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

Similar documents
MAT 445/ INTRODUCTION TO REPRESENTATION THEORY

Representation Theory

Representation Theory

Math 250: Higher Algebra Representations of finite groups

L(C G (x) 0 ) c g (x). Proof. Recall C G (x) = {g G xgx 1 = g} and c g (x) = {X g Ad xx = X}. In general, it is obvious that

REPRESENTATION THEORY WEEK 5. B : V V k

Algebra Questions. May 13, Groups 1. 2 Classification of Finite Groups 4. 3 Fields and Galois Theory 5. 4 Normal Forms 9

REPRESENTATION THEORY WEEK 7

Notes on nilpotent orbits Computational Theory of Real Reductive Groups Workshop. Eric Sommers

Exercises on chapter 4

INTRODUCTION TO REPRESENTATION THEORY AND CHARACTERS

Problems in Linear Algebra and Representation Theory

Real representations

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

CHAPTER 6. Representations of compact groups

3 Representations of finite groups: basic results

Math 210C. The representation ring

REPRESENTATIONS OF S n AND GL(n, C)

REPRESENTATION THEORY NOTES FOR MATH 4108 SPRING 2012

A Field Extension as a Vector Space

Character tables for some small groups

Representations. 1 Basic definitions

Algebra Exam Topics. Updated August 2017

REPRESENTATION THEORY OF S n

Representation Theory. Ricky Roy Math 434 University of Puget Sound

Algebra SEP Solutions

A PROOF OF BURNSIDE S p a q b THEOREM

Weeks 6 and 7. November 24, 2013

GRE Subject test preparation Spring 2016 Topic: Abstract Algebra, Linear Algebra, Number Theory.

Exercises on chapter 1

10 l-adic representations

CHARACTERS OF FINITE GROUPS.

1 Homework 8 Solutions

18.702: Quiz 1 Solutions

REPRESENTATION THEORY, LECTURE 0. BASICS


MAT 449 : Problem Set 7

Solutions to Example Sheet 1

Notes 10: Consequences of Eli Cartan s theorem.

Math 594. Solutions 5

LECTURE 4: REPRESENTATION THEORY OF SL 2 (F) AND sl 2 (F)

ALGEBRA QUALIFYING EXAM PROBLEMS LINEAR ALGEBRA

Topics in linear algebra

ALGEBRAIC GROUPS J. WARNER

Exercises Lie groups

ALGEBRA QUALIFYING EXAM, FALL 2017: SOLUTIONS

33 Idempotents and Characters

4 Group representations

Elementary linear algebra

MATH 101A: ALGEBRA I, PART D: GALOIS THEORY 11

REPRESENTATIONS OF U(N) CLASSIFICATION BY HIGHEST WEIGHTS NOTES FOR MATH 261, FALL 2001

Real, Complex, and Quarternionic Representations

ALGEBRA QUALIFYING EXAM PROBLEMS

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

Notation. For any Lie group G, we set G 0 to be the connected component of the identity.

SOLVABLE FUSION CATEGORIES AND A CATEGORICAL BURNSIDE S THEOREM

THE EULER CHARACTERISTIC OF A LIE GROUP

Real Analysis Prelim Questions Day 1 August 27, 2013

Honors Algebra 4, MATH 371 Winter 2010 Assignment 4 Due Wednesday, February 17 at 08:35

Some notes on Coxeter groups

Linear Algebra. Workbook

Weyl Group Representations and Unitarity of Spherical Representations.

5 Irreducible representations

Math 306 Topics in Algebra, Spring 2013 Homework 7 Solutions

CHARACTER THEORY OF FINITE GROUPS. Chapter 1: REPRESENTATIONS

1. Group Theory Permutations.

1 Fields and vector spaces

14 From modular forms to automorphic representations

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

REPRESENTATION THEORY FOR FINITE GROUPS

LINEAR ALGEBRA BOOT CAMP WEEK 4: THE SPECTRAL THEOREM

CHARACTERS AS CENTRAL IDEMPOTENTS

Appendix Homework and answers

A PRIMER ON SESQUILINEAR FORMS

Math 25a Practice Final #1 Solutions

LECTURE 3: REPRESENTATION THEORY OF SL 2 (C) AND sl 2 (C)

Peter Hochs. Strings JC, 11 June, C -algebras and K-theory. Peter Hochs. Introduction. C -algebras. Group. C -algebras.

