs r rr Also we set Γ s : e trx s x detx r+ dy This integral converges if Re s j > j, and we have Γ s n+r e trbtb s b t b detb t b r+ b r b r b rr db n+r n+r t B t B j π n r and therefore we have Γ s + m Γ s e i j b ijb s bs bsr rr b b b rr r+ b r b r j j e b jjb s j j jj db jj Γ s j j, i j Γ s j + m j j Γ s j j e b ijdb ij j b rr db s j j s m m j Now we start the proof Let K W z, w Pp + p +, EndV be the reproducing kernel of W with respect to F,τ Then the ratio R W,λ is computed as c λ Tr V τi ww K W w, w deti ww λ r+ dw R W,λ Tr V K W w, we trww dw p + To proceed the computation, we prove the following lemma Lemma 4 For any integrable function f on p +, we have fwdw c fkx t kdkdx p + K where c is a constant 6

7 Proof By the integral formulas fwdw c p + K fxdx c K L fka t k i<j fk t t k i<j a i a j a j da da r dk, j t i t j dt dt r dk where a diaga,, a r, t diagt,, t r, we can deduce the lemma by putting a j t j By this lemma, this is equal to c λ Tr V τi kxk K W kx t k, kx t k deti x λ r+ dkdx I K R W,λ Tr V K W kx t k, kx t k e trx dkdx Since the reproducing kernel satisfies K K W kz t k, k w k τkk W z, wτk z, w p +, k K C, we have, for k K and x, Therefore we have Thus we get K W kx t k, kx t k τkk W x 4 xx 4, x 4 Ix 4 τk τkτx 4 KW x, eτx 4 τk Tr V K W kx, kx Tr V K W x, I, Tr V τi kxk K W kx t k, kx t k Tr V τi x K W x, I R W,λ c λ Now we set B W,λ : I I Tr V τi x K W x, I deti x λ r+ dkdx Tr V K W x, Ie trx dkdx Tr V τi x K W x, I deti x λ r+ dkdx, Γ W : Tr V K W x, Ie trx dkdx so that R W,λ c λ B W,λ /W W Now, we regard K W x, I Pp +, EndV as a function of x We define the action τ of K C on Pp +, EndV by τkf x : τkf k x t k τ t k k K C, F Pp +, EndV, x p + Then K W x, I is K L -invariant under τ Now we use the following isomorphism τ, Pp +, EndV ˆτ τ, Pp +, V V, 7

8 where τ, V is the complex conjugate of τ, V as a representation of L In this case L GLr, R, and we have τ, V τ, V Then under this isomorphism K W x, I sits in W V Since all the K L -spherical component in this tensor product has the lowest weight n, we conclude that K W x, I sits in V n, that is, there exists a function F Pp +, EndV such that, for any b b ij j i r t B, and τbf x b n b n b n r rr F x n b t b F x, τkf xdk K W x, I K L By using F, we rewrite B W,λ and Γ W B W,λ Tr V τi x F x deti x λ r+ dx, I Γ W Tr V F xe trx dx From now we calculate B W,λ For y, we set Iy : Tr V τy x F x dety x λ r+ dx y so that Ie B W,λ We take b t B such that y b t b, and set x bz t b Then Iy Tr V τbi z t b F bz t b detbi z t b λ r+ detb t b r+ dz I I I Tr V τi z τb F bz t bτ t b deti z λ r+ detb t r+ λ b dz Tr V τi z F z n b t b deti z λ r+ detb t r+ λ b dz r+ λ Ie n y dety B W,λ λ+n y dety r+ Now we calculate Iye try dy by two ways Iye try dy B W,λ e try λ+n y dety r+ dy BW,λ Γ λ + n, Iye try dy x,y x x,z Tr V e try Tr V τy x F x dety x λ r+ dxdy e trx+z Tr V τz F x detz λ r+ dxdz e trx F xdx e trz τz detz λ r+ dz Since e trz τz detz λ r+ dz commutes with K L -action and V KL is irreducible, this is the scalar operator on V Moreover, for a lowest weight vector v V and z b t b b t B, we have τz v, v τ τ t b b v, v τ τb v τ b k bkr rr v τ k b t b v τ k z v τ, 8

9 and e trz τz detz λ r+ dzv, v e trz k z detz λ r+ dz v τ Γ λ + k r + τ v τ Therefore e trz τz detz λ r+ dz Γ λ + k r+ idv, and B W,λ Γ Thus we have Now we determine c λ : References λ + k r+ Tr V e trx F xdx Γ Γ λ + n Γ λ + k r+ R W,λ c λ Γ λ + n Γ λ+k Then we have Γ λ+k r+ R W,λ Γ λ + k Γ λ + n Γ λ + k Γ λ Γ λ Γ λ + n λ k λ n λ + k r+ Γ W Γ λ + n [] J Faraut and A Korányi, Analysis on symmetric cones Oxford Mathematical Monographs Oxford Science Publications The Clarendon Press, Oxford University Press, New York, 994 [] S Hwang, Y Liu and G Zhang, Hilbert spaces of tensor-valued holomorphic functions on the unit ball of C n Pacific J Math 4 4, no, 33 3 [3] B Ørsted, Composition series for analytic continuations of holomorphic discrete series representations of SUn,n, Trans Amer Math Soc 6 98, no, [4] B Ørsted and G Zhang, Reproducing kernels and composition series for spaces of vector-valued holomorphic functions on tube domains J Funct Anal 4 994, no, 8 4 [5] B Ørsted and G Zhang, Reproducing kernels and composition series for spaces of vector-valued holomorphic functions Pacific J Math 7 995, no,

