Lie Algebras of Differential Operators and D-Modules by Dmitry Donin A

Total Page:16

File Type:pdf, Size:1020Kb

Lie Algebras of Differential Operators and D-Modules by Dmitry Donin A Lie algebras of differential operators and D-modules by Dmitry Donin A thesis submitted in conformity with the requirements for the degree of Doctor of Philosophy Graduate Department of Mathematics University of Toronto Copyright °c 2008 by Dmitry Donin Abstract Lie algebras of differential operators and D-modules Dmitry Donin Doctor of Philosophy Graduate Department of Mathematics University of Toronto 2008 In our thesis we study the algebras of differential operators in algebraic and geometric terms. We consider two problems in which the algebras of differential operators naturally arise. The first one deals with the algebraic structure of differential and pseudodifferential operators. We define the Krichever-Novikov type Lie algebras of differential operators and pseudodifferential symbols on Riemann surfaces, along with their outer derivations and central extensions. We show that the corresponding algebras of meromorphic differ- ential operators and pseudodifferential symbols have many invariant traces and central extensions, given by the logarithms of meromorphic vector fields. We describe which of these extensions survive after passing to the algebras of operators and symbols holo- morphic away from several fixed points. We also describe the associated Manin triples, emphasizing the similarities and differences with the case of smooth symbols on the circle. The second problem is related to the geometry of differential operators and its con- nection with representations of semi-simple Lie algebras. We show that the semiregular module, naturally associated with a Z-graded semi-simple complex Lie algebra g, can be realized in geometric terms, using the Brion’s construction of degeneration of the diag- onal in the square of the flag variety of g. Namely, we consider the Beilinson-Bernstein localization of the semiregular module and show that it is isomorphic to the D-module obtained by applying the Emerton-Nadler-Vilonen geometric Jacquet functor to the D- module of distributions on the square of the flag variety with support on the diagonal. ii ACKNOWLEDGEMENTS I would like to express profound gratitude to my advisors, Prof. Boris Khesin and Prof. Sergey Arkhipov for their invaluable support, encouragement, supervision and useful suggestions throughout this research work. I am highly thankful to Prof. Pierre Milman for his valuable suggestions and supervision during the whole course of my study. The moral support and continuous guidance of these people enabled me to complete my work successfully. I also would like to express my gratitude to Graduate Coordinator of the Department of Mathematics, Ida Bulat, for her continuous attention and kindness during my whole stay in the University of Toronto. iii Contents 1 Introduction 1 1.1 Krichever-Novikov type algebras . 2 1.2 A geometric realization of semiregular modules . 6 I Krichever-Novikov algebras of differential operators 12 2 History and Context 13 3 Meromorphic pseudodifferential symbols on Riemann surfaces 16 3.1 The algebras of meromorphic differential and pseudodifferential symbols . 16 3.2 Outer derivations of pseudodifferential symbols . 18 3.3 The traces . 21 3.4 The logarithmic 2-cocycles . 23 3.5 Proof of the theorem on outer derivations . 28 3.6 The double extension of the meromorphic symbols and Manin triples . 29 4 Holomorphic pseudodifferential symbols on Riemann surfaces 31 4.1 The Krichever-Novikov algebra . 31 4.2 Holomorphic differential operators and pseudodifferential symbols . 32 4.3 Holomorphic pseudodifferential symbols and the spaces of densities . 34 4.4 The density of holomorphic symbols in the smooth ones . 35 iv 4.5 The property of generalized grading . 37 4.6 Cocycles and extensions . 39 4.7 Manin triples for holomorphic pseudodifferential symbols . 44 5 Appendix A: Poisson–Lie groups, Lie bialgebras, and Manin triples 46 6 Appendix B: The Krichever-Novikov basis 48 6.1 The Riemann-Roch theorem for line bundles and the Krichever-Novikov basis . 48 6.2 Construction of the Krichever-Novikov basis . 50 6.3 Relation to the Lie algebra of vector fields on the circle . 51 II A geometric realization of semiregular modules 53 7 Notations and Preliminaries 54 8 Categories of g-modules 56 8.1 Category O .................................. 56 8.2 Verma modules . 58 8.3 Action of the Center and Harish-Chandra’s Theorem . 60 8.4 Decomposition of the category O with respect to the center and duality . 61 8.5 Projective objects in O, standard filtrations, and BGG reciprocity . 63 8.6 Harish-Chandra modules and the functor H . 65 9 Semiregular modules 70 9.1 Semiregular module . 70 9.2 Twisting functors . 73 9.3 Example . 75 10 The Jacquet functor 77 v 11 Algebraic results 81 11.1 Semiregular module as the image of the Jacquet functor . 81 11.2 Filtrations . 86 12 Geometric results 90 12.1 The De Concini-Procesi compactification . 90 12.2 Degeneration of the diagonal in the square of the flag variety . 91 12.3 Example . 92 12.4 The geometric Jacquet functor . 