Geometric Methods in Representation Theory
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Affine Springer Fibers and Affine Deligne-Lusztig Varieties
Affine Springer Fibers and Affine Deligne-Lusztig Varieties Ulrich G¨ortz Abstract. We give a survey on the notion of affine Grassmannian, on affine Springer fibers and the purity conjecture of Goresky, Kottwitz, and MacPher- son, and on affine Deligne-Lusztig varieties and results about their dimensions in the hyperspecial and Iwahori cases. Mathematics Subject Classification (2000). 22E67; 20G25; 14G35. Keywords. Affine Grassmannian; affine Springer fibers; affine Deligne-Lusztig varieties. 1. Introduction These notes are based on the lectures I gave at the Workshop on Affine Flag Man- ifolds and Principal Bundles which took place in Berlin in September 2008. There are three chapters, corresponding to the main topics of the course. The first one is the construction of the affine Grassmannian and the affine flag variety, which are the ambient spaces of the varieties considered afterwards. In the following chapter we look at affine Springer fibers. They were first investigated in 1988 by Kazhdan and Lusztig [41], and played a prominent role in the recent work about the “fun- damental lemma”, culminating in the proof of the latter by Ngˆo. See Section 3.8. Finally, we study affine Deligne-Lusztig varieties, a “σ-linear variant” of affine Springer fibers over fields of positive characteristic, σ denoting the Frobenius au- tomorphism. The term “affine Deligne-Lusztig variety” was coined by Rapoport who first considered the variety structure on these sets. The sets themselves appear implicitly already much earlier in the study of twisted orbital integrals. We remark that the term “affine” in both cases is not related to the varieties in question being affine, but rather refers to the fact that these are notions defined in the context of an affine root system. -
Dynamics for Discrete Subgroups of Sl 2(C)
DYNAMICS FOR DISCRETE SUBGROUPS OF SL2(C) HEE OH Dedicated to Gregory Margulis with affection and admiration Abstract. Margulis wrote in the preface of his book Discrete subgroups of semisimple Lie groups [30]: \A number of important topics have been omitted. The most significant of these is the theory of Kleinian groups and Thurston's theory of 3-dimensional manifolds: these two theories can be united under the common title Theory of discrete subgroups of SL2(C)". In this article, we will discuss a few recent advances regarding this missing topic from his book, which were influenced by his earlier works. Contents 1. Introduction 1 2. Kleinian groups 2 3. Mixing and classification of N-orbit closures 10 4. Almost all results on orbit closures 13 5. Unipotent blowup and renormalizations 18 6. Interior frames and boundary frames 25 7. Rigid acylindrical groups and circular slices of Λ 27 8. Geometrically finite acylindrical hyperbolic 3-manifolds 32 9. Unipotent flows in higher dimensional hyperbolic manifolds 35 References 44 1. Introduction A discrete subgroup of PSL2(C) is called a Kleinian group. In this article, we discuss dynamics of unipotent flows on the homogeneous space Γn PSL2(C) for a Kleinian group Γ which is not necessarily a lattice of PSL2(C). Unlike the lattice case, the geometry and topology of the associated hyperbolic 3-manifold M = ΓnH3 influence both topological and measure theoretic rigidity properties of unipotent flows. Around 1984-6, Margulis settled the Oppenheim conjecture by proving that every bounded SO(2; 1)-orbit in the space SL3(Z)n SL3(R) is compact ([28], [27]). -
A NEW APPROACH to RANK ONE LINEAR ALGEBRAIC GROUPS An
A NEW APPROACH TO RANK ONE LINEAR ALGEBRAIC GROUPS DANIEL ALLCOCK Abstract. One can develop the basic structure theory of linear algebraic groups (the root system, Bruhat decomposition, etc.) in a way that bypasses several major steps of the standard development, including the self-normalizing property of Borel subgroups. An awkwardness of the theory of linear algebraic groups is that one must develop a lot of material before one can even characterize PGL2. Our goal here is to show how to develop the root system, etc., using only the completeness of the flag variety, its immediate consequences, and some facts about solvable groups. In particular, one can skip over the usual analysis of Cartan subgroups, the fact that G is the union of its Borel subgroups, the