Symmetric Spaces. Andrew Fiori. Sept McGill University

Symmetric Spaces. Andrew Fiori. Sept McGill University McGill University Sept 2010 What are Hermitian? A Riemannian manifold M is called a Riemannian symmetric space if for each point x M there exists an involution s x which is an isometry of M and a neighbourhood

More information

Classification of discretely decomposable A q (λ) with respect to reductive symmetric pairs UNIVERSITY OF TOKYO

Classification of discretely decomposable A q (λ) with respect to reductive symmetric pairs UNIVERSITY OF TOKYO UTMS 2011 8 April 22, 2011 Classification of discretely decomposable A q (λ) with respect to reductive symmetric pairs by Toshiyuki Kobayashi and Yoshiki Oshima T UNIVERSITY OF TOKYO GRADUATE SCHOOL OF

More information

Representation Theory

Representation Theory Representation Theory Representations Let G be a group and V a vector space over a field k. A representation of G on V is a group homomorphism ρ : G Aut(V ). The degree (or dimension) of ρ is just dim

More information

A PIERI RULE FOR HERMITIAN SYMMETRIC PAIRS. Thomas J. Enright, Markus Hunziker and Nolan R. Wallach

A PIERI RULE FOR HERMITIAN SYMMETRIC PAIRS. Thomas J. Enright, Markus Hunziker and Nolan R. Wallach A PIERI RULE FOR HERMITIAN SYMMETRIC PAIRS Thomas J. Enright, Markus Hunziker and Nolan R. Wallach Abstract. Let (G, K) be a Hermitian symmetric pair and let g and k denote the corresponding complexified

More information

Talk at Workshop Quantum Spacetime 16 Zakopane, Poland,

Talk at Workshop Quantum Spacetime 16 Zakopane, Poland, Talk at Workshop Quantum Spacetime 16 Zakopane, Poland, 7-11.02.2016 Invariant Differential Operators: Overview (Including Noncommutative Quantum Conformal Invariant Equations) V.K. Dobrev Invariant differential

More information

Fermionic coherent states in infinite dimensions

Fermionic coherent states in infinite dimensions Fermionic coherent states in infinite dimensions Robert Oeckl Centro de Ciencias Matemáticas Universidad Nacional Autónoma de México Morelia, Mexico Coherent States and their Applications CIRM, Marseille,

More information

Symmetries, Fields and Particles. Examples 1.

Symmetries, Fields and Particles. Examples 1. Symmetries, Fields and Particles. Examples 1. 1. O(n) consists of n n real matrices M satisfying M T M = I. Check that O(n) is a group. U(n) consists of n n complex matrices U satisfying U U = I. Check

More information

THE CENTRALIZER OF K IN U(g) C(p) FOR THE GROUP SO e (4,1) Ana Prlić University of Zagreb, Croatia

THE CENTRALIZER OF K IN U(g) C(p) FOR THE GROUP SO e (4,1) Ana Prlić University of Zagreb, Croatia GLASNIK MATEMATIČKI Vol. 5(7)(017), 75 88 THE CENTRALIZER OF K IN U(g) C(p) FOR THE GROUP SO e (4,1) Ana Prlić University of Zagreb, Croatia Abstract. Let G be the Lie group SO e(4,1), with maximal compact

More information

Homogeneous para-kähler Einstein manifolds. Dmitri V. Alekseevsky

Homogeneous para-kähler Einstein manifolds. Dmitri V. Alekseevsky Homogeneous para-kähler Einstein manifolds Dmitri V. Alekseevsky Hamburg,14-18 July 2008 1 The talk is based on a joint work with C.Medori and A.Tomassini (Parma) See ArXiv 0806.2272, where also a survey

More information

SPHERICAL UNITARY REPRESENTATIONS FOR REDUCTIVE GROUPS

SPHERICAL UNITARY REPRESENTATIONS FOR REDUCTIVE GROUPS SPHERICAL UNITARY REPRESENTATIONS FOR REDUCTIVE GROUPS DAN CIUBOTARU 1. Classical motivation: spherical functions 1.1. Spherical harmonics. Let S n 1 R n be the (n 1)-dimensional sphere, C (S n 1 ) the

More information

Representation theory

Representation theory Representation theory Dr. Stuart Martin 2. Chapter 2: The Okounkov-Vershik approach These guys are Andrei Okounkov and Anatoly Vershik. The two papers appeared in 96 and 05. Here are the main steps: branching

More information

REPRESENTATION THEORY OF S n

REPRESENTATION THEORY OF S n REPRESENTATION THEORY OF S n EVAN JENKINS Abstract. These are notes from three lectures given in MATH 26700, Introduction to Representation Theory of Finite Groups, at the University of Chicago in November

More information

Elementary linear algebra

Elementary linear algebra Chapter 1 Elementary linear algebra 1.1 Vector spaces Vector spaces owe their importance to the fact that so many models arising in the solutions of specific problems turn out to be vector spaces. The

More information

IRREDUCIBLE REPRESENTATIONS OF SEMISIMPLE LIE ALGEBRAS. Contents

IRREDUCIBLE REPRESENTATIONS OF SEMISIMPLE LIE ALGEBRAS. Contents IRREDUCIBLE REPRESENTATIONS OF SEMISIMPLE LIE ALGEBRAS NEEL PATEL Abstract. The goal of this paper is to study the irreducible representations of semisimple Lie algebras. We will begin by considering two