FFTs in Graphics and Vision. Groups and Representations

Highest-weight Theory: Verma Modules

MATRIX LIE GROUPS AND LIE GROUPS

Problem set 2. Math 212b February 8, 2001 due Feb. 27

Weil Representations of Finite Fields

9 Artin representations

Liouvillian solutions of third order differential equations

LIE ALGEBRAS: LECTURE 7 11 May 2010

ORAL QUALIFYING EXAM QUESTIONS. 1. Algebra

Representation theory and quantum mechanics tutorial Spin and the hydrogen atom

5 Quiver Representations

Exercises on chapter 4

AHAHA: Preliminary results on p-adic groups and their representations.

Index. Banach space 630 Basic Jordan block 378, 420

The Gelfand-Tsetlin Basis (Too Many Direct Sums, and Also a Graph)

Functional Analysis Review

UC Berkeley Summer Undergraduate Research Program 2015 July 9 Lecture

CHARACTERISTIC POLYNOMIAL PATTERNS IN DIFFERENCE SETS OF MATRICES

Permutation groups/1. 1 Automorphism groups, permutation groups, abstract

Topics in Representation Theory: Roots and Weights

Solution. That ϕ W is a linear map W W follows from the definition of subspace. The map ϕ is ϕ(v + W ) = ϕ(v) + W, which is well-defined since

Notes on Representations of Finite Groups. Ambar N. Sengupta

Profinite Groups. Hendrik Lenstra. 1. Introduction

Transcription:

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 general groups? Since G is a compact Lie group, we can apply Schur orthogonality to see that G χ π (g) 2 dg = G χ π(g) 2 dg = G χ π(g) 2 dg = 1, so π is irreducible. For any G, the trivial representation π satisfies π π. For G the cyclic group of order 3 generated by g, the representation π : g i ζ3 i is not isomorphic to π : g i ζ3 i. This is true for finite dimensional irreducible representations. This follows as if W V a proper, non-zero G-invariant representation for a group G, then W = {φ V φ(w ) = 0} is a proper, non-zero G-invariant subspace and applying this to V as V = V we get V is irreducible if and only if V is irreducible. This is false for general representations and general groups. Take G = S to be the symmetric group on countably infinitely many letters, and let G act on a vector space V over C with basis e 1, e 2, by sending σ : e i e σ(i). Let W be the sub-representation given by the kernel of the map V C sending λ i e i λ i. Then W is irreducible because given any λ 1 e 1 + + λ n e n V where λ n 0, and we see that λ 1 n [(n n + 1) 1] C[G] sends this to e n+1 e n, and elements like this span W. Then W will be functions on W, which is uncountable. Let e i be the dual of e i, so the subspace of those functions spanned by the e i has countable dimension and is a subrepresentation. Problem 2 Show that the only finite dimensional unitary representation of SL(n, R) trivial. (Hint: You can use the fact that the Lie algebra sl n is simple.) Let π : SL(n, R) U(m) be a finite dimensional unitary representation. As SL(n, R) is connected, it follows that π is determined uniquely from dπ : sl(n, R) u(m). Taking the inclusions sl(2) sl(n) and u(m) gl(v ) where V is an m-dimensional complex vector space, find a highest weight vector v V on which h sl(2) acts by hv = λv, where λ is a nonnegative integer. Since h acts as a skew-hermitian matrix, its eigenvalues are purely imaginary so that forces λ = 0. So h acts as 0 on all of V, hence the kernel is always nontrivial. The kernel is then a nonzero ideal of sl(n), so by simplicity it is all of sl(n). As π is determined by dπ, we conclude that π is trivial. Problem 3 Let G be a group acting on a finite dimensional vector space V 0 over R. In this case we will call the representation V := V 0 R C, real (i.e. We will call a representation V of G over C real, if it is obtained by complexifying a representation over R.). (a) Let us talk a bit about characters and finite groups. For a finite group G, the character table of G is the table with first row consisting of the conjugacy classes, the first column consisting of the characters of irreducible representations, and each entry is the value χ(γ) for the corresponding character χ and conjugacy class γ. i. If two finite groups have the same character table does it imply that they are isomorphic? ii. Show that the entries of the character table are algebraic numbers (they actually belong to a cyclotomic extension of Q). iii. Let Gal be the Galois group of the (Galois closure of the) field obtained by adjoining all the entries of the character table acts on the table by shuffling the entries. Show that Gal acts 1

