Proquest Dissertations

Total Page:16

File Type:pdf, Size:1020Kb

Proquest Dissertations University of Alberta Fixed Point Factorization and NIM-reps for the Affine Kac-Moody Algebras, and the Non-unitary W3 Minimal Models by Elaine Myra Beltaos A thesis submitted to the Faculty of Graduate Studies and Research in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Pure Mathematics Mathematical and Statistical Sciences ©Elaine Myra Beltaos Fall 2009 Edmonton, Alberta Permission is hereby granted to the University of Alberta Libraries to reproduce single copies of this thesis and to lend or sell such copies for private, scholarly or scientific research purposes only. Where the thesis is converted to, or otherwise made available in digital form, the University of Alberta will advise potential users of the thesis of these terms. The author reserves all other publication and other rights in association with the copyright in the thesis and, except as herein before provided, neither the thesis nor any substantial portion thereof may be printed or otherwise reproduced in any material form whatsoever without the author's prior written permission. Library and Archives Bibliotheque et 1*1 Canada Archives Canada Published Heritage Direction du Branch Patrimoine de I'edition 395 Wellington Street 395, rue Wellington Ottawa ON K1A 0N4 OttawaONK1A0N4 Canada Canada Your file Votre reference ISBN: 978-0-494-55802-7 Our file Notre reference ISBN: 978-0-494-55802-7 NOTICE: AVIS: The author has granted a non­ L'auteur a accorde une licence non exclusive exclusive license allowing Library and permettant a la Bibliotheque et Archives Archives Canada to reproduce, Canada de reproduce, publier, archiver, publish, archive, preserve, conserve, sauvegarder, conserver, transmettre au public communicate to the public by par telecommunication ou par I'lnternet, preter, telecommunication or on the Internet, distribuer et vendre des theses partout dans le loan, distribute and sell theses monde, a des fins commerciales ou autres, sur worldwide, for commercial or non­ support microforme, papier, electronique et/ou commercial purposes, in microform, autres formats. paper, electronic and/or any other formats. The author retains copyright L'auteur conserve la propriete du droit d'auteur ownership and moral rights in this et des droits moraux qui protege cette these. Ni thesis. Neither the thesis nor la these ni des extraits substantiels de celle-ci substantial extracts from it may be ne doivent etre imprimes ou autrement printed or otherwise reproduced reproduits sans son autorisation. without the author's permission. In compliance with the Canadian Conformement a la loi canadienne sur la Privacy Act some supporting forms protection de la vie privee, quelques may have been removed from this formulaires secondaires ont ete enleves de thesis. cette these. While these forms may be included Bien que ces formulaires aient inclus dans in the document page count, their la pagination, il n'y aura aucun contenu removal does not represent any loss manquant. of content from the thesis. 1+1 Canada Examining Committee Terry Gannon, Mathematical and Statistical Sciences Gerald Cliff, Mathematical and Statistical Sciences Nicolas Guay, Mathematical and Statistical Sciences Marc de Montigny, Faculte Saint-Jean Mark Walton, Physics and Astronomy, University of Lethbridge I dedicate this thesis to my siblings, Andrew, Angela and Terry, and my parents, Lillian and Spyros. ABSTRACT In this thesis, we find the modular invariants for the non-unitary W3 minimal models (which is the first nontrivial non-unitary modular invariant classification), and the fixed point factorizations and NIM-reps for the B, C and D afiine Kac- Moody algebras (the only other known case is for the yl-series, [26] and [15] respec­ tively). Using the fixed point factorizations, we are able to find remarkably simple expressions for the corresponding NIM-reps. Keywords: affine Kac-Moody algebras, modular data, NIM-rep, modular invari­ ants ACKNOWLEDGEMENTS I would like to first of all thank my supervisor Dr. Terry Gannon for his guidance and support (both mathematical and financial) throughout my research and the writing of this thesis. I wish to thank Dr. Gannon also more