More information

INTRODUCTION TO REPRESENTATION THEORY AND CHARACTERS

INTRODUCTION TO REPRESENTATION THEORY AND CHARACTERS INTRODUCTION TO REPRESENTATION THEORY AND CHARACTERS HANMING ZHANG Abstract. In this paper, we will first build up a background for representation theory. We will then discuss some interesting topics in

More information

EXPLICIT QUANTIZATION OF THE KEPLER MANIFOLD

EXPLICIT QUANTIZATION OF THE KEPLER MANIFOLD proceedings of the american mathematical Volume 77, Number 1, October 1979 society EXPLICIT QUANTIZATION OF THE KEPLER MANIFOLD ROBERT J. BLATTNER1 AND JOSEPH A. WOLF2 Abstract. Any representation ir of

More information

Cartan s Criteria. Math 649, Dan Barbasch. February 26

Cartan s Criteria. Math 649, Dan Barbasch. February 26 Cartan s Criteria Math 649, 2013 Dan Barbasch February 26 Cartan s Criteria REFERENCES: Humphreys, I.2 and I.3. Definition The Cartan-Killing form of a Lie algebra is the bilinear form B(x, y) := Tr(ad

More information

LECTURE 25-26: CARTAN S THEOREM OF MAXIMAL TORI. 1. Maximal Tori

LECTURE 25-26: CARTAN S THEOREM OF MAXIMAL TORI. 1. Maximal Tori LECTURE 25-26: CARTAN S THEOREM OF MAXIMAL TORI 1. Maximal Tori By a torus we mean a compact connected abelian Lie group, so a torus is a Lie group that is isomorphic to T n = R n /Z n. Definition 1.1.

More information

Traces, Cauchy identity, Schur polynomials

Traces, Cauchy identity, Schur polynomials June 28, 20 Traces, Cauchy identity, Schur polynomials Paul Garrett garrett@math.umn.edu http://www.math.umn.edu/ garrett/. Example: GL 2 2. GL n C and Un 3. Decomposing holomorphic polynomials over GL

More information

Representations of su(2)

Representations of su(2) Representations of su2 The purpose of these notes is to construct the representations of su2 using the method of weightvectors, based on the discussion of the representations of sl2, R in the notes for

More information

Topics in Representation Theory: Roots and Complex Structures

Topics in Representation Theory: Roots and Complex Structures Topics in Representation Theory: Roots and Complex Structures 1 More About Roots To recap our story so far: we began by identifying an important abelian subgroup of G, the maximal torus T. By restriction

More information

Topics in Representation Theory: Roots and Weights

Topics in Representation Theory: Roots and Weights Topics in Representation Theory: Roots and Weights 1 The Representation Ring Last time we defined the maximal torus T and Weyl group W (G, T ) for a compact, connected Lie group G and explained that our

More information

MAT 445/ INTRODUCTION TO REPRESENTATION THEORY

MAT 445/ INTRODUCTION TO REPRESENTATION THEORY MAT 445/1196 - INTRODUCTION TO REPRESENTATION THEORY CHAPTER 1 Representation Theory of Groups - Algebraic Foundations 1.1 Basic definitions, Schur s Lemma 1.2 Tensor products 1.3 Unitary representations

More information

INTRODUCTION TO LIE ALGEBRAS. LECTURE 7.

INTRODUCTION TO LIE ALGEBRAS. LECTURE 7. INTRODUCTION TO LIE ALGEBRAS. LECTURE 7. 7. Killing form. Nilpotent Lie algebras 7.1. Killing form. 7.1.1. Let L be a Lie algebra over a field k and let ρ : L gl(v ) be a finite dimensional L-module. Define

More information

Symmetry Characterization Theorems for Homogeneous Convex Cones and Siegel Domains. Takaaki NOMURA

Symmetry Characterization Theorems for Homogeneous Convex Cones and Siegel Domains. Takaaki NOMURA Symmetry Characterization Theorems for Homogeneous Convex Cones and Siegel Domains Takaaki NOMURA (Kyushu University) Cadi Ayyad University, Marrakech April 1 4, 2009 1 2 Interpretation via Cayley transform

More information

INTRODUCTION TO LIE ALGEBRAS. LECTURE 2.

INTRODUCTION TO LIE ALGEBRAS. LECTURE 2. INTRODUCTION TO LIE ALGEBRAS. LECTURE 2. 2. More examples. Ideals. Direct products. 2.1. More examples. 2.1.1. Let k = R, L = R 3. Define [x, y] = x y the cross-product. Recall that the latter is defined

More information

EXAM MATHEMATICAL METHODS OF PHYSICS. TRACK ANALYSIS (Chapters I-V). Thursday, June 7th,

EXAM MATHEMATICAL METHODS OF PHYSICS. TRACK ANALYSIS (Chapters I-V). Thursday, June 7th, EXAM MATHEMATICAL METHODS OF PHYSICS TRACK ANALYSIS (Chapters I-V) Thursday, June 7th, 1-13 Students who are entitled to a lighter version of the exam may skip problems 1, 8-11 and 16 Consider the differential

More information

Symmetries, Fields and Particles 2013 Solutions

Symmetries, Fields and Particles 2013 Solutions Symmetries, Fields and Particles 013 Solutions Yichen Shi Easter 014 1. (a) Define the groups SU() and SO(3), and find their Lie algebras. Show that these Lie algebras, including their bracket structure,