93 12.5 A geometric realization of semiregular modules . 95 13 Appendix A: Representable functors and Yoneda lemma 97 14 Appendix B: D-modules and the Beilinson-Bernstein localization 99 14.1 Basics on D-modules . 99 14.2 Equivariant D-modules and the Beilinson-Bernstein localization . 102 15 Appendix C: The nearby cycles functor 105 15.1 The Kashiwara-Malgrange filtration . 105 15.2 Specializable modules and nearby cycles . 106 vi Chapter 1 Introduction Differential operators appear naturally in many constructions of representation theory. In this thesis we explore certain algebraic and geometric constructions related to them and focus on the following two scopes of problems emphasizing these two sides respectively. In the first part of the thesis we study the Krichever-Novikov type Lie algebras of differential operators, as well as algebraic structures, related to them. We describe gener- alizations of the Krichever-Novikov algebras of holomorphic vector fields on a punctured Riemann surface to the case of differential operators and pseudodifferential symbols on such a surface. These algebras have a rich source of cocycles, traces, central extensions, and Manin triples. They can be defined in both the meromorphic and holomorphic contexts, have special density and almost grading properties. The second part of the thesis deals with the geometric side of differential operators and representations of semi-simple Lie algebras. We study semiregular representations associated with semi-simple Lie algebras in geometric terms. Using the Brion’s construc- tion of a degeneration of the diagonal in the square of the flag variety of the Lie algebra, we realize it as a certain degeneration of D-modules which is obtained by applying the Emerton-Nadler-Vilonen geometric Jacquet functor to the D-module of distributions on the square of the flag variety with support on the diagonal. 1 Chapter 1. Introduction 2 1.1 Krichever-Novikov type algebras The Krichever-Novikov algebras are the centrally extended Lie algebras of meromorphic vector fields on a Riemann surface Σ, which are holomorphic away from several fixed points [35, 36], see also [42, 47]. They are natural generalizations of the Virasoro algebra, which corresponds to the case of Σ = CP 1 with two punctures. A central extension of the Lie algebras of vector fields on a given Riemann surface is defined by the Gelfand-Fuchs cocycle in a fixed projective structure (that is a class of coordinates related by projective transformations). In our thesis we deal with two generalizations of the Krichever-Novikov (KN) al- gebras. The first one is the Lie algebras of all meromorphic differential operators and pseudodifferential symbols on a Riemann surface, while the second one is the Lie algebras of meromorphic differential operators and pseudodifferential symbols which are holomor- phic away from several fixed points. The main tool which we employ is fixing a reference meromorphic vector field instead of a projective structure on Σ. It turns out that such a choice allows one to write more explicit formulas for the corresponding cocycles, both for the Krichever-Novikov algebra of vector fields and for its generalizations to operators and symbols. Several features of these algebras of meromorphic symbols make them different from their smooth analogue, the algebra of pseudodifferential symbols with smooth coefficients on the circle. First of all, this is the existence of many invariant traces on the former algebras: one can associate such a trace to every point on the surface. Furthermore, we show that the logarithm log X of any meromorphic pseudodifferential symbol X defines an outer derivation of the Lie algebra of meromorphic symbols: Theorem 3.8. All derivations of the algebra of meromorphic pseudodifferential symbols defined by log X for any meromorphic pseudodifferential symbol X are outer and equiva- lent to a linear combination of derivations given by log Dv for meromorphic vector fields v. Chapter 1. Introduction 3 In turn, the combination of invariant traces and outer derivations produces a variety of independent non-trivial 2-cocycles on the Lie algebras of meromorphic pseudodifferential symbols and differential operators: Theorem 3.18. All the logarithmic 2-cocycles cv are nontrivial and non-cohomologous to each other on the algebra of meromorphic pseudodifferential symbols for different choices of meromorphic fields v 6= 0. Note that the above mentioned scheme of generating 2-cocycles in the meromorphic case, which involve log X for any meromorphic pseudodifferential symbol X, provides a natural unifying framework for the existence of two independent cocycles (generated by log @=@x and log x) in the smooth case, cf. [34, 32]. The second type of algebras under consideration, those of holomorphic differential op- erators and pseudodifferential symbols, are more direct generalizations of the Krichever- Novikov algebras of holomorphic vector fields on a punctured Riemann surface. For them we prove the density and filtered generalized grading properties, similarly to the corresponding properties of the KN algebras [35, 36]: Theorem 4.6.