generally for his ongoing support during my graduate studies, and for generously sharing his mathematical and professional wisdom, for which I am very grateful. I am very grateful to my family for their support, which has come in many forms over the years and during the writing of this thesis, and especially thank you to my mother for her many great suggestions and strategic wisdom. Thank you to my brother Andrew and David Churchill for valuable help with LaTex, and to Hongtao Yang, the creator of the template which I used to write this thesis. I would also like to thank the Department of Mathematical and Statistical Sci­ ences at the University of Alberta for financial support during my graduate studies. Table of Contents List of Tables List of Figures List of Symbols 1 1 Introduction 3 2 Background 6 2.1 Some Lie theory 6 2.1.1 Lie algebras 6 2.1.2 Lie algebra representations 7 2.1.3 Lie algebra characters 8 2.1.4 Affine Lie algebras 9 2.2 Conformal field theory 10 2.2.1 Quantum field theories 10 2.2.2 Modular data 11 2.2.3 Properties of modular data and the Galois symmetry 12 2.2.4 The modular invariant partition function 13 2.2.5 The S-matrix and Lie algebra characters 14 2.2.6 The fusion ring and simple-currents 15 2.3 Data for the algebras 17 2.3.1 The data 17 2.3.2 Proofs of Lemmas 2.1, 2.2 and 2.3 23 3 The Ws modular invariant classification 35 3.1 Modular invariant classifications 36 3.2 The modular invariants of {A2 © A2)W 37 1] 3.2.1 The A2 classification 37 {1) 3.2.2 The (A2 © A2) modular invariants 39 3.3 The modular invariants of W$ 41 3.4 The (A2 © A2)^ classification 45 3.4.1 The permutation invariants 46 3.4.2 The vacuum couplings 47 3.4.3 The simple-current extensions 48 3.4.4 The classification when J has no fixed points 50 3.4.5 The classification when J has a fixed point 51 3.4.6 The exceptional invariants 52 3.4.7 q = 8, 3 \ p, and HR = 1IL = {pp, pp") 52 3.4.8 q = 8,p=3l, and KR = JR(pp)UjR{pp") and KL = JL(pp)U MPP") 54 3.4.9 q = 8, 3 \ p, and 11= {{p,p),(p,p")} 55 3.4.10 q = 8, 3|p, and ft = {(JV,p), (JV,//') :i = 0,1,2} 57 3.4.11 The exceptionals at (12, q) and (24, q) 58 4 Fixed point factorization for the affine Kac-Moody algebras 59 4.1 The problem 59 4.2 The Ar ' fixed point factorization 60 4.2.1 The special case of the fundamental weights 61 4.3 The Cr fixed point factorization 62 4.3.1 The r even case 62 4.3.2 The r odd case 64 4.3.3 The special case of the fundamental weights 66 4.4 The Br ' fixed point factorization 69 4.5 The Dr ' fixed point factorization 72 4.5.1 The simple-current Jv 72 4.5.2 The simple-current Js when r is even 74 4.5.3 The simple-current Js when r is odd 81 4.5.4 The simple-current JVJS, r even 84 4.5.5 The full simple-current group (Jv, Js) when r is even 85 5 Applications of fixed point factorization to NIM-reps 86 5.1 TheNIM-rep 86 ( 1] 5.2 The NIM-reps for A r 88 1] 5.3 The NIM-reps for Cr 89 5.3.1 The r even case 89 5.3.2 The r odd case 93 5.3.3 Examples of B and £ 93 5.4 The NIM-reps for B^ 94 5.4.1 The case k odd 94 5.4.2 The case k even 95 5.5 The NIM-reps for D^ 95 5.5.1 The simple-current Jv 95 5.5.2 The simple-current Js when r is even 95 5.5.3 The simple-current Js when r is odd 97 5.5.4 The full simple-current group {JV,JS) when r is even 98 5.6 Using the Pieri rules: an example 99 6 Concluding remarks 102 6.1 Summary and discussion 102 6.1.1 The non-unitary W3 minimal models 102 6.1.2 Fixed point factorization 103 6.1.3 NIM-reps 105 6.2 Future work 106 6.2.1 Work related to fixed point factorization 106 6.2.2 Work related to the NIM-rep formulas 107 Bibliography 109 List of Tables 2.1 Simple currents and Qj, rj for the classical affine algebras 16 6.1 Fixed point factorization algebras for the classical affine algebras . 