More information

REPRESENTATION THEORY WEEK 7

REPRESENTATION THEORY WEEK 7 REPRESENTATION THEORY WEEK 7 1. Characters of L k and S n A character of an irreducible representation of L k is a polynomial function constant on every conjugacy class. Since the set of diagonalizable

More information

Non-separable AF-algebras

Non-separable AF-algebras Non-separable AF-algebras Takeshi Katsura Department of Mathematics, Hokkaido University, Kita 1, Nishi 8, Kita-Ku, Sapporo, 6-81, JAPAN katsura@math.sci.hokudai.ac.jp Summary. We give two pathological

More information

1: Lie groups Matix groups, Lie algebras

1: Lie groups Matix groups, Lie algebras Lie Groups and Bundles 2014/15 BGSMath 1: Lie groups Matix groups, Lie algebras 1. Prove that O(n) is Lie group and that its tangent space at I O(n) is isomorphic to the space so(n) of skew-symmetric matrices

More information

On the Harish-Chandra Embedding

On the Harish-Chandra Embedding On the Harish-Chandra Embedding The purpose of this note is to link the Cartan and the root decompositions. In addition, it explains how we can view a Hermitian symmetric domain as G C /P where P is a

More information

These notes are incomplete they will be updated regularly.

These notes are incomplete they will be updated regularly. These notes are incomplete they will be updated regularly. LIE GROUPS, LIE ALGEBRAS, AND REPRESENTATIONS SPRING SEMESTER 2008 RICHARD A. WENTWORTH Contents 1. Lie groups and Lie algebras 2 1.1. Definition

More information

NOTES ON NEWLANDER-NIRENBERG THEOREM XU WANG

NOTES ON NEWLANDER-NIRENBERG THEOREM XU WANG NOTES ON NEWLANDER-NIRENBERG THEOREM XU WANG Abstract. In this short note we shall recall the classical Newler-Nirenberg theorem its vector bundle version. We shall also recall an L 2 -Hörmer-proof given

More information

The Spinor Representation

The Spinor Representation The Spinor Representation Math G4344, Spring 2012 As we have seen, the groups Spin(n) have a representation on R n given by identifying v R n as an element of the Clifford algebra C(n) and having g Spin(n)

More information

14 From modular forms to automorphic representations

14 From modular forms to automorphic representations 14 From modular forms to automorphic representations We fix an even integer k and N > 0 as before. Let f M k (N) be a modular form. We would like to product a function on GL 2 (A Q ) out of it. Recall

More information

X-RAY TRANSFORM ON DAMEK-RICCI SPACES. (Communicated by Jan Boman)

X-RAY TRANSFORM ON DAMEK-RICCI SPACES. (Communicated by Jan Boman) Volume X, No. 0X, 00X, X XX Web site: http://www.aimsciences.org X-RAY TRANSFORM ON DAMEK-RICCI SPACES To Jan Boman on his seventy-fifth birthday. François Rouvière Laboratoire J.A. Dieudonné Université

More information

BRST and Dirac Cohomology

BRST and Dirac Cohomology BRST and Dirac Cohomology Peter Woit Columbia University Dartmouth Math Dept., October 23, 2008 Peter Woit (Columbia University) BRST and Dirac Cohomology October 2008 1 / 23 Outline 1 Introduction 2 Representation

More information

Intertwining integrals on completely solvable Lie groups

Intertwining integrals on completely solvable Lie groups s on s on completely solvable Lie June 16, 2011 In this talk I shall explain a topic which interests me in my collaboration with Ali Baklouti and Jean Ludwig. s on In this talk I shall explain a topic

More information

Group Theory - QMII 2017

Group Theory - QMII 2017 Group Theory - QMII 017 Reminder Last time we said that a group element of a matrix lie group can be written as an exponent: U = e iαaxa, a = 1,..., N. We called X a the generators, we have N of them,

More information

A method for construction of Lie group invariants

A method for construction of Lie group invariants arxiv:1206.4395v1 [math.rt] 20 Jun 2012 A method for construction of Lie group invariants Yu. Palii Laboratory of Information Technologies, Joint Institute for Nuclear Research, Dubna, Russia and Institute

More information

TRANSLATION-INVARIANT FUNCTION ALGEBRAS ON COMPACT GROUPS

TRANSLATION-INVARIANT FUNCTION ALGEBRAS ON COMPACT GROUPS PACIFIC JOURNAL OF MATHEMATICS Vol. 15, No. 3, 1965 TRANSLATION-INVARIANT FUNCTION ALGEBRAS ON COMPACT GROUPS JOSEPH A. WOLF Let X be a compact group. $(X) denotes the Banach algebra (point multiplication,

More information

CLASSICAL GROUPS DAVID VOGAN

CLASSICAL GROUPS DAVID VOGAN CLASSICAL GROUPS DAVID VOGAN 1. Orthogonal groups These notes are about classical groups. That term is used in various ways by various people; I ll try to say a little about that as I go along. Basically

More information

Subquotients of Minimal Principal Series

Subquotients of Minimal Principal Series Subquotients of Minimal Principal Series ν 1 = ν 2 Sp(4) 0 1 2 ν 2 = 0 Alessandra Pantano, UCI July 2008 1 PART 1 Introduction Preliminary Definitions and Notation 2 Langlands Quotients of Minimal Principal

More information

Homogeneous spaces of compact connected Lie groups which admit nontrivial invariant algebras

Homogeneous spaces of compact connected Lie groups which admit nontrivial invariant algebras Journal of Lie Theory Volume 9 (1999) 355 360 C 1999 Heldermann Verlag Homogeneous spaces of compact connected Lie groups which admit nontrivial invariant algebras Ilyas A. Latypov Communicated by E. B.