Recommended publications
  • Computational Topics in Lie Theory and Representation Theory
    Utah State University DigitalCommons@USU All Graduate Theses and Dissertations Graduate Studies 5-2014 Computational Topics in Lie Theory and Representation Theory Thomas J. Apedaile Utah State University Follow this and additional works at: https://digitalcommons.usu.edu/etd Part of the Applied Statistics Commons Recommended Citation Apedaile, Thomas J., "Computational Topics in Lie Theory and Representation Theory" (2014). All Graduate Theses and Dissertations. 2156. https://digitalcommons.usu.edu/etd/2156 This Thesis is brought to you for free and open access by the Graduate Studies at DigitalCommons@USU. It has been accepted for inclusion in All Graduate Theses and Dissertations by an authorized administrator of DigitalCommons@USU. For more information, please contact [email protected]. COMPUTATIONAL TOPICS IN LIE THEORY AND REPRESENTATION THEORY by Thomas J. Apedaile A thesis submitted in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE in Mathematics Approved: Ian Anderson Nathan Geer Major Professor Committee Member Zhaohu Nie Mark R McLellan Committee Member Vice President for Research and Dean of the School of Graduate Studies UTAH STATE UNIVERSITY Logan, Utah 2014 ii Copyright c Thomas J. Apedaile 2014 All Rights Reserved iii ABSTRACT Computational Topics in Lie Theory and Representation Theory by Thomas J. Apedaile, Master of Science Utah State University, 2014 Major Professor: Dr. Ian Anderson Department: Mathematics and Statistics The computer algebra system Maple contains a basic set of commands for work- ing with Lie algebras. The purpose of this thesis was to extend the functionality of these Maple packages in a number of important areas. First, programs for defining multiplication in several types of Cayley algebras, Jordan algebras and Clifford algebras were created to allow users to perform a variety of calculations.
    [Show full text]
  • LIE GROUPS and ALGEBRAS NOTES Contents 1. Definitions 2
    LIE GROUPS AND ALGEBRAS NOTES STANISLAV ATANASOV Contents 1. Definitions 2 1.1. Root systems, Weyl groups and Weyl chambers3 1.2. Cartan matrices and Dynkin diagrams4 1.3. Weights 5 1.4. Lie group and Lie algebra correspondence5 2. Basic results about Lie algebras7 2.1. General 7 2.2. Root system 7 2.3. Classification of semisimple Lie algebras8 3. Highest weight modules9 3.1. Universal enveloping algebra9 3.2. Weights and maximal vectors9 4. Compact Lie groups 10 4.1. Peter-Weyl theorem 10 4.2. Maximal tori 11 4.3. Symmetric spaces 11 4.4. Compact Lie algebras 12 4.5. Weyl's theorem 12 5. Semisimple Lie groups 13 5.1. Semisimple Lie algebras 13 5.2. Parabolic subalgebras. 14 5.3. Semisimple Lie groups 14 6. Reductive Lie groups 16 6.1. Reductive Lie algebras 16 6.2. Definition of reductive Lie group 16 6.3. Decompositions 18 6.4. The structure of M = ZK (a0) 18 6.5. Parabolic Subgroups 19 7. Functional analysis on Lie groups 21 7.1. Decomposition of the Haar measure 21 7.2. Reductive groups and parabolic subgroups 21 7.3. Weyl integration formula 22 8. Linear algebraic groups and their representation theory 23 8.1. Linear algebraic groups 23 8.2. Reductive and semisimple groups 24 8.3. Parabolic and Borel subgroups 25 8.4. Decompositions 27 Date: October, 2018. These notes compile results from multiple sources, mostly [1,2]. All mistakes are mine. 1 2 STANISLAV ATANASOV 1. Definitions Let g be a Lie algebra over algebraically closed field F of characteristic 0.
