On the Conjugacy Theorem of Cartan Subalgebras
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Irreducible Representations of Complex Semisimple Lie Algebras
Irreducible Representations of Complex Semisimple Lie Algebras Rush Brown September 8, 2016 Abstract In this paper we give the background and proof of a useful theorem classifying irreducible representations of semisimple algebras by their highest weight, as well as restricting what that highest weight can be. Contents 1 Introduction 1 2 Lie Algebras 2 3 Solvable and Semisimple Lie Algebras 3 4 Preservation of the Jordan Form 5 5 The Killing Form 6 6 Cartan Subalgebras 7 7 Representations of sl2 10 8 Roots and Weights 11 9 Representations of Semisimple Lie Algebras 14 1 Introduction In this paper I build up to a useful theorem characterizing the irreducible representations of semisim- ple Lie algebras, namely that finite-dimensional irreducible representations are defined up to iso- morphism by their highest weight ! and that !(Hα) is an integer for any root α of R. This is the main theorem Fulton and Harris use for showing that the Weyl construction for sln gives all (finite-dimensional) irreducible representations. 1 In the first half of the paper we'll see some of the general theory of semisimple Lie algebras| building up to the existence of Cartan subalgebras|for which we will use a mix of Fulton and Harris and Serre ([1] and [2]), with minor changes where I thought the proofs needed less or more clarification (especially in the proof of the existence of Cartan subalgebras). Most of them are, however, copied nearly verbatim from the source. In the second half of the paper we will describe the roots of a semisimple Lie algebra with respect to some Cartan subalgebra, the weights of irreducible representations, and finally prove the promised result. -
Algebraic D-Modules and Representation Theory Of
Contemporary Mathematics Volume 154, 1993 Algebraic -modules and Representation TheoryDof Semisimple Lie Groups Dragan Miliˇci´c Abstract. This expository paper represents an introduction to some aspects of the current research in representation theory of semisimple Lie groups. In particular, we discuss the theory of “localization” of modules over the envelop- ing algebra of a semisimple Lie algebra due to Alexander Beilinson and Joseph Bernstein [1], [2], and the work of Henryk Hecht, Wilfried Schmid, Joseph A. Wolf and the author on the localization of Harish-Chandra modules [7], [8], [13], [17], [18]. These results can be viewed as a vast generalization of the classical theorem of Armand Borel and Andr´e Weil on geometric realiza- tion of irreducible finite-dimensional representations of compact semisimple Lie groups [3]. 1. Introduction Let G0 be a connected semisimple Lie group with finite center. Fix a maximal compact subgroup K0 of G0. Let g be the complexified Lie algebra of G0 and k its subalgebra which is the complexified Lie algebra of K0. Denote by σ the corresponding Cartan involution, i.e., σ is the involution of g such that k is the set of its fixed points. Let K be the complexification of K0. The group K has a natural structure of a complex reductive algebraic group. Let π be an admissible representation of G0 of finite length. Then, the submod- ule V of all K0-finite vectors in this representation is a finitely generated module over the enveloping algebra (g) of g, and also a direct sum of finite-dimensional U irreducible representations of K0. -
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. -
Lattic Isomorphisms of Lie Algebras
LATTICE ISOMORPHISMS OF LIE ALGEBRAS D. W. BARNES (received 16 March 1964) 1. Introduction Let L be a finite dimensional Lie algebra over the field F. We denote by -S?(Z.) the lattice of all subalgebras of L. By a lattice isomorphism (which we abbreviate to .SP-isomorphism) of L onto a Lie algebra M over the same field F, we mean an isomorphism of £P(L) onto J&(M). It is possible for non-isomorphic Lie algebras to be J?-isomorphic, for example, the algebra of real vectors with product the vector product is .Sf-isomorphic to any 2-dimensional Lie algebra over the field of real numbers. Even when the field F is algebraically closed of characteristic 0, the non-nilpotent Lie algebra L = <a, bt, • • •, br} with product defined by ab{ = b,, b(bf = 0 (i, j — 1, 2, • • •, r) is j2?