More information

On classification of minimal orbits of the Hermann action satisfying Koike s conditions (Joint work with Minoru Yoshida)

On classification of minimal orbits of the Hermann action satisfying Koike s conditions (Joint work with Minoru Yoshida) Proceedings of The 21st International Workshop on Hermitian Symmetric Spaces and Submanifolds 21(2017) 1-2 On classification of minimal orbits of the Hermann action satisfying Koike s conditions (Joint

More information

On the singular elements of a semisimple Lie algebra and the generalized Amitsur-Levitski Theorem

On the singular elements of a semisimple Lie algebra and the generalized Amitsur-Levitski Theorem On the singular elements of a semisimple Lie algebra and the generalized Amitsur-Levitski Theorem Bertram Kostant, MIT Conference on Representations of Reductive Groups Salt Lake City, Utah July 10, 2013

More information

Unitarity of non-spherical principal series

Unitarity of non-spherical principal series Unitarity of non-spherical principal series Alessandra Pantano July 2005 1 Minimal Principal Series G: a real split semisimple Lie group θ: Cartan involution; g = k p: Cartan decomposition of g a: maximal

More information

Introduction to Index Theory. Elmar Schrohe Institut für Analysis

Introduction to Index Theory. Elmar Schrohe Institut für Analysis Introduction to Index Theory Elmar Schrohe Institut für Analysis Basics Background In analysis and pde, you want to solve equations. In good cases: Linearize, end up with Au = f, where A L(E, F ) is a

More information

Part III Symmetries, Fields and Particles

Part III Symmetries, Fields and Particles Part III Symmetries, Fields and Particles Theorems Based on lectures by N. Dorey Notes taken by Dexter Chua Michaelmas 2016 These notes are not endorsed by the lecturers, and I have modified them (often

More information

Notes on Lie Algebras

Notes on Lie Algebras NEW MEXICO TECH (October 23, 2010) DRAFT Notes on Lie Algebras Ivan G. Avramidi Department of Mathematics New Mexico Institute of Mining and Technology Socorro, NM 87801, USA E-mail: iavramid@nmt.edu 1

More information

Topics in Representation Theory: Fourier Analysis and the Peter Weyl Theorem

Topics in Representation Theory: Fourier Analysis and the Peter Weyl Theorem Topics in Representation Theory: Fourier Analysis and the Peter Weyl Theorem 1 Fourier Analysis, a review We ll begin with a short review of simple facts about Fourier analysis, before going on to interpret

More information

Dirac Cohomology, Orbit Method and Unipotent Representations

Dirac Cohomology, Orbit Method and Unipotent Representations Dirac Cohomology, Orbit Method and Unipotent Representations Dedicated to Bert Kostant with great admiration Jing-Song Huang, HKUST Kostant Conference MIT, May 28 June 1, 2018 coadjoint orbits of reductive

More information

arxiv: v1 [math.rt] 31 Oct 2008

arxiv: v1 [math.rt] 31 Oct 2008 Cartan Helgason theorem, Poisson transform, and Furstenberg Satake compactifications arxiv:0811.0029v1 [math.rt] 31 Oct 2008 Adam Korányi* Abstract The connections between the objects mentioned in the

More information

Lemma 1.3. The element [X, X] is nonzero.

Lemma 1.3. The element [X, X] is nonzero. Math 210C. The remarkable SU(2) Let G be a non-commutative connected compact Lie group, and assume that its rank (i.e., dimension of maximal tori) is 1; equivalently, G is a compact connected Lie group

More information

Representations of algebraic groups and their Lie algebras Jens Carsten Jantzen Lecture III

Representations of algebraic groups and their Lie algebras Jens Carsten Jantzen Lecture III Representations of algebraic groups and their Lie algebras Jens Carsten Jantzen Lecture III Lie algebras. Let K be again an algebraically closed field. For the moment let G be an arbitrary algebraic group

More information

AN UPPER BOUND FOR SIGNATURES OF IRREDUCIBLE, SELF-DUAL gl(n, C)-REPRESENTATIONS

AN UPPER BOUND FOR SIGNATURES OF IRREDUCIBLE, SELF-DUAL gl(n, C)-REPRESENTATIONS AN UPPER BOUND FOR SIGNATURES OF IRREDUCIBLE, SELF-DUAL gl(n, C)-REPRESENTATIONS CHRISTOPHER XU UROP+ Summer 2018 Mentor: Daniil Kalinov Project suggested by David Vogan Abstract. For every irreducible,

More information

INTRODUCTION TO LIE ALGEBRAS. LECTURE 1.

INTRODUCTION TO LIE ALGEBRAS. LECTURE 1. INTRODUCTION TO LIE ALGEBRAS. LECTURE 1. 1. Algebras. Derivations. Definition of Lie algebra 1.1. Algebras. Let k be a field. An algebra over k (or k-algebra) is a vector space A endowed with a bilinear

More information

Rings and groups. Ya. Sysak

Rings and groups. Ya. Sysak Rings and groups. Ya. Sysak 1 Noetherian rings Let R be a ring. A (right) R -module M is called noetherian if it satisfies the maximum condition for its submodules. In other words, if M 1... M i M i+1...

