0. Many Years After I Produced This Document, Deligne Gave It His Blessing, So It Is No Longer an "Unauthorized" Translation
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Arxiv:1302.5859V2 [Math.RT] 13 May 2015 Upre Ynfflosi DMS-0902661
STABILITY PATTERNS IN REPRESENTATION THEORY STEVEN V SAM AND ANDREW SNOWDEN Abstract. We develop a comprehensive theory of the stable representation categories of several sequences of groups, including the classical and symmetric groups, and their relation to the unstable categories. An important component of this theory is an array of equivalences between the stable representation category and various other categories, each of which has its own flavor (representation theoretic, combinatorial, commutative algebraic, or categorical) and offers a distinct perspective on the stable category. We use this theory to produce a host of specific results, e.g., the construction of injective resolutions of simple objects, duality between the orthogonal and symplectic theories, a canonical derived auto-equivalence of the general linear theory, etc. Contents 1. Introduction 2 1.1. Overview 2 1.2. Descriptions of stable representation theory 4 1.3. Additional results, applications, and remarks 7 1.4. Relation to other work 10 1.5. Future directions 11 1.6. Organization 13 1.7. Notation and conventions 13 2. Preliminaries 14 2.1. Representations of categories 14 2.2. Polynomial representations of GL(∞) and category V 19 2.3. Twisted commutative algebras 22 2.4. Semi-group tca’s and diagram categories 24 2.5. Profinite vector spaces 25 arXiv:1302.5859v2 [math.RT] 13 May 2015 3. The general linear group 25 3.1. Representations of GL(∞) 25 3.2. The walled Brauer algebra and category 29 3.3. Modules over Sym(Ch1, 1i) 33 3.4. Rational Schur functors, universal property and specialization 36 4. The orthogonal and symplectic groups 39 4.1. -
An Introduction to Operad Theory
AN INTRODUCTION TO OPERAD THEORY SAIMA SAMCHUCK-SCHNARCH Abstract. We give an introduction to category theory and operad theory aimed at the undergraduate level. We first explore operads in the category of sets, and then generalize to other familiar categories. Finally, we develop tools to construct operads via generators and relations, and provide several examples of operads in various categories. Throughout, we highlight the ways in which operads can be seen to encode the properties of algebraic structures across different categories. Contents 1. Introduction1 2. Preliminary Definitions2 2.1. Algebraic Structures2 2.2. Category Theory4 3. Operads in the Category of Sets 12 3.1. Basic Definitions 13 3.2. Tree Diagram Visualizations 14 3.3. Morphisms and Algebras over Operads of Sets 17 4. General Operads 22 4.1. Basic Definitions 22 4.2. Morphisms and Algebras over General Operads 27 5. Operads via Generators and Relations 33 5.1. Quotient Operads and Free Operads 33 5.2. More Examples of Operads 38 5.3. Coloured Operads 43 References 44 1. Introduction Sets equipped with operations are ubiquitous in mathematics, and many familiar operati- ons share key properties. For instance, the addition of real numbers, composition of functions, and concatenation of strings are all associative operations with an identity element. In other words, all three are examples of monoids. Rather than working with particular examples of sets and operations directly, it is often more convenient to abstract out their common pro- perties and work with algebraic structures instead. For instance, one can prove that in any monoid, arbitrarily long products x1x2 ··· xn have an unambiguous value, and thus brackets 2010 Mathematics Subject Classification. -
SCHUR-WEYL DUALITY Contents Introduction 1 1. Representation