-isomorphic to the abelian algebra of the same di- mension1. In this paper, we assume throughout that F is algebraically closed of characteristic 0 and are principally concerned with semi-simple algebras. We show that semi-simplicity is preserved under .Sf-isomorphism, and that ^-isomorphic semi-simple Lie algebras are isomorphic. We write mappings exponentially, thus the image of A under the map <p v will be denoted by A . If alt • • •, an are elements of the Lie algebra L, we denote by <a,, • • •, an> the subspace of L spanned by au • • • ,an, and denote by <<«!, • • •, «„» the subalgebra generated by a,, •••,«„. For a single element a, <#> = «a>>. The product of two elements a, 6 el. -
LIE ALGEBRAS in CLASSICAL and QUANTUM MECHANICS By
LIE ALGEBRAS IN CLASSICAL AND QUANTUM MECHANICS by Matthew Cody Nitschke Bachelor of Science, University of North Dakota, 2003 A Thesis Submitted to the Graduate Faculty of the University of North Dakota in partial ful¯llment of the requirements for the degree of Master of Science Grand Forks, North Dakota May 2005 This thesis, submitted by Matthew Cody Nitschke in partial ful¯llment of the require- ments for the Degree of Master of Science from the University of North Dakota, has been read by the Faculty Advisory Committee under whom the work has been done and is hereby approved. (Chairperson) This thesis meets the standards for appearance, conforms to the style and format require- ments of the Graduate School of the University of North Dakota, and is hereby approved. Dean of the Graduate School Date ii PERMISSION Title Lie Algebras in Classical and Quantum Mechanics Department Physics Degree Master of Science In presenting this thesis in partial ful¯llment of the requirements for a graduate degree from the University of North Dakota, I agree that the library of this University shall make it freely available for inspection. I further agree that permission for extensive copying for scholarly purposes may be granted by the professor who supervised my thesis work or, in his absence, by the chairperson of the department or the dean of the Graduate School. It is understood that any copying or publication or other use of this thesis or part thereof for ¯nancial gain shall not be allowed without my written permission. It is also understood that due recognition shall be given to me and to the University of North Dakota in any scholarly use which may be made of any material in my thesis. -
Contents 1 Root Systems
Stefan Dawydiak February 19, 2021 Marginalia about roots These notes are an attempt to maintain a overview collection of facts about and relationships between some situations in which root systems and root data appear. They also serve to track some common identifications and choices. The references include some helpful lecture notes with more examples. The author of these notes learned this material from courses taught by Zinovy Reichstein, Joel Kam- nitzer, James Arthur, and Florian Herzig, as well as many student talks, and lecture notes by Ivan Loseu. These notes are simply collected marginalia for those references. Any errors introduced, especially of viewpoint, are the author's own. The author of these notes would be grateful for their communication to [email protected]. Contents 1 Root systems 1 1.1 Root space decomposition . .2 1.2 Roots, coroots, and reflections . .3 1.2.1 Abstract root systems . .7 1.2.2 Coroots, fundamental weights and Cartan matrices . .7 1.2.3 Roots vs weights . .9 1.2.4 Roots at the group level . .9 1.3 The Weyl group . 10 1.3.1 Weyl Chambers . 11 1.3.2 The Weyl group as a subquotient for compact Lie groups . 13 1.3.3 The Weyl group as a subquotient for noncompact Lie groups . 13 2 Root data 16 2.1 Root data . 16 2.2 The Langlands dual group . 17 2.3 The flag variety . 18 2.3.1 Bruhat decomposition revisited . 18 2.3.2 Schubert cells . 19 3 Adelic groups 20 3.1 Weyl sets . 20 References 21 1 Root systems The following examples are taken mostly from [8] where they are stated without most of the calculations. -
Ind-Varieties of Generalized Flags: a Survey of Results