106 List of Figures 2.1 The Coxeter-Dynkin diagrams for the affine Kac-Moody algebras 9 List of Symbols Q Lie algebra 6 Xr simple finite-dimensional Lie algebra of rank r 7 P+(Q) dominant integral weights of g 7 L(X) highest weight module 7 Vp weight space 8 O weights of a representation 8 ch\ character of L{\) 8 p Weyl vector 8 R+ set of positive roots 8 K central element of g'1^ 9 Q^ affinization of g 9 Xr affinization of simple rank r algebra Xr 9 P\ set of level k highest weights 10 (R)CFT (rational) conformal field theory 10 $ set of primary fields 11 S, T S-matrix, T-matrix 12 t complex conjugate transpose 12 C charge-conjugation 12 * complex conjugation 12 ^ob> ^x,ti fusion coefficients 12 a Galois automorphism 13 ea(a), eCT(A) parity of a, A 13 Z(T) modular invariant partition function 13 M modular invariant 14 A Xr highest weight 14 Aj fundamental weight (usually affine) 14 Aj fundamental weight for Xr 14 XxilA characters at elements of finite order 14 mx(f3) multiplicity of (3 in L{\) 14 W(P) Weyl orbit of /? 14 fi+(A) dominant weights of A 15 Fus fusion ring 15 Ch character ring 15 j, J simple-current 15 Qj, rj rational numbers obeying simple-current symmetries 15 1 M\J] simple-current matrix 16 <5z(x) 1 if x e Z, 0 else 16 X[i], A+ [i] orthogonal coordinates (non-shifted and shifted) 17 t(X) n-ality (triality if n = 3) of A 17 (ai,..., ar) r-tuple with respect to orthonormal basis of W 23 0 the empty set 29 x =m y x = y (mod m) 31 n,p,q height of a representation 37 P++ p-shifted height n highest weights 37 0(A) simple-current orbit of A 38 o minimal primary 41 [Xfi] W% primary 41 m\n m does
Recommended publications
  • A Localization Argument for Characters of Reductive Lie Groups: an Introduction and Examples Matvei Libine
    This is page 375 Printer: Opaque this A localization argument for characters of reductive Lie groups: an introduction and examples Matvei Libine In Honor of Jacques Carmona ABSTRACT In this article I describe my recent geometric localization argument dealing with actions of noncompact groups which provides a geometric bridge between two entirely different character formulas for reductive Lie groups and answers the question posed in [Sch]. A corresponding problem in the compact group setting was solved by N. Berline, E. Getzler and M. Vergne in [BGV] by an application of the theory of equivariant forms and, particularly, the fixed point integral localization formula. This localization argument seems to be the first successful attempt in the direction of build- ing a similar theory for integrals of differential forms, equivariant with respect to actions of noncompact groups. I will explain how the argument works in the SL(2, R) case, where the key ideas are not obstructed by technical details and where it becomes clear how it extends to the general case. The general argument appears in [L]. Ihavemade every effort to present this article so that it is widely accessible. Also, although characteristic cycles of sheaves is mentioned, I do not assume that the reader is familiar with this notion. 1 Introduction For motivation, let us start with the case of a compact group. Thus we consider a connected compact group K and a maximal torus T ⊂ K . Let kR and tR denote the Lie algebras of K and T respectively, and k, t be their complexified Lie algebras. Let π be a finite-dimensional representation of K , that is π is a group homomorphism K → Aut(V ).
    [Show full text]
  • NOTES on the WEYL CHARACTER FORMULA the Aim of These Notes
    NOTES ON THE WEYL CHARACTER FORMULA The aim of these notes is to give a self-contained algebraic proof of the Weyl Character Formula. The necessary background results on modules for sl2(C) and complex semisimple Lie algebras are outlined in the first two sections. Some technical details are left to the exercises at the end; solutions are provided when the exercise is needed for the proof. 1. Representations of sl2(C) Define ! ! ! 1 0 0 1 0 0 h = ; e = ; f = 0 −1 0 0 1 0 2 and note that hh; e; fi = sl2(C). Let u; v be the canonical basis of E = C . Then each Symd E is irreducible with ud spanning the highest-weight space d of weight d and, up to isomorphism, Sym E is the unique irreducible sl2(C)- module with highest weight d. (See Exercises 1.1 and 1.2.) The diagram below shows the actions of h, e and f on the canonical basis of Symd E: loops show the action of h, arrows to the right show the action of e, arrow to the left show the action of f. d−2c−2 d−2c d−2c+2 d−c+1 d−c d−c−1 i • j * • j * • ) c−1 ud−c−1vc+1 c ud−cvc c+1 ud−c+1vc−1 In particular (a) the eigenvalues of h on Symd E are −d; −d + 2; : : : ; d − 2; d and each h-eigenspace is 1-dimensional, (b) if w 2 Symd E and h · w = (d − 2c)w then f · e · w = c(d − c + 1)w.