SCHUR-WEYL DUALITY JAMES STEVENS Contents Introduction 1 1. Representation Theory of Finite Groups 2 1.1. Preliminaries 2 1.2. Group Algebra 4 1.3. Character Theory 5 2. Irreducible Representations of the Symmetric Group 8 2.1. Specht Modules 8 2.2. Dimension Formulas 11 2.3. The RSK-Correspondence 12 3. Schur-Weyl Duality 13 3.1. Representations of Lie Groups and Lie Algebras 13 3.2. Schur-Weyl Duality for GL(V ) 15 3.3. Schur Functors and Algebraic Representations 16 3.4. Other Cases of Schur-Weyl Duality 17 Appendix A. Semisimple Algebras and Double Centralizer Theorem 19 Acknowledgments 20 References 21 Introduction. In this paper, we build up to one of the remarkable results in representation theory called Schur-Weyl Duality. It connects the irreducible rep- resentations of the symmetric group to irreducible algebraic representations of the general linear group of a complex vector space. We do so in three sections: (1) In Section 1, we develop some of the general theory of representations of finite groups. In particular, we have a subsection on character theory. We will see that the simple notion of a character has tremendous consequences that would be very difficult to show otherwise. Also, we introduce the group algebra which will be vital in Section 2. (2) In Section 2, we narrow our focus down to irreducible representations of the symmetric group. We will show that the irreducible representations of Sn up to isomorphism are in bijection with partitions of n via a construc- tion through certain elements of the group algebra. -
The Partition Algebra and the Kronecker Product (Extended Abstract)
FPSAC 2013, Paris, France DMTCS proc. (subm.), by the authors, 1–12 The partition algebra and the Kronecker product (Extended abstract) C. Bowman1yand M. De Visscher2 and R. Orellana3z 1Institut de Mathematiques´ de Jussieu, 175 rue du chevaleret, 75013, Paris 2Centre for Mathematical Science, City University London, Northampton Square, London, EC1V 0HB, England. 3 Department of Mathematics, Dartmouth College, 6188 Kemeny Hall, Hanover, NH 03755, USA Abstract. We propose a new approach to study the Kronecker coefficients by using the Schur–Weyl duality between the symmetric group and the partition algebra. Resum´ e.´ Nous proposons une nouvelle approche pour l’etude´ des coefficients´ de Kronecker via la dualite´ entre le groupe symetrique´ et l’algebre` des partitions. Keywords: Kronecker coefficients, tensor product, partition algebra, representations of the symmetric group 1 Introduction A fundamental problem in the representation theory of the symmetric group is to describe the coeffi- cients in the decomposition of the tensor product of two Specht modules. These coefficients are known in the literature as the Kronecker coefficients. Finding a formula or combinatorial interpretation for these coefficients has been described by Richard Stanley as ‘one of the main problems in the combinatorial rep- resentation theory of the symmetric group’. This question has received the attention of Littlewood [Lit58], James [JK81, Chapter 2.9], Lascoux [Las80], Thibon [Thi91], Garsia and Remmel [GR85], Kleshchev and Bessenrodt [BK99] amongst others and yet a combinatorial solution has remained beyond reach for over a hundred years. Murnaghan discovered an amazing limiting phenomenon satisfied by the Kronecker coefficients; as we increase the length of the first row of the indexing partitions the sequence of Kronecker coefficients obtained stabilises. -
Equivariant De Rham Cohomology and Gauged Field Theories
Equivariant de Rham cohomology and gauged field theories August 15, 2013 Contents 1 Introduction 2 1.1 Differential forms and de Rham cohomology . .2 1.2 A commercial for supermanifolds . .3 1.3 Topological field theories . .5 2 Super vector spaces, super algebras and super Lie algebras 11 2.1 Super algebras . 12 2.2 Super Lie algebra . 14 3 A categorical Digression 15 3.1 Monoidal categories . 15 3.2 Symmetric monoidal categories . 17 4 Supermanifolds 19 4.1 Definition and examples of supermanifolds . 19 4.2 Super Lie groups and their Lie algebras . 23 4.3 Determining maps from a supermanifold to Rpjq ................ 26 5 Mapping supermanifolds and the functor of points formalism 31 5.1 Internal hom objects . 32 5.2 The functor of points formalism . 34 5.3 The supermanifold of endomorphisms of R0j1 .................. 36 5.4 Vector bundles on supermanifolds . 37 5.5 The supermanifold of maps R0j1 ! X ...................... 41 5.6 The algebra of functions on a generalized supermanifold . 43 1 1 INTRODUCTION 2 6 Gauged field theories and equivariant de Rham cohomology 47 6.1 Equivariant cohomology . 47 6.2 Differential forms on G-manifolds. 49 6.3 The Weil algebra . 53 6.4 A geometric interpretation of the Weil algebra . 57 1 Introduction 1.1 Differential forms and de Rham cohomology Let X be a smooth manifold of dimension n. We recall that Ωk(X) := C1(X; ΛkT ∗X) is the vector space of differential k-forms on X. What is the available structure on differential forms? 1. There is the wedge product Ωk(M) ⊗ Ω`(M) −!^ Ωk+`(X) induced by a vector bundle homomorphism ΛkT ∗X ⊗ Λ`T ∗X −! Λk+`T ∗X ∗ Ln k This gives Ω (X) := k=0 Ω (X) the structure of a Z-graded algebra. -