on the character table by permuting rows and columns. (Bonus) Show, furthermore, that the cycle type of the action over the rows is the same as the one over columns. (b) Now back to general compact groups. It is clear that if π is a real representation then its character χ π is real valued. Is the converse true? i.e. If the character (of a representation on a finite dimensional C-vector space) is real valued does it necessarily imply that the representation is real? Hint: Think of finite groups. (c) Show that an irreducible representation (π, V ) is real if and only if there exists a non-degenerate, symmetric, bilinear, G-invariant form on V. (d) Let G be a compact group and (π, V ), (σ, W ) be two irreducible representations of G. Show that the space of G-invariant bilinear forms B : V W C is at most one dimensional. Moreover, show that it is one dimensional if and only if π = σ. Show also that in the case π = π and B(, ) is a G-invariant invariant bilinear form, ɛ π {±1} such that B(v, w) = ɛ π B(w, v). (This ɛ π is called the Frobenius-Schur indicator of π.) (a) i. Since G is finite, we know that every function is a matrix coefficient as its left G-translates span a finite dimensional space. Since matrix coefficients that happen to be class functions are linear combinations of characters, we see that characters span the whole space of class functions, so the number of characters (and hence the number of irreducible representations) is the number of conjugacy classes. Computation reveals that the quaternion group Q 8 and the dihedral group D 8 both have five conjugacy classes. Their character tables will be the same, but they are not isomorphic. Present D 8 as r, s r 4 = s 2 = (rs) 2 = 1 and Q 8 as i, j i 4 = j 4 = 1, ij = j 3 i. They both have four one dimensional representations, where their generators r, s or i, j get sent to ±1. By orthogonality relations this determines the last representation completely. There is a bijection between them that preserves conjugacy classes, namely {1} {1}, {r 2 } { 1}, {r ±1 } {±i}, {s, r 2 s} {±j}, {r ±1 s} {±ij}, so the sizes of their conjugacy classes are 1, 1, 2, 2, 2. Their character tables will then be D 8 1 r 2 r ±1 s, r 2 s r ±1 s Q 8 1 1 ±i ±j ±k C ++ 1 1 1 1 1 C + 1 1 1 1 1 C + 1 1 1 1 1 C 1 1 1 1 1 C 2 2 2 0 0 0 ii. Any matrix in the representation must act as a G -th root of the identity, hence its eigenvalues are G -th roots of unity since the characteristic polynomial has the same roots as the minimal polynomial, which divides T G 1. So the trace lies in Q(ζ G ). iii. First we show that every representation is defined over Q. To see this the same proof as over any algebraically closed field shows that there are the number of conjugacy classes of irreducible representations defined over Q and thus all the irreducible representations of C are defined over Q. Let σ be in the absolute Galois group of Q. For any irreducible representation π : G GL(V ), then we can apply σ to all the entries of the matrices of π(g) to get a new irreducible 2