    [Show full text]
  • Title: Algebraic Group Representations, and Related Topics a Lecture by Len Scott, Mcconnell/Bernard Professor of Mathemtics, the University of Virginia
    Title: Algebraic group representations, and related topics a lecture by Len Scott, McConnell/Bernard Professor of Mathemtics, The University of Virginia. Abstract: This lecture will survey the theory of algebraic group representations in positive characteristic, with some attention to its historical development, and its relationship to the theory of finite group representations. Other topics of a Lie-theoretic nature will also be discussed in this context, including at least brief mention of characteristic 0 infinite dimensional Lie algebra representations in both the classical and affine cases, quantum groups, perverse sheaves, and rings of differential operators. Much of the focus will be on irreducible representations, but some attention will be given to other classes of indecomposable representations, and there will be some discussion of homological issues, as time permits. CHAPTER VI Linear Algebraic Groups in the 20th Century The interest in linear algebraic groups was revived in the 1940s by C. Chevalley and E. Kolchin. The most salient features of their contributions are outlined in Chapter VII and VIII. Even though they are put there to suit the broader context, I shall as a rule refer to those chapters, rather than repeat their contents. Some of it will be recalled, however, mainly to round out a narrative which will also take into account, more than there, the work of other authors. §1. Linear algebraic groups in characteristic zero. Replicas 1.1. As we saw in Chapter V, §4, Ludwig Maurer thoroughly analyzed the properties of the Lie algebra of a complex linear algebraic group. This was Cheval­ ey's starting point.
    [Show full text]
  • A Recursive Formula for Characters of Simple Lie Algebras
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector JOURNAL OF ALGEBRA 137, 126-144 (1991) A Recursive Formula for Characters of Simple Lie Algebras STEVEN N. KASS* Centre de recherches mathkmatiques, UniversitP de MontrPal C. P. 6128, &cc. “A”, MontrPal, Qutbec, Canada H3C 357 Communicated by Robert Steinberg Received July 20, 1988; accepted July 18, 1989 In 1964, Antoine and Speiser published succinct and elegant formulae for the characters of the irreducible highest weight modules for the Lie algebras A, and B,. (The result for A, may have been known as early as 1957.) These can be derived from a recursive formula for characters valid for all simple complex Kac-Moody Lie algebras for which the Weyl-Kac character formula holds. 0 1991 Academic Press. Inc. 1. INTRODUCTION To avoid the encumbrance of technicalities, we present the results first for simple finite-dimensional Lie algebras over C. We use the following notation, generally following Humphreys [H]. Let L be a finite-dimensional complex simple Lie algebra of rank 1. We denote by H a Cartan subalgebra of L, by ai (1 Q i < I) a choice of simple roots, by Q the integral lattice they generate, and by R, R+, and R- the root system, positive roots, and negative roots with respect to H and the ai, respectively. Let A be the weight lattice for L, and li (1~ i,< I) the fundamental weights corresponding to the choice of simple roots. The set of dominant weights will be denoted A +.