Dissertation Superrings and Supergroups
DISSERTATION Titel der Dissertation Superrings and Supergroups Verfasser Dr. Dennis Bouke Westra zur Erlangung des akademischen Grades Doktor der Naturwissenschaften (Dr.rer.nat.) Wien, Oktober 2009 Studienkennzahl lt. Studienblatt: A 091 405 Studienrichtung lt. Studienblatt: Mathematik Betreuer: Univ.-Prof. Dr. Peter Michor Contents 1 Introduction 1 1.1 Anexample....................................... .. 1 1.2 Motivation ...................................... ... 1 1.3 Plan............................................ 2 1.4 Notationandconventions . ....... 2 2 Super vector spaces 5 2.1 Supervectorspaces............................... ...... 5 2.2 Liesuperalgebras................................ ...... 7 3 Basics of superrings and supermodules 11 3.1 Superringsandsuperalgebras . ......... 11 3.2 Supermodules.................................... .... 15 3.3 Noetheriansuperrings . ....... 17 3.4 Artiniansuperrings. .. .. .. .. .. .. .. .. .. .. .. .. .. ....... 20 3.5 Splitsuperrings................................. ...... 22 3.6 Grassmannenvelopes.. .. .. .. .. .. .. .. .. .. .. .. .. ...... 23 3.7 Freemodulesandsupermatrices . ........ 24 4 Primes and primaries 29 4.1 Propertiesofprimeideals . ........ 29 4.2 Primary ideals and primary decompositions . ............ 35 4.3 Primarydecompositions . ....... 36 5 Localization and completion 39 5.1 Localization.................................... ..... 39 5.2 Application to Artinian superrings . ........... 45 5.3 Geometricsuperalgebras. ........ 46 5.4 Superschemes................................... -
Simple Weight Q2(ℂ)-Supermodules
U.U.D.M. Project Report 2009:12 Simple weight q2( )-supermodules Ekaterina Orekhova ℂ Examensarbete i matematik, 30 hp Handledare och examinator: Volodymyr Mazorchuk Juni 2009 Department of Mathematics Uppsala University Simple weight q2(C)-supermodules Ekaterina Orekhova June 6, 2009 1 Abstract The first part of this paper gives the definition and basic properties of the queer Lie superalgebra q2(C). This is followed by a complete classification of simple h-supermodules, which leads to a classification of all simple high- est and lowest weight q2(C)-supermodules. The paper also describes the structure of all Verma supermodules for q2(C) and gives a classification of finite-dimensional q2(C)-supermodules. 2 Contents 1 Introduction 4 1.1 General definitions . 4 1.2 The queer Lie superalgebra q2(C)................ 5 2 Classification of simple h-supermodules 6 3 Properties of weight q-supermodules 11 4 Universal enveloping algebra U(q) 13 5 Simple highest weight q-supermodules 15 5.1 Definition and properties of Verma supermodules . 15 5.2 Structure of typical Verma supermodules . 27 5.3 Structure of atypical Verma supermodules . 28 6 Finite-Dimensional simple weight q-supermodules 31 7 Simple lowest weight q-supermodules 31 3 1 Introduction Significant study of the characters and blocks of the category O of the queer Lie superalgebra qn(C) has been done by Brundan [Br], Frisk [Fr], Penkov [Pe], Penkov and Serganova [PS1], and Sergeev [Se1]. This paper focuses on the case n = 2 and gives explicit formulas, diagrams, and classification results for simple lowest and highest weight q2(C) supermodules. -
Bases of Infinite-Dimensional Representations Of