    [Show full text]
  • Introduction to Lie Groups and Lie Algebras
    Introduction to Lie Groups and Lie Algebras Alexander Kirillov, Jr. Department of Mathematics, SUNY at Stony Brook, Stony Brook, NY 11794, USA E-mail address: [email protected] URL: http://www.math.sunysb.edu/~kirillov Contents Chapter 1. Introduction 7 Chapter 2. Lie Groups: Basic Definitions 9 §2.1. Lie groups, subgroups, and cosets 9 §2.2. Action of Lie groups on manifolds and representations 12 §2.3. Orbits and homogeneous spaces 13 §2.4. Left, right, and adjoint action 14 §2.5. Classical groups 15 Exercises 18 Chapter 3. Lie Groups and Lie algebras 21 §3.1. Exponential map 21 §3.2. The commutator 23 §3.3. Adjoint action and Jacobi identity 24 §3.4. Subalgebras, ideals, and center 25 §3.5. Lie algebra of vector fields 26 §3.6. Stabilizers and the center 28 §3.7. Campbell–Hausdorff formula 29 §3.8. Fundamental theorems of Lie theory 30 §3.9. Complex and real forms 34 §3.10. Example: so(3, R), su(2), and sl(2, C). 35 Exercises 36 Chapter 4. Representations of Lie Groups and Lie Algebras 39 §4.1. Basic definitions 39 §4.2. Operations on representations 41 §4.3. Irreducible representations 42 §4.4. Intertwining operators and Schur lemma 43 §4.5. Complete reducibility of unitary representations. Representations of finite groups 45 §4.6. Haar measure on compact Lie groups 46 3 4 Contents §4.7. Orthogonality of characters and Peter-Weyl theorem 48 §4.8. Universal enveloping algebra 51 §4.9. Poincare-Birkhoff-Witt theorem 53 Exercises 55 Chapter 5. Representations of sl(2, C) and Spherical Laplace Operator 59 §5.1.
    [Show full text]
  • Group Theory –
    DRAFT 2019 February 26 Mathematical Methods in Physics - 231B { Group Theory { Eric D'Hoker Mani L. Bhaumik Institute for Theoretical Physics Department of Physics and Astronomy University of California, Los Angeles, CA 90095, USA [email protected] The purpose of this course is to present an introduction to standard and widely used methods of group theory in Physics, including Lie groups and Lie algebras, representation theory, tensors, spinors, structure theory of solvable and simple Lie algebras, homogeneous and symmetric spaces. Contents 1 Definition and examples of groups 5 1.1 A little history . .5 1.2 Groups . .6 1.3 Topological groups . .9 1.4 Lie Groups . 12 1.5 Vector spaces . 13 1.6 Lie Algebras . 13 1.7 Relating Lie groups and Lie algebras . 15 1.8 Tangent vectors, tangent space, and cotangent space . 16 2 Matrix Lie groups and Lie algebras 18 2.1 The general linear group GL(n)........................ 18 2.2 Closed subgroups of the general linear group . 21 2.3 The orthogonal groups SO(n) and Lie algebras so(n)............ 21 2.4 The symplectic group Sp(2n) and Lie algebra sp(2n)............ 23 2.5 The unitary group SU(n) and Lie algebra su(n)............... 25 2.6 Cartan subalgebras and subgroups and the center . 26 2.7 Summary of matrix Lie groups and Lie algebras . 26 2.8 Non-semi-simple matrix groups . 30 2.9 Invariant differential forms, metric, and measure . 31 2.10 Spontaneous symmetry breaking, order parameters . 37 2.11 Lie supergroups and Lie superalgebras . 38 3 Representations 41 3.1 Representations of groups .