Ind-varieties of generalized flags: a survey of results∗ Mikhail V. Ignatyev Ivan Penkov Abstract. This is a review of results on the structure of the homogeneous ind-varieties G/P of the ind-groups G = GL∞(C), SL∞(C), SO∞(C), Sp∞(C), subject to the condition that G/P is a inductive limit of compact homogeneous spaces Gn/Pn. In this case the subgroup P ⊂ G is a splitting parabolic subgroup of G, and the ind-variety G/P admits a “flag realization”. Instead of ordinary flags, one considers generalized flags which are, generally infinite, chains C of subspaces in the natural representation V of G which satisfy a certain condition: roughly speaking, for each nonzero vector v of V there must be a largest space in C which does not contain v, and a smallest space in C which contains v. We start with a review of the construction of the ind-varieties of generalized flags, and then show that these ind-varieties are homogeneous ind-spaces of the form G/P for splitting parabolic ind-subgroups P ⊂ G. We also briefly review the characterization of more general, i.e. non-splitting, parabolic ind-subgroups in terms of generalized flags. In the special case of an ind-grassmannian X, we give a purely algebraic-geometric construction of X. Further topics discussed are the Bott– Borel–Weil Theorem for ind-varieties of generalized flags, finite-rank vector bundles on ind-varieties of generalized flags, the theory of Schubert decomposition of G/P for arbitrary splitting parabolic ind-subgroups P ⊂ G, as well as the orbits of real forms on G/P for G = SL∞(C). -
Parabolic Subalgebras, Parabolic Buildings and Parabolic Projection
PARABOLIC SUBALGEBRAS, PARABOLIC BUILDINGS AND PARABOLIC PROJECTION DAVID M. J. CALDERBANK AND PASSAWAN NOPPAKAEW Abstract. Reductive (or semisimple) algebraic groups, Lie groups and Lie algebras have a rich geometry determined by their parabolic subgroups and subalgebras, which carry the structure of a building in the sense of J. Tits. We present herein an elementary approach to the geometry of parabolic subalgebras, over an arbitrary field of characteristic zero, which does not rely upon the structure theory of semisimple Lie algebras. Indeed we derive such structure theory, from root systems to the Bruhat decomposition, from the properties of parabolic subalgebras. As well as constructing the Tits building of a reductive Lie algebra, we establish a “parabolic projection” process which sends parabolic subalgebras of a reductive Lie algebra to parabolic subalgebras of a Levi subquotient. We indicate how these ideas may be used to study geometric configurations and their moduli. Parabolic subgroups and their Lie algebras are fundamental in Lie theory and the theory of algebraic groups [2, 16, 17, 19, 21, 25, 29, 35, 38]. They play a key role in combinatorial, differential and integrable geometry through Tits buildings and parabolic invariant theory [1, 3, 5, 8, 31, 33, 36]. Traditional approaches define parabolic subalgebras of semisimple or reductive Lie algebras as those containing a Borel (maximal solvable) subalgebra in some field extension, and typically develop the theory of parabolic subalgebras using the root system associated to a Cartan subalgebra of such a Borel subalgebra. Such approaches are far from elementary, and provide limited insight when the field is not algebraically closed. -
Automorphisms of Modular Lie Algebr S
Non Joumal of Algebra and Geometty ISSN 1060.9881 Vol. I, No.4, pp. 339-345, 1992 @ 1992 Nova Sdence Publishers, Inc. Automorphisms of Modular Lie Algebr�s Daniel E. Frohardt Robert L. Griess Jr. Dept. Math Dept. Math Wayne State University University of Michigan Faculty / Administration Building & Angell Hall Detroit, MI 48202 Ann Arbor, MI 48104 USA USA Abstract: We give a short argument ,that certain modular Lie algebras have sur prisingly large automorphism groups. 