Complex Orbits of Solvable Groups
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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. -
Representation Theory
M392C NOTES: REPRESENTATION THEORY ARUN DEBRAY MAY 14, 2017 These notes were taken in UT Austin's M392C (Representation Theory) class in Spring 2017, taught by Sam Gunningham. I live-TEXed them using vim, so there may be typos; please send questions, comments, complaints, and corrections to [email protected]. Thanks to Kartik Chitturi, Adrian Clough, Tom Gannon, Nathan Guermond, Sam Gunningham, Jay Hathaway, and Surya Raghavendran for correcting a few errors. Contents 1. Lie groups and smooth actions: 1/18/172 2. Representation theory of compact groups: 1/20/174 3. Operations on representations: 1/23/176 4. Complete reducibility: 1/25/178 5. Some examples: 1/27/17 10 6. Matrix coefficients and characters: 1/30/17 12 7. The Peter-Weyl theorem: 2/1/17 13 8. Character tables: 2/3/17 15 9. The character theory of SU(2): 2/6/17 17 10. Representation theory of Lie groups: 2/8/17 19 11. Lie algebras: 2/10/17 20 12. The adjoint representations: 2/13/17 22 13. Representations of Lie algebras: 2/15/17 24 14. The representation theory of sl2(C): 2/17/17 25 15. Solvable and nilpotent Lie algebras: 2/20/17 27 16. Semisimple Lie algebras: 2/22/17 29 17. Invariant bilinear forms on Lie algebras: 2/24/17 31 18. Classical Lie groups and Lie algebras: 2/27/17 32 19. Roots and root spaces: 3/1/17 34 20. Properties of roots: 3/3/17 36 21. Root systems: 3/6/17 37 22. Dynkin diagrams: 3/8/17 39 23. -
Special Unitary Group - Wikipedia
Special unitary group - Wikipedia https://en.wikipedia.org/wiki/Special_unitary_group Special unitary group In mathematics, the special unitary group of degree n, denoted SU( n), is the Lie group of n×n unitary matrices with determinant 1. (More general unitary matrices may have complex determinants with absolute value 1, rather than real 1 in the special case.) The group operation is matrix multiplication. The special unitary group is a subgroup of the unitary group U( n), consisting of all n×n unitary matrices. As a compact classical group, U( n) is the group that preserves the standard inner product on Cn.[nb 1] It is itself a subgroup of the general linear group, SU( n) ⊂ U( n) ⊂ GL( n, C). The SU( n) groups find wide application in the Standard Model of particle physics, especially SU(2) in the electroweak interaction and SU(3) in quantum chromodynamics.[1] The simplest case, SU(1) , is the trivial group, having only a single element. The group SU(2) is isomorphic to the group of quaternions of norm 1, and is thus diffeomorphic to the 3-sphere. Since unit quaternions can be used to represent rotations in 3-dimensional space (up to sign), there is a surjective homomorphism from SU(2) to the rotation group SO(3) whose kernel is {+ I, − I}. [nb 2] SU(2) is also identical to one of the symmetry groups of spinors, Spin(3), that enables a spinor presentation of rotations. Contents Properties Lie algebra Fundamental representation Adjoint representation The group SU(2) Diffeomorphism with S 3 Isomorphism with unit quaternions Lie Algebra The group SU(3) Topology Representation theory Lie algebra Lie algebra structure Generalized special unitary group Example Important subgroups See also 1 of 10 2/22/2018, 8:54 PM Special unitary group - Wikipedia https://en.wikipedia.org/wiki/Special_unitary_group Remarks Notes References Properties The special unitary group SU( n) is a real Lie group (though not a complex Lie group). -
Lie Groups and Linear Algebraic Groups I. Complex and Real Groups Armand Borel
Lie Groups and Linear Algebraic Groups I. Complex and Real Groups Armand Borel 1. Root systems x 1.1. Let V be a finite dimensional vector space over Q. A finite subset of V is a root system if it satisfies: RS 1. Φ is finite, consists of non-zero elements and spans V . RS 2. Given a Φ, there exists an automorphism ra of V preserving Φ 2 ra such that ra(a) = a and its fixed point set V has codimension 1. [Such a − transformation is unique, of order 2.] The Weyl group W (Φ) or W of Φ is the subgroup of GL(V ) generated by the ra (a Φ). It is finite. Fix a positive definite scalar product ( , ) on V invariant 2 under W . Then ra is the reflection to the hyperplane a. ? 1 RS 3. Given u; v V , let nu;v = 2(u; v) (v; v)− . We have na;b Z for all 2 · 2 a; b Φ. 2 1.2. Some properties. (a) If a and c a (c > 0) belong to Φ, then c = 1; 2. · The system Φ is reduced if only c = 1 occurs. (b) The reflection to the hyperplane a = 0 (for any a = 0) is given by 6 (1) ra(v) = v nv;aa − therefore if a; b Φ are linearly independent, and (a; b) > 0 (resp. (a; b) < 0), 2 then a b (resp. a + b) is a root. On the other hand, if (a; b) = 0, then either − a + b and a b are roots, or none of them is (in which case a and b are said to be − strongly orthogonal). -
Lie Groups and Representations