    [Show full text]
  • Bases for Representation Rings of Lie Groups and Their Maximal Tori
    Bases for representation rings of Lie groups and their maximal tori A Senior Project submitted to The Division of Science, Mathematics, and Computing of Bard College by Changwei Zhou arXiv:1509.08198v1 [math.RT] 28 Sep 2015 Annandale-on-Hudson, New York May, 2012 Abstract A Lie group is a group that is also a differentiable manifold, such that the group operation is continuous respect to the topological structure. To every Lie group we can associate its tangent space in the identity point as a vector space, which is its Lie algebra. Killing and Cartan completely classified simple Lie groups into seven types. Representation of a Lie group is a homomorphism from the Lie group to the automor- phism group of a vector space. In general represenations of Lie group are determined by its Lie algebra and its the connected components. We may consider operations like direct sum and tensor product with respect to which the representations of G form a ring R(G). Assume the group is compact. For every Lie group we may find a maximal torus inside of it. By projecting the representation ring of the Lie group to the representation ring of its maximal torus, we may consider to express R(T ) elements as sums of products of base elements with R(G) elements. In 1970s Pittie and Steinberg proved R(T ) is a free module over R(G) using homological algebra methods without specifying the bases in each seven types. In this senior project I found an explicit basis for the representation ring of the maximal torus of Lie group SUn in terms of the represenation ring of the Lie group itself.
    [Show full text]
  • Representations of Reductive Lie Groups
    Representations of reductive Lie groups Lectures delivered by Joe Harris Notes by Akhil Mathew Spring 2013, Harvard Contents Lecture 1 1/28 x1 Mechanics 5 x2 Philosophy 6 x3 Basic definitions 7 x4 Examples 9 Lecture 2 1/30 x1 Examples 11 x2 More examples 12 x3 General remarks 13 x4 Neighborhoods of e generate 14 x5 Isogenies and covering spaces 15 Lecture 3 2/1 x1 Recap 16 x2 Isogeny 18 x3 The adjoint representation 19 x4 Differentiating the adjoint representation 21 Lecture 4 2/4 x1 The basic setup 22 x2 Describing the bracket 23 x3 Some general re- marks 25 x4 Lie brackets and commutators 26 x5 Some more terminology 26 x6 Representations of Lie algebras 27 Lecture 5 2/6 x1 Recap 28 x2 The exponential map 31 Lecture 6 2/8 x1 The exponential map 33 x2 The Baker-Campbell-Hausdorff formula 35 Lecture 7 2/11 x1 The dictionary 38 x2 Nilpotent, solvable, and semisimple Lie algebras 39 x3 Engel's and Lie's theorems 41 Lecture 8 2/13 x1 Engel's theorem 42 x2 Lie's theorem 45 1 Lecture 9 2/15 x1 The radical 47 x2 Jordan decomposition 49 x3 An example: sl2 51 Lecture 10 2/20 x1 sl2(C) 53 x2 Irreducible representations 54 Lecture 11 2/22 x1 Recap 58 x2 Plethysm 59 x3 sl3 60 Lecture 12 2/25 x1 Recap on sl3 63 x2 Irreducible representations of sl3 64 Lecture 13 2/27 x1 Continuation of sl3 67 x2 Irreducible representations 70 Lecture 14 3/1 x1 sl3 71 x2 Examples 73 Lecture 15 3/4 x1 Examples 77 Lecture 16 3/6 x1 Outline 78 Lecture 17 3/8 Lecture 18 3/11 x1 The Killing form 85 x2 sln 87 Lecture 19 3/13 x1 sln 90 Lecture 20 3/15 x1 Geometric plethysm 92
    [Show full text]
  • On the Representation Theory of Semisimple Lie Groups
    On the Representation Theory of Semisimple Lie Groups by Faisal Al-Faisal A thesis presented to the University of Waterloo in fulfillment of the thesis requirement for the degree of Master of Mathematics in Pure Mathematics Waterloo, Ontario, Canada, 2010 c Faisal Al-Faisal 2010 I hereby declare that I am the sole author of this thesis. This is a true copy of the thesis, including any required final revisions, as accepted by my examiners. I understand that my thesis may be made electronically available to the public. ii Abstract This thesis is an expository account of three central theorems in the representation theory of semisimple Lie groups, namely the theorems of Borel{Weil{Bott, Casselman{ Osborne and Kostant. The first of these realizes all the irreducible holomorphic repre- sentations of a complex semisimple Lie group G in the cohomology of certain sheaves of equivariant line bundles over the flag variety of G. The latter two theorems describe the Lie algebra cohomology of a maximal nilpotent subalgebra of g with coefficients in an irreducible g-module. Applications to geometry and representation theory are given. Also included is a brief overview of Schmid's far-reaching generalization of the Borel{ Weil{Bott theorem to the setting of unitary representations of real semisimple Lie groups on (possibly infinite-dimensional) Hilbert spaces. iii Acknowledgements I would like to express my sincere thanks to my family and friends for their support, to my advisor Professor Wentang Kuo for his patience and insight, to my readers Professors Spiro Karigiannis and Kevin Purbhoo for their helpful comments, and to the Department of Pure Mathematics at the University of Waterloo for being my home away from home.