1. Introduction and statement of results A classical Lie algebra is one that has a Chevalley basis associated with an irre ducible root system. If L is a classical Lie algebra over a field K of characteristic 0 the'D.,L�has the following properties: (1) The automorphism group of L contains the ChevaUey group associated with the root system as a normal subgroup with torsion quotient grouPi (2) Lis simple. It has been known for some time that these properties do not always hold when K has positive characteristic, even when (2) is relaxed to condition (2') Lis quasi-simple, (that is, L/Z{L) is simple, where Z'{L) is the center of L), but the proofs have involved explicit computations with elements of the &lgebras. See [Stein] (whose introduction surveys the early results in this area ), [Hog]. Our first reSult is an easy demonstration of the instances of failure for (1) or (2') by use of graph automorphisms for certain Dynkin diagrams; see (2.4), (3.2) and Table 1. Only characteristics 2 and 3 are involved here., We also determine the automorphism groups of algebras of the form L/Z, where Z is a centr&l ideal of Land Lis one of the above classical quasisimple Lie algebras failing to satisfy (1) or (2'); see (3.8) and (3.9). -
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). -
Parabolic Subalgebras, Parabolic Buildings and Parabolic Projection
PARABOLIC SUBALGEBRAS, PARABOLIC BUILDINGS AND PARABOLIC PROJECTION DAVID M. J. CALDERBANK AND PASSAWAN NOPPAKAEW Abstract. Reductive (or semisimple) algebraic groups, Lie groups and Lie algebras have a rich geometry determined by their parabolic subgroups and subalgebras, which carry the structure of a building in the sense of J. Tits. We present herein an elementary approach to the geometry of parabolic subalgebras, over an arbitrary field of characteristic zero, which does not rely upon the structure theory of semisimple Lie algebras. Indeed we derive such structure theory, from root systems to the Bruhat decomposition, from the properties of parabolic subalgebras. As well as constructing the Tits building of a reductive Lie algebra, we establish a \parabolic projection" process which sends parabolic subalgebras of a reductive Lie algebra to parabolic subalgebras of a Levi subquotient. We indicate how these ideas may be used to study geometric configurations and their moduli. Parabolic subgroups and their Lie algebras are fundamental in Lie theory and the theory of algebraic groups [2, 16, 17, 19, 21, 25, 29, 35, 38]. They play a key role in combinatorial, differential and integrable geometry through Tits buildings and parabolic invariant theory [1, 3, 5, 8, 31, 33, 36]. Traditional approaches define parabolic subalgebras of semisimple or reductive Lie algebras as those containing a Borel (maximal solvable) subalgebra in some field extension, and typically develop the theory of parabolic subalgebras using the root system associated to a Cartan subalgebra of such a Borel subalgebra. Such approaches are far from elementary, and provide limited insight when the field is not algebraically closed. -
Abelian Ideals of Maximal Dimension for Solvable Lie Algebras
ABELIAN IDEALS OF MAXIMAL DIMENSION FOR SOLVABLE LIE ALGEBRAS DIETRICH BURDE AND MANUEL CEBALLOS Abstract. We compare the maximal dimension of abelian subalgebras and the maximal di- mension of abelian ideals for finite-dimensional Lie algebras. We show that these dimensions coincide for solvable Lie algebras over an algebraically closed field of characteristic zero. We compute this invariant for all complex nilpotent Lie algebras of dimension n ≤ 7. Furthermore we study the case where there exists an abelian subalgebra of codimension 2. Here we explicitly construct an abelian ideal of codimension 2 in case of nilpotent Lie algebras. 1. Introduction Let g be a finite-dimensional Lie algebra. Denote by α(g) the maximal dimension of an abelian subalgebra of g, and by β(g) the maximal dimension of an abelian ideal of g. Both invariants are important for many subjects. First of all they are very useful invariants in the study of Lie algebra contractions and degenerations. There is a large literature, in particular for low-dimensional Lie algebras, see [11, 3, 17, 21, 10], and the references given therein. Secondly, there are several results concerning the question of how big or small these maximal dimensions can be, compared to the dimension of the Lie algebra. For references see [20, 19, 15]. The results show, roughly speaking, that a Lie algebra of large dimension contains abelian sub- algebras of large dimension. For example, the dimension of a nilpotent Lie algebra g satisfying `(`+1) α(g) = ` is bounded by dim(g) ≤ 2 [20, 19]. There is a better bound for 2-step nilpotent Lie algebras, see [16].