Notes for Lie Groups & Representations Instructor: Andrei Okounkov Henry Liu December 12, 2016 Abstract These are my live-texed notes for the Fall 2016 offering of MATH GR6343 Lie Groups & Representa- tions. There are known omissions from when I zone out in class, and additional material from when I'm trying to better understand the material. Let me know when you find errors or typos. I'm sure there are plenty. 1 Lie Groups 1 1.1 Definition and Examples . 1 1.2 Lie group actions . 2 1.3 Proper actions . 4 1.4 Some Lie group properties . 7 1.5 Symplectic matrices . 7 1.6 Fundamental groups of Lie groups . 8 2 Lie Algebras 9 2.1 From Lie groups to Lie algebras . 9 2.2 The Lie functor . 10 2.3 Lie algebra to Lie group . 11 2.4 Exponential map . 12 2.5 Digression: classical mechanics . 14 2.6 Universal enveloping algebra . 15 2.7 Poisson algebras and Poisson manifolds . 17 2.8 Baker{Campbell–Hausdorff formula . 19 3 Compact Lie groups 21 3.1 Peter{Weyl theorem . 21 3.2 Compact operators . 23 3.3 Complexifications . 24 3.4 Symmetric spaces . 24 4 Subgroups and subalgebras 27 4.1 Solvable and nilpotent Lie algebras . 27 4.2 Parabolic and Borel subgroups . 30 4.3 Maximal tori . 32 4.4 More Borel subgroups . 33 4.5 Levi{Malcev decomposition . 35 5 Semisimple theory 37 5.1 Roots and weights . 37 5.2 Root systems . 39 a Chapter 1 Lie Groups 1.1 Definition and Examples Definition 1.1.1. -
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. -
Complex Geometry and Representations of Lie Groups
http://dx.doi.org/10.1090/conm/288/04826 Contemporary Mathematics Volume 288, 2001 Complex Geometry and Representations of Lie Groups Joseph A. Wolf Dedicated to the memory of my friend and colleague Alfred Gray ABSTRACT. Let Z = G/Q be a complex flag manifold and let Go be a real form of G. Then the representation theory of the real reductive Lie group Go is intimately connected with the geometry of Go-orbits on Z. The open orbits correspond to the discrete series representations and their analytic con- tinuations, closed orbits correspond to the principal series, and certain other orbits give the other series of tempered representations. Here I try to indicate some of that interplay between geometry and analysis, concentrating on the complex geometric aspects of the open orbits and the related representations. Contents: §0. Introduction Part I. Geometry of Flag Manifolds §1. Parabolic Subalgebras and Complex Flags §2. Real Group Orbits on Complex Flags §3. The Closed Orbit §4. Open Orbits §5. Cycle Spaces §6. The Double Fibration Transform Part II. Representations of Reductive Lie Groups §7. The Principal Series §8. The Discrete Series §9. The Various Tempered Series §10. The Plancherel Formula Part III. Geometric Realizations of Representations §11. L 2 Realizations of the Principal Series §12. £ 2 Realizations of the Discrete Series §13. L 2 Realizations of the Various Tempered Series §14. Approaches to Non-Tempered Representations 2000 Mathematics Subject Classification. Primary 22E15, 22E46, 43A80; secondary 22E10, 32E10, 32M10, 32T15. Key words and phrases. reductive Lie group, reductive Lie algebra, semisimple Lie group, semisimple Lie algebra, representation, flag manifold, flag domain. -
Lie Algebras, Algebraic Groups, and Lie Groups
Lie Algebras, Algebraic Groups, and Lie Groups J.S. Milne Version 2.00 May 5, 2013 These notes are an introduction to Lie algebras, algebraic groups, and Lie groups in characteristic zero, emphasizing the relationships between these objects visible in their cat- egories of representations. Eventually these notes will consist of three chapters, each about 100 pages long, and a short appendix. BibTeX information: @misc{milneLAG, author={Milne, James S.}, title={Lie Algebras, Algebraic Groups, and Lie Groups}, year={2013}, note={Available at www.jmilne.org/math/} } v1.00 March 11, 2012; 142 pages. V2.00 May 1, 2013; 186 pages. Please send comments and corrections to me at the address on my website http://www.jmilne.org/math/. The photo is of a grotto on The Peak That Flew Here, Hangzhou, Zhejiang, China. Copyright c 2012, 2013 J.S. Milne. Single paper copies for noncommercial personal use may be made without explicit permis- sion from the copyright holder. Table of Contents Table of Contents3 Preface........................................ 5 I Lie Algebras 11 1 Definitions and basic properties........................ 11 2 Nilpotent Lie algebras: Engel’s theorem................... 26 3 Solvable Lie algebras: Lie’s theorem..................... 33 4 Semisimple Lie algebras ........................... 40 5 Representations of Lie algebras: Weyl’s theorem .............. 46 6 Reductive Lie algebras; Levi subalgebras; Ado’s theorem.......... 56 7 Root systems and their classification..................... 66 8 Split semisimple Lie algebras......................... 77 9 Representations of split semisimple Lie algebras . 100 10 Real Lie algebras...............................102 11 Classical Lie algebras.............................103 II Algebraic Groups 105 1 Algebraic groups ...............................106 2 Representations of algebraic groups; tensor categories . -