    [Show full text]
  • Lie Groups, Lie Algebras, and Their Representations
    Lie groups, Lie algebras, and their representations Gwyn Bellamy [email protected] www.maths.gla.ac.uk/∼gbellamy September 16, 2016 Abstract These are the lecture notes for the 5M reading course "Lie groups, Lie algebras, and their representations" at the University of Glasgow, autumn 2015. Contents 1 Introduction i 2 Manifolds - a refresher 2 3 Lie groups and Lie algebras 11 4 The exponential map 20 5 The classical Lie groups and their Lie algebras 30 6 Representation theory 35 7 The structure of Lie algebras 40 8 Complete reducibility 48 9 Cartan subalgebras and Dynkin diagrams 54 10 The classification of simple, complex Lie algebras 65 11 Weyl's character formula 69 12 Appendix: Quotient vector spaces 76 1 Introduction Lie groups and Lie algebras, together called Lie theory, originated in the study of natural symme- tries of solutions of differential equations. However, unlike say the finite collection of symmetries of the hexagon, these symmetries occurred in continuous families, just as the rotational symmetries of the plane form a continuous family isomorphic to the unit circle. The theory as we know it today began with the ground breaking work of the Norwegian mathematician Sophus Lie, who introduced the notion of continuous transformation groups and showed the crucial role that Lie algebras play in their classification and representation theory. Lie's ideas played a central role in Felix Klein's grand "Erlangen program" to classify all possible geometries using group theory. Today Lie theory plays an important role in almost every branch of pure and applied mathematics, is used to describe much of modern physics, in particular classical and quantum mechanics, and is an active area of research.
    [Show full text]
  • Arxiv:1704.07819V2 [Math.RA] 7 Aug 2017 2 5.3
    NOTES ON G2: THE LIE ALGEBRA AND THE LIE GROUP CRISTINA DRAPER FONTANALS∗ Abstract. These notes have been prepared for the Workshop on "(Non)- 6 existence of complex structures on S ", celebrated in Marburg in March, 2017. The material is not intended to be original. It contains a survey about the smallest of the exceptional Lie groups: G2, its definition and different char- 6 7 acterizations as well as its relationship to the spheres S and S . With the exception of the summary of the Killing-Cartan classification, this survey is self-contained, and all the proofs are provided. Although these proofs are well- known, they are scattered, some of them are difficult to find, and others require stronger background, while we will usually stick to linear algebra arguments. The approach is algebraical, working at the Lie algebra level most often. We analyze the complex Lie algebra (and group) of type G2 as well as the two real Lie algebras of type G2, the split and the compact one. The octonion algebra will play its role, but it is not the starting point. Also, both the 3- forms approach and the spinorial approach are viewed and connected. Special emphasis is put on relating all the viewpoints by providing precise models. Contents 1. A summary of the Killing-Cartan classification via roots 2 1.1. On simple real Lie algebras 6 2. A first linear model of (split) G2 7 2.1. The model 7 2.2. A little bit of representation theory 10 3. Understanding G2 better 11 7 3.1.