More information

Howe Duality Correspondence of (O(p, q), osp(2, 2))

Howe Duality Correspondence of (O(p, q), osp(2, 2)) Howe Duality Correspondence of (O(p, q), osp(, )) Dan Lu November 19, 009 Abstract The local theta correspondence for reductive dual pairs of subgroups of the symplectic group formulated by R. Howe has

More information

Math 210C. The representation ring

Math 210C. The representation ring Math 210C. The representation ring 1. Introduction Let G be a nontrivial connected compact Lie group that is semisimple and simply connected (e.g., SU(n) for n 2, Sp(n) for n 1, or Spin(n) for n 3). Let

More information

Zonal Polynomials and Hypergeometric Functions of Matrix Argument. Zonal Polynomials and Hypergeometric Functions of Matrix Argument p.

Zonal Polynomials and Hypergeometric Functions of Matrix Argument. Zonal Polynomials and Hypergeometric Functions of Matrix Argument p. Zonal Polynomials and Hypergeometric Functions of Matrix Argument Zonal Polynomials and Hypergeometric Functions of Matrix Argument p. 1/2 Zonal Polynomials and Hypergeometric Functions of Matrix Argument

More information

Highest-weight Theory: Verma Modules

Highest-weight Theory: Verma Modules Highest-weight Theory: Verma Modules Math G4344, Spring 2012 We will now turn to the problem of classifying and constructing all finitedimensional representations of a complex semi-simple Lie algebra (or,

More information

A simple proof of the existence of sampling spaces with the interpolation property on the Heisenberg group

A simple proof of the existence of sampling spaces with the interpolation property on the Heisenberg group A simple proof of the existence of sampling spaces with the interpolation property on the Heisenberg group Vignon Oussa Abstract A surprisingly short geometric proof of the existence of sampling spaces

More information

ISOLATED SEMIDEFINITE SOLUTIONS OF THE CONTINUOUS-TIME ALGEBRAIC RICCATI EQUATION

ISOLATED SEMIDEFINITE SOLUTIONS OF THE CONTINUOUS-TIME ALGEBRAIC RICCATI EQUATION ISOLATED SEMIDEFINITE SOLUTIONS OF THE CONTINUOUS-TIME ALGEBRAIC RICCATI EQUATION Harald K. Wimmer 1 The set of all negative-semidefinite solutions of the CARE A X + XA + XBB X C C = 0 is homeomorphic

More information

Non separated points in the dual spaces of semi simple Lie groups

Non separated points in the dual spaces of semi simple Lie groups 1 Non separated points in the dual spaces of semi simple Lie groups Let G be a connected semi simple Lie group with finite center, g its Lie algebra, g c = g R C, G the universal enveloping algebra of

More information

is an isomorphism, and V = U W. Proof. Let u 1,..., u m be a basis of U, and add linearly independent

is an isomorphism, and V = U W. Proof. Let u 1,..., u m be a basis of U, and add linearly independent Lecture 4. G-Modules PCMI Summer 2015 Undergraduate Lectures on Flag Varieties Lecture 4. The categories of G-modules, mostly for finite groups, and a recipe for finding every irreducible G-module of a

More information

Symmetric Spaces Toolkit

Symmetric Spaces Toolkit Symmetric Spaces Toolkit SFB/TR12 Langeoog, Nov. 1st 7th 2007 H. Sebert, S. Mandt Contents 1 Lie Groups and Lie Algebras 2 1.1 Matrix Lie Groups........................ 2 1.2 Lie Group Homomorphisms...................

More information

A CHARACTERIZATION OF THE MOONSHINE VERTEX OPERATOR ALGEBRA BY MEANS OF VIRASORO FRAMES. 1. Introduction

A CHARACTERIZATION OF THE MOONSHINE VERTEX OPERATOR ALGEBRA BY MEANS OF VIRASORO FRAMES. 1. Introduction A CHARACTERIZATION OF THE MOONSHINE VERTEX OPERATOR ALGEBRA BY MEANS OF VIRASORO FRAMES CHING HUNG LAM AND HIROSHI YAMAUCHI Abstract. In this article, we show that a framed vertex operator algebra V satisfying

More information

SYMPLECTIC GEOMETRY: LECTURE 5

SYMPLECTIC GEOMETRY: LECTURE 5 SYMPLECTIC GEOMETRY: LECTURE 5 LIAT KESSLER Let (M, ω) be a connected compact symplectic manifold, T a torus, T M M a Hamiltonian action of T on M, and Φ: M t the assoaciated moment map. Theorem 0.1 (The

More information

Symmetries, Fields and Particles 2013 Solutions

Symmetries, Fields and Particles 2013 Solutions Symmetries, Fields and Particles 03 Solutions Yichen Shi July 9, 04. a Define the groups SU and SO3, and find their Lie algebras. Show that these Lie algebras, including their bracket structure, are isomorphic.