representation whose character is σ(χ π ) (since the diagonal entries get acted on by σ). So σ acts on the set of irreducible representations by permuting them, as σ 1 undoes the action of σ; hence it permutes the rows of the character table. To see there is a permutation of the columns as well that gives σ, suppose σ takes a primitive G th-root of unity ζ to its k-th power. Expressing each element of the character table as an integer linear combination of powers of ζ, note that χ(g k ) = σ(χ(g)). So if C g is the conjugacy class for g, then σ takes the column for C g to that of C g k, which gets sent to that of C g k2, and so on. Hence this is a permutation of the columns. Consider the character table as a square matrix M (which is invertible, as it is unitary). Let C be the permutation matrix by which σ acts on the columns, and similarly define R for the rows. That is, σ(m) = MC = RM. Then M 1 RM = C, so R and C are conjugate to each other. It suffices to show that R and C have the same cycle lengths. Their characteristic polynomials are the same as they are conjugate, so it suffices to show that the characteristic polynomial contains the information of the cycle types. By changing basis, we can assume that the permutation matrix is block-diagonal and the blocks correspond to cycles (cycle decomposition of a permutation). Then the characteristic polynomial of an n-cycle is easily seen to be T n 1 (if the matrix is written in basis e i, then ζ i ne i are an eigenbasis by Vandermonde), so if a permutation has m d d-cycles, then the r-th cyclotomic polynomial shows up r d m d times (in the characteristic polynomial). Unique factorization allows us to recover these r d m d, and Mobius inversion then allows us to recover the m d. (b) It is false, and we have the two dimensional Q 8 example whose character is real valued from above. This representation can be realized as follows: imagine Q as a multiplicative subgroup of H, and allow Q to act on H via the inverse on the right; that is, for g G and α H, we have g α = αg 1. Embedding C into H by sending 1 to i, we see this action is also C-linear if we put the C-linear action on the left; that is, for z C and g Q we have g (zα) = zαg 1 = z(αg 1 ) = z(g α). Hence we get a homomorphism Q Aut C (H). Let the character of this representation be χ. A C-basis for H will be {1, j}. Then 1 acts as the identity, so χ(1) = 2. Note 1 acts as negative of the identity, so χ( 1) = 2. We have that: i acts by 1 i and j ji 1 = ij, so χ(i) = i + i = 0, j acts by 1 j, j 1, so χ(j) = 0 + 0 = 0, k = ij acts by 1 (ij) 1 = ij, j j(ij) 1 = i, so χ(k) = 0 + 0 = 0. This can t be defined over the reals as R[G] acts exactly via multiplication by H and so this is irreducible as a real representation. But if it was defined over the reals, then there would be a real vector space V such that H = V C and so as a real representation we would have H = V V contradicting it being irreducible over R. (c) First, a general claim. Suppose V is any complex representation of a compact group G. Then V R C V V by considering characters: if we put g in Jordan normal form with basis e j for V and consider the basis {e j } {1, i} for V R C, we get two copies of each real part on the diagonal. Therefore when V is irreducible, End R[G] (V ) Hom C[G] (V R C, V ) is either 2-dimensional or 4-dimensional; the former happens when V V, and the latter happens otherwise. Now to the problem. We claim that V V 0 R C for some irreducible real representation V 0 if and only if End R[G] (V ) Mat 2 (R). If V V 0 R C, then as a R[G]-module we see that V V 0 V 0 which implies the following as R[G]-modules: End R[G] (V ) Mat 2 (End R[G] (V 0 )). 3

Since End R[G] (V ) is either two or four dimensional, we see that it must indeed be 4-dimensional and that End R[G] (V 0 ) R (using knowledge of division algebras), so End R[G] (V ) Mat 2 (R). For the converse, we use semisimplicity to see that End R[G] (V ) Mat 2 (R) implies there exists some irreducible R[G]-module V 0 with V V 0 V 0 (with End R[G] (V 0 ) R). Extending scalars to C, we see that V V V R C (V 0 R C) (V 0 R C), so that V (V 0 R C) ( V ). Suppose first that V V 0 R C. Then taking any nondegenerate symmetric bilinear form on V 0, averaging it so that it is G-invariant (and it is still nondegenerate), and then by extending scalars to C, we can produce an invariant nondegenerate symmetric bilinear form on V. Now suppose we have a nondegenerate symmetric bilinear form B : V V C. Let, be an invariant nondegenerate Hermitian form on V, and define the map j : V V by v, jw = B(v, w). Then j is complex antilinear, so j 2 End C[G] (V ) implies j 2 is multiplication by a complex scalar λ. Then v, j 2 w = B(v, jw) = B(jw, v) = jw, jv = jv, jw, so v, j 2 w = jv, jw and similarly jv, jw = j 2 v, w implies j 2 v, w = v, j 2 w. So λ = λ and that means λ is real. For any v we know that jv, jv, v, v are positive reals, so λ v, v = j 2 v, v = jv, jv = jv, jv implies λ is a positive real. By scaling j, we can now assume that j 2 = 1. So we have found j End R[G] (V ) which is not ±1 (as it is complex antilinear), but whose square is 1. This eliminates the possibility that End R[G] (V ) is a division algebra, and since it is either 2 or 4 dimensional we conclude that End R[G] (V ) Mat 2 (R). (d) The space of G-invariant bilinear forms V W C is Hom G (V W, C) = Hom G (V, W ) is at most one dimensional by Schur s lemma, and is one dimensional exactly when π σ. In the case π π there is a G-invariant bilinear form B Hom G (V V, C). By one-dimensionality, B(v, w) and B(w, v) are nonzero scalar multiples of each other, and B(v, w) = ε π B(w, v) = ε 2 πb(v, w) implies ε π {±1}. Problem 4 Let π = π be an irreducible representation of a compact group G, and let ɛ π be as above. Show that ɛ π = χ π (g 2 )dg, G where dg is the Haar measure normalized so that G dg = 1. (Hint: First show that χ π(g 2 ) = χ Sym2 (π)(g) χ 2 π(g), where Sym 2 is the symmetric square and 2 is the exterior square of π.) Let λ 1,, λ m be the eigenvalues of g, with multiplicity. Then those of g 2 will be λ 2 1,, λ 2 m, those of g on Sym 2 (π) will be λ i λ j for i j, and those of g on 2 π will be λ i λ j for i < j. As λ 2 1 + + λ 2 m = i j λ iλ j i<j λ iλ j, we conclude that χ π (g 2 ) = χ Sym 2 π(g) χ 2 π(g). So using Schur orthogonality, we conclude that G χ π(g 2 ) dg = dim C (Sym 2 (π)) G dim C ( 2 (π)) G. Identify (Sym 2 (π)) G and ( 2 (π)) G within (π π) G = Hom G (V V, C) as the space of G-invariant bilinear symmetric and alternating forms, respectively. The assumption π π implies (π π) G is one dimensional, so this number is either 1 or 1. If it is 1, then that means there is a G-invariant bilinear symmetric form, so ε π = 1. Otherwise, there is a G-invariant bilinear alternating form, so ε π = 1. In either case we have ε π = G χ π(g 2 ) dg. Problem 5 Let G be a compact group. Show that g, h Gare conjugate if and only if χ π (g) = χ π (h) 4