BASES OF INFINITE-DIMENSIONAL REPRESENTATIONS OF ORTHOSYMPLECTIC LIE SUPERALGEBRAS by DWIGHT ANDERSON WILLIAMS II Presented to the Faculty of the Graduate School of The University of Texas at Arlington in Partial Fulfillment of the Requirements for the Degree of DOCTOR OF PHILOSOPHY THE UNIVERSITY OF TEXAS AT ARLINGTON May 2020 Copyright c by Dwight Anderson Williams II 2020 All Rights Reserved ACKNOWLEDGEMENTS God is the only mathematician who should say that the proof is trivial. Thank you God for showing me well-timed hints and a few nearly-complete solutions. \The beginning of the beginning." Thank you Dimitar Grantcharov for advising me, for allowing your great sense of humor, kindness, brilliance, respect, and mathe- matical excellence to easily surpass your great height{it is an honor to look up to you and to look forward towards continued collaboration. Work done by committee Thank you to my committe members (alphabetically listed by surname): Edray Goins, David Jorgensen, Christopher Kribs, Barbara Shipman, and Michaela Vancliff. April 30, 2020 iii ABSTRACT BASES OF INFINITE-DIMENSIONAL REPRESENTATIONS OF ORTHOSYMPLECTIC LIE SUPERALGEBRAS Dwight Anderson Williams II, Ph.D. The University of Texas at Arlington, 2020 Supervising Professor: Dimitar Grantcharov We provide explicit bases of representations of the Lie superalgebra osp(1j2n) obtained by taking tensor products of infinite-dimensional representation and the standard representation. This infinite-dimensional representation is the space of polynomials C[x1; : : : ; xn]. Also, we provide a new differential operator realization of osp(1j2n) in terms of differential operators of n commuting variables x1; : : : ; xn and 2n anti-commuting variables ξ1; : : : ; ξ2n. -
Boolean Product Polynomials, Schur Positivity, and Chern Plethysm
BOOLEAN PRODUCT POLYNOMIALS, SCHUR POSITIVITY, AND CHERN PLETHYSM SARA C. BILLEY, BRENDON RHOADES, AND VASU TEWARI Abstract. Let k ≤ n be positive integers, and let Xn = (x1; : : : ; xn) be a list of n variables. P The Boolean product polynomial Bn;k(Xn) is the product of the linear forms i2S xi where S ranges over all k-element subsets of f1; 2; : : : ; ng. We prove that Boolean product polynomials are Schur positive. We do this via a new method of proving Schur positivity using vector bundles and a symmetric function operation we call Chern plethysm. This gives a geometric method for producing a vast array of Schur positive polynomials whose Schur positivity lacks (at present) a combinatorial or representation theoretic proof. We relate the polynomials Bn;k(Xn) for certain k to other combinatorial objects including derangements, positroids, alternating sign matrices, and reverse flagged fillings of a partition shape. We also relate Bn;n−1(Xn) to a bigraded action of the symmetric group Sn on a divergence free quotient of superspace. 1. Introduction The symmetric group Sn of permutations of [n] := f1; 2; : : : ; ng acts on the polynomial ring C[Xn] := C[x1; : : : ; xn] by variable permutation. Elements of the invariant subring Sn (1.1) C[Xn] := fF (Xn) 2 C[Xn]: w:F (Xn) = F (Xn) for all w 2 Sn g are called symmetric polynomials. Symmetric polynomials are typically defined using sums of products of the variables x1; : : : ; xn. Examples include the power sum, the elementary symmetric polynomial, and the homogeneous symmetric polynomial which are (respectively) (1.2) k k X X pk(Xn) = x1 + ··· + xn; ek(Xn) = xi1 ··· xik ; hk(Xn) = xi1 ··· xik : 1≤i1<···<ik≤n 1≤i1≤···≤ik≤n Given a partition λ = (λ1 ≥ · · · ≥ λk > 0) with k ≤ n parts, we have the monomial symmetric polynomial X (1.3) m (X ) = xλ1 ··· xλk ; λ n i1 ik i1; : : : ; ik distinct as well as the Schur polynomial sλ(Xn) whose definition is recalled in Section 2. -
Matrix Computations in Linear Superalgebra Institute De Znvestigaciones En Matemhticas Aplicadas Y Sistemus Universidad Nacionul
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Matrix Computations in Linear Superalgebra Oscar Adolf0 Sanchez Valenzuela* Institute de Znvestigaciones en Matemhticas Aplicadas y Sistemus Universidad Nacionul Authwmu de M&co Apdo, Postal 20-726; Admon. No. 20 Deleg. Alvaro Obreg6n 01000 M&ico D.F., M&co Submitted by Marvin D. Marcus ABSTRACT The notions of supervector space, superalgebra, supermodule, and finite dimen- sional free super-module over a supercommutative superalgebra are reviewed. Then, a functorial correspondence is established between (free) supermodule morphisms and matrices with coefficients in the corresponding supercommutative superalgebra. It is shown