More information

Since G is a compact Lie group, we can apply Schur orthogonality to see that G χ π (g) 2 dg =

Since G is a compact Lie group, we can apply Schur orthogonality to see that G χ π (g) 2 dg = Problem 1 Show that if π is an irreducible representation of a compact lie group G then π is also irreducible. Give an example of a G and π such that π = π, and another for which π π. Is this true for

More information

2.2. OPERATOR ALGEBRA 19. If S is a subset of E, then the set

2.2. OPERATOR ALGEBRA 19. If S is a subset of E, then the set 2.2. OPERATOR ALGEBRA 19 2.2 Operator Algebra 2.2.1 Algebra of Operators on a Vector Space A linear operator on a vector space E is a mapping L : E E satisfying the condition u, v E, a R, L(u + v) = L(u)

More information

Representations of moderate growth Paul Garrett 1. Constructing norms on groups

Representations of moderate growth Paul Garrett 1. Constructing norms on groups (December 31, 2004) Representations of moderate growth Paul Garrett Representations of reductive real Lie groups on Banach spaces, and on the smooth vectors in Banach space representations,

More information

08a. Operators on Hilbert spaces. 1. Boundedness, continuity, operator norms

08a. Operators on Hilbert spaces. 1. Boundedness, continuity, operator norms (February 24, 2017) 08a. Operators on Hilbert spaces Paul Garrett garrett@math.umn.edu http://www.math.umn.edu/ garrett/ [This document is http://www.math.umn.edu/ garrett/m/real/notes 2016-17/08a-ops

More information

REPRESENTATION THEORY NOTES FOR MATH 4108 SPRING 2012

REPRESENTATION THEORY NOTES FOR MATH 4108 SPRING 2012 REPRESENTATION THEORY NOTES FOR MATH 4108 SPRING 2012 JOSEPHINE YU This note will cover introductory material on representation theory, mostly of finite groups. The main references are the books of Serre

More information

Lecture 7: Positive Semidefinite Matrices

Lecture 7: Positive Semidefinite Matrices Lecture 7: Positive Semidefinite Matrices Rajat Mittal IIT Kanpur The main aim of this lecture note is to prepare your background for semidefinite programming. We have already seen some linear algebra.

More information

Branching rules of unitary representations: Examples and applications to automorphic forms.

Branching rules of unitary representations: Examples and applications to automorphic forms. Branching rules of unitary representations: Examples and applications to automorphic forms. Basic Notions: Jerusalem, March 2010 Birgit Speh Cornell University 1 Let G be a group and V a vector space.

More information

LIE ALGEBRAS: LECTURE 7 11 May 2010

LIE ALGEBRAS: LECTURE 7 11 May 2010 LIE ALGEBRAS: LECTURE 7 11 May 2010 CRYSTAL HOYT 1. sl n (F) is simple Let F be an algebraically closed field with characteristic zero. Let V be a finite dimensional vector space. Recall, that f End(V

More information

EXERCISES IN MODULAR FORMS I (MATH 726) (2) Prove that a lattice L is integral if and only if its Gram matrix has integer coefficients.

EXERCISES IN MODULAR FORMS I (MATH 726) (2) Prove that a lattice L is integral if and only if its Gram matrix has integer coefficients. EXERCISES IN MODULAR FORMS I (MATH 726) EYAL GOREN, MCGILL UNIVERSITY, FALL 2007 (1) We define a (full) lattice L in R n to be a discrete subgroup of R n that contains a basis for R n. Prove that L is

More information

INTRODUCTION TO LIE ALGEBRAS. LECTURE 10.

INTRODUCTION TO LIE ALGEBRAS. LECTURE 10. INTRODUCTION TO LIE ALGEBRAS. LECTURE 10. 10. Jordan decomposition: theme with variations 10.1. Recall that f End(V ) is semisimple if f is diagonalizable (over the algebraic closure of the base field).

More information

The Heat equation, the Segal-Bargmann transform and generalizations. B. Krötz B. Ørsted H. Schlichtkrull R. Stanton

The Heat equation, the Segal-Bargmann transform and generalizations. B. Krötz B. Ørsted H. Schlichtkrull R. Stanton The Heat equation, the Segal-Bargmann transform and generalizations Based on joint work with B. Krötz B. Ørsted H. Schlichtkrull R. Stanton - p. 1/54 Organizations 1. The heat equation on R n. 2. The Fock

More information

Lie Algebras. Shlomo Sternberg

Lie Algebras. Shlomo Sternberg Lie Algebras Shlomo Sternberg March 8, 2004 2 Chapter 5 Conjugacy of Cartan subalgebras It is a standard theorem in linear algebra that any unitary matrix can be diagonalized (by conjugation by unitary

More information

Weyl Group Representations and Unitarity of Spherical Representations.

Weyl Group Representations and Unitarity of Spherical Representations. Weyl Group Representations and Unitarity of Spherical Representations. Alessandra Pantano, University of California, Irvine Windsor, October 23, 2008 β ν 1 = ν 2 S α S β ν S β ν S α ν S α S β S α S β ν

More information

REGULAR TRIPLETS IN COMPACT SYMMETRIC SPACES

REGULAR TRIPLETS IN COMPACT SYMMETRIC SPACES REGULAR TRIPLETS IN COMPACT SYMMETRIC SPACES MAKIKO SUMI TANAKA 1. Introduction This article is based on the collaboration with Tadashi Nagano. In the first part of this article we briefly review basic

More information

The Cartan Decomposition of a Complex Semisimple Lie Algebra

The Cartan Decomposition of a Complex Semisimple Lie Algebra The Cartan Decomposition of a Complex Semisimple Lie Algebra Shawn Baland University of Colorado, Boulder November 29, 2007 Definition Let k be a field. A k-algebra is a k-vector space A equipped with

More information

Transformations Groups of the Andersson-Perlman Cone

Transformations Groups of the Andersson-Perlman Cone Journal of Lie Theory Volume 9 (1999) 203 213 C 1999 Heldermann. Verlag Transformations Groups of the Andersson-Perlman Cone Erhard Neher Communicated by J. Faraut Abstract. An Andersson-Perlman cone is