connectedness of torus centralizers, and the normalizer theorem (that Borel subgroups are self-normalizing). The main idea is a new approach to the structure of rank 1 groups; the key step is lemma 5. All algebraic geometry is over a fixed algebraically closed field. G always denotes a connected linear algebraic group with Lie algebra g, T a maximal torus, and B a Borel subgroup containing it. We assume the structure theory for connected solvable groups, and the completeness of the flag variety G/B and some of its consequences. Namely: that all Borel subgroups (resp. maximal tori) are conjugate; that G is nilpotent if one of its Borel subgroups is; that CG(T )0 lies in every Borel subgroup containing T ; and that NG(B) contains B of finite index and (therefore) is self-normalizing. -
Notes 9: Eli Cartan's Theorem on Maximal Tori
Notes 9: Eli Cartan’s theorem on maximal tori. Version 1.00 — still with misprints, hopefully fewer Tori Let T be a torus of dimension n. This means that there is an isomorphism T S1 S1 ... S1. Recall that the Lie algebra Lie T is trivial and that the exponential × map× is× a group homomorphism, so there is an exact sequence of Lie groups exp 0 N Lie T T T 1 where the kernel NT of expT is a discrete subgroup Lie T called the integral lattice of T . The isomorphism T S1 S1 ... S1 induces an isomorphism Lie T Rn under which the exponential map× takes× the× form 2πit1 2πit2 2πitn exp(t1,...,tn)=(e ,e ,...,e ). Irreducible characters. Any irreducible representation V of T is one dimensio- nal and hence it is given by a multiplicative character; that is a group homomorphism 1 χ: T Aut(V )=C∗. It takes values in the unit circle S — the circle being the → only compact and connected subgroup of C∗ — hence we may regard χ as a Lie group map χ: T S1. → The character χ has a derivative at the unit which is a map θ = d χ :LieT e → Lie S1 of Lie algebras. The two Lie algebras being trivial and Lie S1 being of di- 1 mension one, this is just a linear functional on Lie T . The tangent space TeS TeC∗ = ⊆ C equals the imaginary axis iR, which we often will identify with R. The derivative θ fits into the commutative diagram exp 0 NT Lie T T 1 θ N θ χ | T exp 1 1 0 NS1 Lie S S 1 The linear functional θ is not any linear functional, the values it takes on the discrete 1 subgroup NT are all in N 1 . -
Maximality of Hyperspecial Compact Subgroups Avoiding Bruhat–Tits Theory Tome 67, No 1 (2017), P
R AN IE N R A U L E O S F D T E U L T I ’ I T N S ANNALES DE L’INSTITUT FOURIER Marco MACULAN Maximality of hyperspecial compact subgroups avoiding Bruhat–Tits theory Tome 67, no 1 (2017), p. 1-21. <http://aif.cedram.org/item?id=AIF_2017__67_1_1_0> © Association des Annales de l’institut Fourier, 2017, Certains droits réservés. Cet article est mis à disposition selon les termes de la licence CREATIVE COMMONS ATTRIBUTION – PAS DE MODIFICATION 3.0 FRANCE. http://creativecommons.org/licenses/by-nd/3.0/fr/ L’accès aux articles de la revue « Annales de l’institut Fourier » (http://aif.cedram.org/), implique l’accord avec les conditions générales d’utilisation (http://aif.cedram.org/legal/). cedram Article mis en ligne dans le cadre du Centre de diffusion des revues académiques de mathématiques http://www.cedram.org/ Ann. Inst. Fourier, Grenoble 67, 1 (2017) 1-21 MAXIMALITY OF HYPERSPECIAL COMPACT SUBGROUPS AVOIDING BRUHAT–TITS THEORY by Marco MACULAN Abstract. — Let k be a complete non-archimedean field (non trivially valued). Given a reductive k-group G, we prove that hyperspecial subgroups of G(k) (i.e. those arising from reductive models of G) are maximal among bounded subgroups. The originality resides in the argument: it is inspired by the case of GLn and avoids all considerations on the Bruhat–Tits building of G. Résumé. — Soit k un corps non-archimédien complet et non trivialement va- lué. Étant donné un k-groupe réductif G, nous démontrons que les sous-groupes hyperspéciaux de G(k) (c’est-à-dire ceux qui proviennent des modèles réductifs de G) sont maximaux parmi les sous-groupes bornés. -
Sheets of Symmetric Lie Algebras and Slodowy Slices Michaël Bulois