that functoriality requires the rule for matrix multiplication to be different from the usual one. It has the advantage, however, of making the analogues of the nongraded formulas retain their familiar form (the chain rule is but one example of this). INTRODUCTION This paper is intended to serve as reference for definitions and conven- tions behind our work in super-manifolds: [6], [7], and [8]. More important perhaps, is the fact that we show here how computations have to be carried out in a consistent way within the category of supermodules over a super- commutative superalgebra-a point that has not been stressed in the litera- ture so far., To begin with, we shall adhere to the standard usage of the prefix super by letting it stand for Z,-graded, as in [l]. Thus, we shall review the notions *Current address: Centro de Investigacibn en Matemiticas, CIMAT, Apartado Postal 402, C.P. -
Plethysm and Lattice Point Counting
Plethysm and lattice point counting Thomas Kahle OvG Universit¨at Magdeburg joint work with M. Micha lek Some representation theory • Finite-dimensional, rational, irreducible representations of GL(n) are indexed by Young diagrams with at most n rows. • The correspondence is via the Schur functor: λ $ Sλ. • Sλ applied to the trivial representation gives an irreducible representation. Example and Convention • Only one row (λ = (d)): SλW = SdW (degree d forms on W ) • Only one column (λ = (1;:::; 1)): Sλ(W ) = Vd W Schur functor plethysm The general plethysm A Schur functor Sµ can be applied to any representation, for instance an irreducible SνW µ ν L λ ⊕cλ • S (S W ) decomposes into λ(S ) . • General plethysm: Determine cλ as a function of (λ, µ, ν). ! impossible? More modest goals { Symmetric powers • Decompose Sd(SkW ) into irreducibles. ! still hard. • Low degree: Fix d, seek function of (k; λ). Proposition (Thrall, 1942) One has GL(W )-module decompositions 2 M ^ M S2(SkW ) = SλW; (SkW ) = SµW; where • λ runs over tableaux with 2k boxes in two rows of even length. • µ runs over tableaux with 2k boxes in two rows of odd length. • Note: Divisibility conditions on the appearing tableaux. • Similar formulas for S3(Sk) obtained by Agaoka, Chen, Duncan, Foulkes, Garsia, Howe, Plunkett, Remmel, Thrall, . • A few things are known about S4(Sk) (Duncan, Foulkes, Howe). • Observation: Tableaux counting formulas get unwieldy quickly. Theorem (KM) λ d k Fix d. For any k 2 N, and λ ` dk, the multiplicity of S in S (S ) is d−1 X Dα X (−1)( 2 ) sgn(π)Q (k; λ ) ; d! α π α`d π2Sd−1 where • Qα are counting functions of parametric lattice polytopes • Dα is the number of permutations of cycle type α. -
Topics in Group Representation Theory
Topics in Group Representation Theory Peter Webb October 2, 2017 Contents 0.1 Representations of Sr ............................1 0.2 Polynomial representations of GLn(k)...................1 0.3 Representations of GL(Fpn ).........................2 0.4 Functorial methods . .2 1 Dual spaces and bilinear forms 3 2 Representations of Sr 4 2.1 Tableaux and tabloids . .4 2.2 Permutation modules . .5 2.2.1 Exercise . .7 2.3 p-regular partitions . .7 2.4 Young modules . .9 3 The Schur algebra 11 3.1 Tensor space . 11 3.2 Homomorphisms between permutation modules . 14 3.3 The structure of endomorphism rings . 15 3.4 The radical . 17 3.5 Projective covers, Nakayama's lemma and lifting of idempotents . 20 3.6 Projective modules for finite dimensional algebras . 24 3.7 Cartan invariants . 26 3.8 Projective and simple modules for SF (n; r)................ 28 3.9 Duality and the Schur algebra . 30 4 Polynomial representations of GLn(F ) 33 4.0.1 Multi-indices . 39 4.1 Weights and Characters . 40 5 Connections between the Schur algebra and the symmetric group: the Schur functor 47 5.1 The general theory of the functor f : B -mod ! eBe -mod . 51 5.2 Applications . 51 i CONTENTS ii 6 Representations of the category of vector spaces 54 6.1 Simple representations of the matrix monoid . 55 6.2 Simple representations of categories and the category algebra . 57 6.3 Parametrization of simple and projective representations . 60 6.4 Projective functors . 63 7 Bibliography 68 Landmark Theorems 0.1 Representations of Sr λ Theorem 0.1.1.