More information

HYPERKÄHLER MANIFOLDS

HYPERKÄHLER MANIFOLDS HYPERKÄHLER MANIFOLDS PAVEL SAFRONOV, TALK AT 2011 TALBOT WORKSHOP 1.1. Basic definitions. 1. Hyperkähler manifolds Definition. A hyperkähler manifold is a C Riemannian manifold together with three covariantly

More information

C*-Algebras and Group Representations

C*-Algebras and Group Representations C*-Algebras and Department of Mathematics Pennsylvania State University EMS Joint Mathematical Weekend University of Copenhagen, February 29, 2008 Outline Summary Mackey pointed out an analogy between

More information

Induced Representations and Frobenius Reciprocity. 1 Generalities about Induced Representations

Induced Representations and Frobenius Reciprocity. 1 Generalities about Induced Representations Induced Representations Frobenius Reciprocity Math G4344, Spring 2012 1 Generalities about Induced Representations For any group G subgroup H, we get a restriction functor Res G H : Rep(G) Rep(H) that

More information

Mic ael Flohr Representation theory of semi-simple Lie algebras: Example su(3) 6. and 20. June 2003

Mic ael Flohr Representation theory of semi-simple Lie algebras: Example su(3) 6. and 20. June 2003 Handout V for the course GROUP THEORY IN PHYSICS Mic ael Flohr Representation theory of semi-simple Lie algebras: Example su(3) 6. and 20. June 2003 GENERALIZING THE HIGHEST WEIGHT PROCEDURE FROM su(2)

More information

H(G(Q p )//G(Z p )) = C c (SL n (Z p )\ SL n (Q p )/ SL n (Z p )).

H(G(Q p )//G(Z p )) = C c (SL n (Z p )\ SL n (Q p )/ SL n (Z p )). 92 19. Perverse sheaves on the affine Grassmannian 19.1. Spherical Hecke algebra. The Hecke algebra H(G(Q p )//G(Z p )) resp. H(G(F q ((T ))//G(F q [[T ]])) etc. of locally constant compactly supported

More information

HOLOMORPHIC RETRACTIONS AND BOUNDARY BEREZIN TRANSFORMS

HOLOMORPHIC RETRACTIONS AND BOUNDARY BEREZIN TRANSFORMS HOLOMORPHIC RETRACTIONS AND BOUNDARY BEREZIN TRANSFORMS JONATHAN ARAZY, MIROSLAV ENGLIŠ, AND WILHELM KAUP Abstract. In an earlier paper, the first two authors have shown that the convolution of a function

More information

On the Irreducibility of the Commuting Variety of the Symmetric Pair so p+2, so p so 2

On the Irreducibility of the Commuting Variety of the Symmetric Pair so p+2, so p so 2 Journal of Lie Theory Volume 16 (2006) 57 65 c 2006 Heldermann Verlag On the Irreducibility of the Commuting Variety of the Symmetric Pair so p+2, so p so 2 Hervé Sabourin and Rupert W.T. Yu Communicated

More information

Representations of Totally Disconnected Groups

Representations of Totally Disconnected Groups Chapter 5 Representations of Totally Disconnected Groups Abstract In this chapter our goal is to develop enough of the representation theory of locally compact totally disconnected groups (or td groups

More information

SEMISIMPLE LIE GROUPS

SEMISIMPLE LIE GROUPS SEMISIMPLE LIE GROUPS BRIAN COLLIER 1. Outiline The goal is to talk about semisimple Lie groups, mainly noncompact real semisimple Lie groups. This is a very broad subject so we will do our best to be

More information

k=0 /D : S + S /D = K 1 2 (3.5) consistently with the relation (1.75) and the Riemann-Roch-Hirzebruch-Atiyah-Singer index formula

k=0 /D : S + S /D = K 1 2 (3.5) consistently with the relation (1.75) and the Riemann-Roch-Hirzebruch-Atiyah-Singer index formula 20 VASILY PESTUN 3. Lecture: Grothendieck-Riemann-Roch-Hirzebruch-Atiyah-Singer Index theorems 3.. Index for a holomorphic vector bundle. For a holomorphic vector bundle E over a complex variety of dim

More information

2-STEP NILPOTENT LIE GROUPS ARISING FROM SEMISIMPLE MODULES

2-STEP NILPOTENT LIE GROUPS ARISING FROM SEMISIMPLE MODULES 2-STEP NILPOTENT LIE GROUPS ARISING FROM SEMISIMPLE MODULES PATRICK EBERLEIN UNIVERSITY OF NORTH CAROLINA AT CHAPEL HILL Abstract Let G 0 denote a compact semisimple Lie algebra and U a finite dimensional

More information

The Real Grassmannian Gr(2, 4)

The Real Grassmannian Gr(2, 4) The Real Grassmannian Gr(2, 4) We discuss the topology of the real Grassmannian Gr(2, 4) of 2-planes in R 4 and its double cover Gr + (2, 4) by the Grassmannian of oriented 2-planes They are compact four-manifolds

More information

An Introduction to Kuga Fiber Varieties

An Introduction to Kuga Fiber Varieties An Introduction to Kuga Fiber Varieties Dylan Attwell-Duval Department of Mathematics and Statistics McGill University Montreal, Quebec attwellduval@math.mcgill.ca April 28, 2012 Notation G a Q-simple

More information