1 Representations of Lie Groups
Lie Theory Through Examples John Baez Lecture 3 1 Representations of Lie Groups We’ve been having some fun getting lattices from simply-connected complex simple Lie groups. If someone hands us one of these, say G, we first choose a maximal compact subgroup K ⊆ G. They’re all conjugate inside G, so it doesn’t matter which one we choose. Then, we choose a maximal torus T ⊆ K. Again, they’re all conjugate inside K, so it doesn’t matter which one we choose. Then we can work out the Lie algebra t of T and find a lattice L = ker e =⊆ t, where e: t → T x 7→ exp(2πx). So far we’ve done this for G = SL(3, C) and K = SL(4, C). The other SL(n, C)’s work similarly, and soon we’ll do even more examples. It’s a lot of fun. But, what’s it all good for? Among other things, it’s good for classifying the complex-analytic representations of G, and the unitary representations of K. So, we need a word or two about these. Remember that a representation of any Lie group H is a smooth homomorphism ρ: H → GL(V ) where V is a vector space and GL(V ) is the group of invertible linear transformations of V . In what follows we’ll always assume V is finite-dimensional. When V = Cn we also call GL(V ) the general linear group GL(n, C). Now, the group GL(V ) is always a complex manifold: we can cover it with coordinate charts that look like Cn, with complex-analytic transition functions. -
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. -
CLASSICAL GROUPS 1. Orthogonal Groups These Notes Are About
CLASSICAL GROUPS DAVID VOGAN 1. Orthogonal groups These notes are about \classical groups." That term is used in various ways by various people; I'll try to say a little about that as I go along. Basi- cally these are groups of matrices with entries in fields or division algebras. To warm up, I'll recall a definition of the orthogonal group. Definition 1.1. Suppose n ≥ 1 is an integer. The real orthogonal group O(n) is O(n) = all n × n real matrices g such that tgg = I : Here if A is an m × n matrix, tA is the n × n matrix whose (j; i) entry is equal to the (i; j) entry of A. Here is another way to formulate the definition. Write n (1.2a) R = fcolumn vectors of size ng = fn × 1 matricesg and identify n m (1.2b) Hom(R ; R ) ' fm × n real matrices Ag =def Mm×n(R) by matrix multiplication on the left. For the (most important) case of square matrices, we will write (1.2c) Mn(R) =def Mn×n(R); this is a real algebra under matrix multiplication, and a real Lie algebra under commutator of matrices: (1.2d) [A; B] = AB − BA (A; B 2 Mn(R): Write t n (1.2e) (; ) = (; )n ; (v; w) = v · w; (v; w 2 R ) n for the standard inner product on R . Then t n m (1.2f) (Av; w)m = v; Aw n (v 2 R ; w 2 R ;A 2 Mm×n(R): With this notation, it is very easy to check that n (1.3) O(n) = flinear transformations of R preserving (; )ng : 1 2 DAVID VOGAN The orthogonal group is the first classical group. -
Transformation Groups on Compact Symmetric Spaces
TRANSFORMATION GROUPS ON COMPACT SYMMETRIC SPACES BY TADASHI NAGANO (i) The symmetric spaces constitute the most important class of Riemannian manifolds; some of them have been the standard spaces in various branches of geometry, and many authors threw light upon their deep properties. Still there seems to be no thorough study of general transformation groups L (other than the isometry groups H, but containing G) of compact(2) symmetric spaces M, which we call geometric transformation groups of M in this introduction. Its need will be patent if it will reveal interrelations of symmetric spaces, and if L will be the automorphism group of some geometric structure of M, more or less closely related with the Riemannian structure of M, by which M is geomet- rically distinguished from the other symmetric spaces. Let us observe a few examples. Let M be the sphere as a symmetric space. M has the projective [respectively, conformai] structure; it can be thought of as the set of all geodesies [respectively, the function which gives the angles be- tween two tangent vectors at the same points] of M. This can be defined, of course, for any Riemannian manifold, but the automorphism group L, or the projective [respectively, conformai] transformation group, differs from the isometry group G for the sphere M, and by this fact, M is distinguished from all other symmetric spaces (except the real projective space which is locally isometric with M), as asserted by E. Cartan [Oeuvres complètes, Partie I, Vol. II, Gauthier-Villars, Paris, 1952, p. 659]. (See [7], [8] for the proof.) M is the standard space in the projective [respectively, conformai] differential geometry.