    [Show full text]
  • Notes for Lie Groups & Representations Instructor: Andrei Okounkov
    Notes for Lie Groups & Representations Instructor: Andrei Okounkov Henry Liu May 2, 2017 Abstract These are my live-texed notes for the Spring 2017 offering of MATH GR6344 Lie Groups & Repre- sentations. There are known omissions. Let me know when you find errors or typos. I'm sure there are plenty. 1 Kac{Moody Lie Algebras 1 1.1 Root systems and Weyl groups . 1 1.2 Reflection groups . 2 1.3 Regular polytopes and Coxeter groups . 4 1.4 Kac{Moody Lie algebras . 5 1.5 Examples of Kac{Moody algebras . 7 1.6 Category O . 8 1.7 Gabber{Kac theorem . 10 1.8 Weyl{Kac character formula . 11 1.9 Weyl character formula . 12 1.10 Affine Kac{Moody Lie algebras . 15 2 Equivariant K-theory 18 2.1 Equivariant sheaves . 18 2.2 Equivariant K-theory . 20 3 Geometric representation theory 22 3.1 Borel{Weil . 22 3.2 Localization . 23 3.3 Borel{Weil{Bott . 25 3.4 Hecke algebras . 26 3.5 Convolution . 27 3.6 Difference operators . 31 3.7 Equivariant K-theory of Steinberg variety . 32 3.8 Quantum groups and knots . 33 a Chapter 1 Kac{Moody Lie Algebras Given a semisimple Lie algebra, we can construct an associated root system, and from the root system we can construct a discrete group W generated by reflections (called the Weyl group). 1.1 Root systems and Weyl groups Let g be a semisimple Lie algebra, and h ⊂ g a Cartan subalgebra. Recall that g has a non-degenerate bilinear form (·; ·) which is preserved by the adjoint action, i.e.
    [Show full text]
  • Lie Algebras by Shlomo Sternberg
    Lie algebras Shlomo Sternberg April 23, 2004 2 Contents 1 The Campbell Baker Hausdorff Formula 7 1.1 The problem. 7 1.2 The geometric version of the CBH formula. 8 1.3 The Maurer-Cartan equations. 11 1.4 Proof of CBH from Maurer-Cartan. 14 1.5 The differential of the exponential and its inverse. 15 1.6 The averaging method. 16 1.7 The Euler MacLaurin Formula. 18 1.8 The universal enveloping algebra. 19 1.8.1 Tensor product of vector spaces. 20 1.8.2 The tensor product of two algebras. 21 1.8.3 The tensor algebra of a vector space. 21 1.8.4 Construction of the universal enveloping algebra. 22 1.8.5 Extension of a Lie algebra homomorphism to its universal enveloping algebra. 22 1.8.6 Universal enveloping algebra of a direct sum. 22 1.8.7 Bialgebra structure. 23 1.9 The Poincar´e-Birkhoff-Witt Theorem. 24 1.10 Primitives. 28 1.11 Free Lie algebras . 29 1.11.1 Magmas and free magmas on a set . 29 1.11.2 The Free Lie Algebra LX ................... 30 1.11.3 The free associative algebra Ass(X). 31 1.12 Algebraic proof of CBH and explicit formulas. 32 1.12.1 Abstract version of CBH and its algebraic proof. 32 1.12.2 Explicit formula for CBH. 32 2 sl(2) and its Representations. 35 2.1 Low dimensional Lie algebras. 35 2.2 sl(2) and its irreducible representations. 36 2.3 The Casimir element. 39 2.4 sl(2) is simple.
    [Show full text]
  • Weyl Character Formula for U(N)
    THE WEYL CHARACTER FORMULA–I PRAMATHANATH SASTRY 1. Introduction This is the first of two lectures on the representations of compact Lie groups. In this lecture we concentrate on the group U(n), and classify all its irreducible representations. The methods give the paradigm and set the template for study- ing representations of a large class of compact Lie groups—a class which includes semi-simple compact groups. The climax is the character formula of Weyl, which classifies all irreducible representations for this class, up to unitary equivalence. The typing was done in a hurry (last night and this morning, to be precise), and there may well be more serious errors than mere typos. Typos of course abound. 2. Fourier Analysis on abelian groups It is well-known, and easy to prove, that a compact ableian Lie group 1 is nec- essarily a torus Tn = S1 × . × S1 (n factors). A character on T = Tn is a Lie T C∗ 2 m1 mn group map χ : → . The maps χm1,... ,mn ((t1,...,tn) 7→ t1 ...tn ) lists n all characters on T as (m1,...,mn) varies over Z . This is a fairly elementary result—indeed, the image of a character χ must be a compact connected subgroup of C∗, forcing χ to take values in S1 ⊂ C∗. From there to seeing χ must equal a χm1,... ,mn is easy (try the case n = 1 !). T has an invariant Borel measure dt = dt1 ... dtn (the product of the “arc length” measures on the various S1 factors), the so called Haar measure on T 3.