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Archive Ouverte en Sciences de l'Information et de la Communication Sheets of Symmetric Lie Algebras and Slodowy Slices Michaël Bulois To cite this version: Michaël Bulois. Sheets of Symmetric Lie Algebras and Slodowy Slices. Journal of Lie Theory, 2011, 21, pp.1-54. hal-00464531 HAL Id: hal-00464531 https://hal.archives-ouvertes.fr/hal-00464531 Submitted on 20 Nov 2019 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Sheets of Symmetric Lie Algebras and Slodowy Slices Michaël Bulois ∗ Abstract Let θ be an involution of the finite dimmensional reductive Lie algebra g and g = k ⊕ p be the associated Cartan decomposition. Denote by K ⊂ G the connected subgroup having k as Lie algebra. (m) The K-module p is the union of the subsets p := {x | dim K.x = m}, m ∈ N, and the K-sheets of (g, θ) are the irreducible components of the p(m). The sheets can be, in turn, written as a union of so-called Jordan K-classes. We introduce conditions in order to describe the sheets and Jordan classes in terms of Slodowy slices. -
ADELIC VERSION of MARGULIS ARITHMETICITY THEOREM Hee Oh 1. Introduction Let R Denote the Set of All Prime Numbers Including
ADELIC VERSION OF MARGULIS ARITHMETICITY THEOREM Hee Oh Abstract. In this paper, we generalize Margulis’s S-arithmeticity theorem to the case when S can be taken as an infinite set of primes. Let R be the set of all primes including infinite one ∞ and set Q∞ = R. Let S be any subset of R. For each p ∈ S, let Gp be a connected semisimple adjoint Qp-group without any Qp-anisotropic factors and Dp ⊂ Gp(Qp) be a compact open subgroup for almost all finite prime p ∈ S. Let (GS , Dp) denote the restricted topological product of Gp(Qp)’s, p ∈ S with respect to Dp’s. Note that if S is finite, (GS , Dp) = Qp∈S Gp(Qp). We show that if Pp∈S rank Qp (Gp) ≥ 2, any irreducible lattice in (GS , Dp) is a rational lattice. We also present a criterion on the collections Gp and Dp for (GS , Dp) to admit an irreducible lattice. In addition, we describe discrete subgroups of (GA, Dp) generated by lattices in a pair of opposite horospherical subgroups. 1. Introduction Let R denote the set of all prime numbers including the infinite prime ∞ and Rf the set of finite prime numbers, i.e., Rf = R−{∞}. We set Q∞ = R. For each p ∈ R, let Gp be a non-trivial connected semisimple algebraic Qp-group and for each p ∈ Rf , let Dp be a compact open subgroup of Gp(Qp). The adele group of Gp, p ∈ R with respect to Dp, p ∈ Rf is defined to be the restricted topological product of the groups Gp(Qp) with respect to the distinguished subgroups Dp. -
Math 210C. Simple Factors 1. Introduction Let G Be a Nontrivial Connected Compact Lie Group, and Let T ⊂ G Be a Maximal Torus
Math 210C. Simple factors 1. Introduction Let G be a nontrivial connected compact Lie group, and let T ⊂ G be a maximal torus. 0 Assume ZG is finite (so G = G , and the converse holds by Exercise 4(ii) in HW9). Define Φ = Φ(G; T ) and V = X(T )Q, so (V; Φ) is a nonzero root system. By the handout \Irreducible components of root systems", (V; Φ) is uniquely a direct sum of irreducible components f(Vi; Φi)g in the following sense. There exists a unique collection of nonzero Q-subspaces Vi ⊂ V such that for Φi := Φ \ Vi the following hold: each pair ` (Vi; Φi) is an irreducible root system, ⊕Vi = V , and Φi = Φ. Our aim is to use the unique irreducible decomposition of the root system (which involves the choice of T , unique up to G-conjugation) and some Exercises in HW9 to prove: Theorem 1.1. Let fGjgj2J be the set of minimal non-trivial connected closed normal sub- groups of G. (i) The set J is finite, the Gj's pairwise commute, and the multiplication homomorphism Y Gj ! G is an isogeny. Q (ii) If ZG = 1 or π1(G) = 1 then Gi ! G is an isomorphism (so ZGj = 1 for all j or π1(Gj) = 1 for all j respectively). 0 (iii) Each connected closed normal subgroup N ⊂ G has finite center, and J 7! GJ0 = hGjij2J0 is a bijection between the set of subsets of J and the set of connected closed normal subgroups of G. (iv) The set fGjg is in natural bijection with the set fΦig via j 7! i(j) defined by the condition T \ Gj = Ti(j). -
The Classical Groups and Domains 1. the Disk, Upper Half-Plane, SL 2(R