    [Show full text]
  • Introduction
    DIFFERENTIAL OPERATORS ON HOMOGENEOUS SPACES L. BARCHINI AND R. ZIERAU Abstract. These are notes for lectures given at the ICE-EM Australian Grad- uate School in Mathematics in Brisbane, July 2-20, 2007. Introduction The real flag manifolds are a interesting family of smooth manifolds. Among the real flag manifolds are the spheres, projective spaces and Grassmannians. Each is a compact homogeneous space G/P for reductive Lie group G; see Lecture 3 for a definition. There are (at least) two reasons the real flag manifolds are particularly important. One is that they are flat models for certain geometries, such as con- formal geometry and contact geometry. Another is that in representation theory the standard representations of a reductive Lie group occur as spaces of sections of homogeneous vector bundles over G/P . In both situations differential operators between sections of bundles over G/P play an important role; typically systems of such operators will have some G−equivariance properties. The goal of these lec- tures is to give some methods for constructing and studying interesting (families) of differential operators. The course begins with four lectures on the structure of reductive Lie groups and Lie algebras, and their finite dimensional representations. It is assumed that the student has had an introductory course on Lie groups and understands the basics of manifold theory. The classical groups, such as GL(n, R) and SO(p, q), are examples of reductive Lie groups. Using some linear algebra, much of the structure theory presented is easily understood for these groups. In fact students may wish to focus entirely on the group GL(n, R) (except in Lectures 13 and 14).
    [Show full text]
  • Lie Algebras
    Lie Algebras Mark Wildon October 17, 2006 Small print: These notes are intended to give the logical structure of the first half of the course; proofs and further remarks will be given in lectures. I would very much appreciate being told of any corrections or possible improvements. These notes, together with some brief notes on the linear algebra prerequisites, and the problem sheets for the course, are available via my home page, http://www-maths.swansea.ac.uk/staff/mjw/ My email address is [email protected]. Contents 1 Introduction 2 2 Fundamental definitions 4 3 Solvable Lie algebras 6 4 Engel’s theorem and nilpotent Lie algebras 8 5 Lie’s theorem 9 6 Some representation theory 10 7 Semisimple Lie algebras 14 8 The root space decomposition 15 9 The classification of complex semisimple Lie algebras 20 1 Introduction Challenge 1.1. Let n ≥ 1 and let x, y be square matrices with entries in C. Suppose that xy −yx commutes with x and y. Show that xy −yx is nilpotent; that is, (xy − yx)r =0 for some r > 0. If you solve this problem, you’ll have succeeding in finding the main idea needed to prove a major result in the theory of Lie algebras. (See Theorem 5.2.) Convention 1.2. Vector spaces in this course are always finite-dimensional. Throughout F will be a field. Definition 1.3. A Lie algebra over a field F is an F -vector space L together with a map [−, −] : L × L → L satisfying the following properties: (1) [−, −] is bilinear, (2) [x, x] =0 for all x ∈ L; anticommutativity, (3) [x, [y, z]]+[y, [z, x]]+[z, [x, y]] = 0 forall x, y, z ∈ L; the Jacobi identity.
    [Show full text]
  • Introduction
    Introduction The theory of groups really began with GALOIS ( 1811- 1832 ) who demonstrated that polynomials are best understood by examining certain groups of permutations of their roots .since that time groups have arisen in almost every branch of mathematics. One of the most important groups is the transformation groups and that is the subject of this thesis' What is the transformation groups and what are their actions ? Transformation groups can be defined as (( a collection of transformations which forms a group with composition as operation)). To illustrate this : a map f : x → x from a set X to itself is called a transformation of the set X .It is not our interest to study the properties of a single transformation but rather to study families of transformations of a set X at the same time. In particular we are interested in studying sets of transformations of X which exhibit a group structure . If G is the set of transformations of X which has a group structure then we call G a transformation group of X and X is called the G- set . We also say that G acts on X . If X has some additional mathematical structure then we usually require the transformations to preserve this structure. As an example of transformation groups : consider the usual Euclidean plane. Of course ,it is a two dimensional set, but there is more to it , namely, a concept of distance between pairs of points ,one way to study the Euclidean plane is to concentrate on distance and find enough characteristics of this concept of distance to be able to describe of the Euclidean plane geometry in terms of distance.
    [Show full text]