    [Show full text]
  • Branching Rules of Classical Lie Groups in Two Ways
    Branching Rules of Classical Lie Groups in Two Ways by Lingxiao Li Submitted to the Department of Mathematics in partial fulfillment of the requirements for the degree of Bachelor of Science in Mathematics with Honors at Stanford University June 2018 Thesis advisor: Daniel Bump Contents 1 Introduction 2 2 Branching Rule of Successive Unitary Groups 4 2.1 Weyl Character Formula . .4 2.2 Maximal Torus and Root System of U(n) .....................5 2.3 Statement of U(n) # U(n − 1) Branching Rule . .6 2.4 Schur Polynomials and Pieri’s Formula . .7 2.5 Proof of U(n) # U(n − 1) Branching Rule . .9 3 Branching Rule of Successive Orthogonal Groups 13 3.1 Maximal Tori and Root Systems of SO(2n + 1) and SO(2n) .......... 13 3.2 Branching Rule for SO(2n + 1) # SO(2n) ..................... 14 3.3 Branching Rule for SO(2n) # SO(2n − 1) ..................... 17 4 Branching Rules via Duality 21 4.1 Algebraic Setup . 21 4.2 Representations of Algebras . 22 4.3 Reductivity of Classical Groups . 23 4.4 General Duality Theorem . 25 4.5 Schur-Weyl Duality . 27 4.6 Weyl Algebra Duality . 28 4.7 GL(n; C)-GL(k; C) Duality . 31 4.8 O(n; C)-sp(k; C) Duality . 33 4.9 Seesaw Reciprocity . 36 4.10 Littlewood-Richardson Coefficients . 37 4.11 Stable Branching Rule for O(n; C) × O(n; C) # O(n; C) ............. 39 1 Acknowledgements I would like to express my great gratitude to my honor thesis advisor Daniel Bump for sug- gesting me the interesting problem of branching rules, for unreservedly and patiently sharing his knowledge with me on Lie theory, and for giving me valuable instruction and support in the process of writing this thesis over the recent year.
    [Show full text]
  • Lie Algebras
    Lie algebras Course Notes Alberto Elduque Departamento de Matem´aticas Universidad de Zaragoza 50009 Zaragoza, Spain ©2005-2021 Alberto Elduque These notes are intended to provide an introduction to the basic theory of finite dimensional Lie algebras over an algebraically closed field of characteristic 0 and their representations. They are aimed at beginning graduate students in either Mathematics or Physics. The basic references that have been used in preparing the notes are the books in the following list. By no means these notes should be considered as an alternative to the reading of these books. N. Jacobson: Lie algebras, Dover, New York 1979. Republication of the 1962 original (Interscience, New York). J.E. Humphreys: Introduction to Lie algebras and Representation Theory, GTM 9, Springer-Verlag, New York 1972. W. Fulton and J. Harris: Representation Theory. A First Course, GTM 129, Springer-Verlag, New York 1991. W.A. De Graaf: Lie algebras: Theory and Algorithms, North Holland Mathemat- ical Library, Elsevier, Amsterdan 2000. Contents 1 A short introduction to Lie groups and Lie algebras 1 § 1. One-parameter groups and the exponential map . 2 § 2. Matrix groups . 5 § 3. The Lie algebra of a matrix group . 7 2 Lie algebras 17 § 1. Theorems of Engel and Lie . 17 § 2. Semisimple Lie algebras . 22 § 3. Representations of sl2(k)........................... 29 § 4. Cartan subalgebras . 31 § 5. Root space decomposition . 34 § 6. Classification of root systems . 38 § 7. Classification of the semisimple Lie algebras . 51 § 8. Exceptional Lie algebras . 55 3 Representations of semisimple Lie algebras 61 § 1. Preliminaries . 61 § 2. Properties of weights and the Weyl group .