(June 8, 2018) The Classical Groups and Domains Paul Garrett [email protected] http:=/www.math.umn.edu/egarrett/ The complex unit disk D = fz 2 C : jzj < 1g has four families of generalizations to bounded open subsets in Cn with groups acting transitively upon them. Such domains, defined more precisely below, are bounded symmetric domains. First, we recall some standard facts about the unit disk, the upper half-plane, the ambient complex projective line, and corresponding groups acting by linear fractional (M¨obius)transformations. Happily, many of the higher- dimensional bounded symmetric domains behave in a manner that is a simple extension of this simplest case. 1. The disk, upper half-plane, SL2(R), and U(1; 1) 2. Classical groups over C and over R 3. The four families of self-adjoint cones 4. The four families of classical domains 5. Harish-Chandra's and Borel's realization of domains 1. The disk, upper half-plane, SL2(R), and U(1; 1) The group a b GL ( ) = f : a; b; c; d 2 ; ad − bc 6= 0g 2 C c d C acts on the extended complex plane C [ 1 by linear fractional transformations a b az + b (z) = c d cz + d with the traditional natural convention about arithmetic with 1. But we can be more precise, in a form helpful for higher-dimensional cases: introduce homogeneous coordinates for the complex projective line P1, by defining P1 to be a set of cosets u 1 = f : not both u; v are 0g= × = 2 − f0g = × P v C C C where C× acts by scalar multiplication. -
Cartan and Iwasawa Decompositions in Lie Theory
CARTAN AND IWASAWA DECOMPOSITIONS IN LIE THEORY SUBHAJIT JANA Abstract. In this article we will be discussing about various decom- positions of semisimple Lie algebras, which are very important to un- derstand their structure theories. Throughout the article we will be assuming existence of a compact real form of complex semisimple Lie algebra. We will start with describing Cartan involution and Cartan de- compositions of semisimple Lie algebras. Iwasawa decompositions will also be constructed at Lie group and Lie algebra level. We will also be giving some brief description of Iwasawa of semisimple groups. 1. Introduction The idea for beginning an investigation of the structure of a general semisimple Lie group, not necessarily classical, is to look for same kind of structure in its Lie algebra. We start with a Lie algebra L of matrices and seek a decomposition into symmetric and skew-symmetric parts. To get this decomposition we often look for the occurrence of a compact Lie algebra as a real form of the complexification LC of L. If L is a real semisimple Lie algebra, then the use of a compact real form of LC leads to the construction of a 'Cartan Involution' θ of L. This involution has the property that if L = H ⊕ P is corresponding eigenspace decomposition or 'Cartan Decomposition' then, LC has a compact real form (like H ⊕iP ) which generalize decomposition of classical matrix algebra into Hermitian and skew-Hermitian parts. Similarly if G is a semisimple Lie group, then the 'Iwasawa decomposition' G = NAK exhibits closed subgroups A and N of G such that they are simply connected abelian and nilpotent respectively and A normalizes N and multiplication K ×A×N ! G is a diffeomorphism. -
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. -
Introduction to Representations Theory of Lie Groups
Introduction to Representations Theory of Lie Groups Raul Gomez October 14, 2009 Introduction The purpose of this notes is twofold. The first goal is to give a quick answer to the question \What is representation theory about?" To answer this, we will show by examples what are the most important results of this theory, and the problems that it is trying to solve. To make the answer short we will not develop all the formal details of the theory and we will give preference to examples over proofs. Few results will be proved, and in the ones were a proof is given, we will skip the technical details. We hope that the examples and arguments presented here will be enough to give the reader and intuitive but concise idea of the covered material. The second goal of the notes is to be a guide to the reader interested in starting a serious study of representation theory. Sometimes, when starting the study of a new subject, it's hard to understand the underlying motivation of all the abstract definitions and technical lemmas. It's also hard to know what is the ultimate goal of the subject and to identify the important results in the sea of technical lemmas. We hope that after reading this notes, the interested reader could start a serious study of representation theory with a clear idea of its goals and philosophy. Lets talk now about the material covered on this notes. In the first section we will state the celebrated Peter-Weyl theorem, which can be considered as a generalization of the theory of Fourier analysis on the circle S1.