for every irreducible representation π of G. Deduce that every character is real valued if and only if g is conjugate to g 1 for every g G. Clearly if g, h are conjugate then all characters agree on them, as characters are class functions. Now suppose g, h are not conjugate to each other. Then the conjugacy class C h = {xhx 1 : x G} is a closed subset of G (by compactness), so there is a neighborhood U g of g which avoids C h. Set U = g C g U g, f 1 : G R 0 be a smooth bump function supported in U with value 1 in a neighborhood of C g (this is compact), and define f(y) = G f 1(xyx 1 ) dx. So f is a smooth class function with value 1 at g and value 0 at h. Write f as an infinite linear combination of matrix coefficients converging in the sup-norm; we can do this as matrix coefficients will be dense in C(G). This expansion is unique since the matrix coefficients form an orthonormal basis for L 2 (G). Let M π be the space of matrix coefficients for π, and write f = f π where f π M π. Since the conjugation action takes each M π to itself, we see that each f π is a class function. So the f π are matrix coefficients that happen to be class functions, hence they are linear combinations of characters, and must then agree on g and h. But f does not, and this is a contradiction. The character is real valued iff χ π and χ π agree, iff for all g we have χ π (g) = χ π (g) = χ π (g 1 ). So the character is real valued iff g, g 1 are conjugate to each other for all g G. Problem 6 Let G be a compact Lie group. Show that the right regular action ρ : G L 2 (G) given by (ρ(g)f)(h) = f(hg) decomposes as ρ = i=0 dim(π i)π i, where {π i } is the complete set of inequivalent irreducible representations of G. Since G is compact we know from Peter-Weyl that L 2 (G) decomposes as M π where M π is defined in the previous problem. When g acts on this, it acts on each M π separately, as if f is a matrix coefficient then so is ρ(g)f. Suppose π : G GL(V ) and pick a basis e 1,, e n of V. Then a basis for M π would be given by f ij (h) = π(h)e i, e j, and (ρ(g)f ij )(h) = π(h)π(g)e i, e j, so we see that for a fixed j, the action ρ(g) on f 1j, f 2j,, f nj is precisely the action of π. So M π decomposes as nπ = dim(π)π. Substituting this into L 2 (G) = π M π, we are done. Problem 7 Give an example of a compact operator with no non-zero eigenvalue. Any nilpotent operator over a finite dimensional vector space works, as any operator over a finite dimensional vector space is automatically compact, and nilpotency ensures that the only eigenvalues are zero. Here is an integral operator T over L 2 (S 1 ): consider K(x, y) = e 2πiy, and T : f S 1 K(, y)f(y) dy. Then T is compact as K 1. If f is a nonzero eigenvector with nonzero eigenvalue λ, we see that f = λ 1 T f implies f is constant (as T f is), so if f(x) = C then T f = C S 1 K( y) dy = C 0 = 0 implies f = λ 1 T f = λ 1 0 = 0, which is a contradiction. 5