    [Show full text]
  • Theorem 335 If G Is a Connected Quasi-Simple Compact Lie Group, There Is
    Theorem 335 If G is a connected quasi-simple compact Lie group, there is an element q such that an irreducible representation is real or quaternionic depend- ing on whether q acts as +1 or −1. Proof For the group SU2 we can check this by direct calculation: the irre- ducible representations of even dimension have an alternating form, and those of odd dimension have an even form. So the element q is the non-trivial element of the center. The idea of the proof for general compact groups is to reduce to this case by finding a homomorphism from SU2 to G such that the restriction of any irreducible representation V of G to this SU2 contains some irreducible repre- sentation W with multiplicity exactly 1. Then any alternating or symmetric form on V must restrict to an alternating or symmetric form on W , so we can tell which by examining the action on W of the image q ∈ G of the nontrivial element of the center of the SU2 subgroup. We will find a suitable SU2 subgroup by constructing a basis E, F , H for its complexified Lie algebra. We take E to be the sum Pα Eα where the sum is over the simple roots and Eα is some nonzero element of the simple root space of α. We take H to be the element of the Cartan subalgebra that has inner product 2 with every simple root, which is possible as the simple roots are linearly independent. Finally we choose Fα in the root space of −α so that P[Eα, Fα] = H.
    [Show full text]
  • The Weyl Character Formula Math G4344, Spring 2012
    The Weyl Character Formula Math G4344, Spring 2012 1 Characters We have seen that irreducible representations of a compact Lie group G can be constructed starting from a highest weight space and applying negative roots to a highest weight vector. One crucial thing that this construction does not easily tell us is what the character of this irreducible representation will be. The character would tell us not just which weights occur in the representation, but with what multiplicities they occur (this multiplicity is one for the highest weight, but in general can be larger). Knowing the characters of the irreducibles, we can use this to compute the decomposition of an arbitrary representation into irreducibles. The character of a representation (π; V ) is the complex-valued, conjugation- invariant function on G given by χV (g) = T r(π(g)) The representation ring R(G) of a compact Lie group behaves much the the same as in the finite group case, with the sum over group elements replaced by an integral in the formula for the inner product on R(G) Z < [V ]; [W ] >= χV (g)χW (g)dg G where dg is the invariant Haar measure giving G volume 1. As an inner product space R(G) has a distinguished orthonormal basis given by the characters χVi (g) of the irreducible representations. For an arbitrary representation V , once we know its character χV we can compute the multiplicities ni of the irreducibles in the decomposition M V = niVi i2G^ as Z ni = χVi (g)χV (g)dg Knowing the character of V is equivalent to knowing the weights γi in V , together with their multiplicities ni, since if M V = niCγi i then H X γi(H) T rV (e ) = nie i 1 2 The Weyl Integral Formula We'll give a detailed outline of Weyl's proof of the character formula for a highest-weight irreducible.
    [Show full text]
  • Eigenvalues, Eigenvectors, and Random-Matrix Theory
    Graduate School of Natural Sciences Eigenvalues, eigenvectors, and random-matrix theory Master Thesis Stefan Boere Mathematical Sciences & Theoretical Physics Supervisors: Prof. Dr. C. Morais Smith Institute for Theoretical Physics Dr. J.W. Van de Leur Mathematical Institute W. Vleeshouwers October 22, 2020 i Abstract We study methods for calculating eigenvector statistics of random matrix en- sembles, and apply one of these methods to calculate eigenvector components of Toeplitz ± Hankel matrices. Random matrix theory is a broad field with applica- tions in heavy nuclei scattering, disordered metals and quantum billiards. We study eigenvalue distribution functions of random matrix ensembles, such as the n-point correlation function and level spacings. For critical systems, with eigenvalue statis- tics between Poisson and Wigner-Dyson, the eigenvectors can have multifractal properties. We explore methods for calculating eigenvector component expectation values. We apply one of these methods, referred to as the eigenvector-eigenvalue identity, to show that the absolute values of eigenvector components of certain Toeplitz and Toeplitz±Hankel matrices are equal in the limit of large system sizes. CONTENTS ii Contents 1 Introduction 1 2 Random matrix ensembles 4 2.1 Symmetries and the Gaussian ensembles . .4 2.1.1 Gaussian Orthogonal Ensemble (GOE) . .5 2.1.2 Gaussian Symplectic Ensemble (GSE) . .6 2.1.3 Gaussian Unitary Ensemble (GUE) . .7 2.2 Dyson's three-fold way . .8 2.2.1 Real and quaternionic structures . 13 2.3 The Circular ensembles . 15 2.3.1 Weyl integration . 17 2.3.2 Associated symmetric spaces . 19 2.4 The Gaussian ensembles . 20 2.4.1 Eigenvalue distribution .
    [Show full text]