Computation of Weyl Groups of G-Varieties
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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. -
Some Groups of Finite Homological Type
Some groups of finite homological type Ian J. Leary∗ M¨ugeSaadeto˘glu† June 10, 2005 Abstract For each n ≥ 0 we construct a torsion-free group that satisfies K. S. Brown’s FHT condition and is FPn, but is not FPn+1. 1 Introduction While working on comparing different notions of Euler characteristic, K. S. Brown introduced a new homological finiteness condition for discrete groups [5, IX.6]. The group G is said to be of finite homological type or FHT if G has finite virtual cohomological dimension, and for every G-module M whose underlying abelian group is finitely generated, the homology groups Hi(G; M) are all finitely generated. If G is FHT , then one may define a ‘na¨ıve Euler characteristic’ for every finite-index subgroup H of G, as the alternating sum of the dimensions of the homology groups of H with rational coefficients. One question that arises is the connection between FHT and the usual homological finiteness conditions FP and FPn, which were introduced by J.-P. Serre [8]. (We shall define these conditions below.) It is easy to see that any group G of type FP is FHT , and one might conjecture that every torsion-free group that is FHT is also of type FP . The aim of this paper is to show that this is not the case. For each n ≥ 0, we exhibit a torsion-free group Gn that is FHT and of type FPn, but that is not of type FPn+1. Our construction is based on R. Bieri’s construction of a group that is FPn but not FPn+1 [2, Prop 2.14]. -
A Theorem on Discrete Groups and Some Consequences of Kazdan's
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector JOURNAL OF FUNCTIONAL ANALYSIS 6, 203-207 (1970) A Theorem on Discrete Groups and Some Consequences of Kazdan’s Thesis ROBERT R. KALLMAN* Department of Mathematics, Yale University, New Haven, Connecticut 06520 Communicated by Irving Segal Received June 21, 1969 Let G be a noncompact simple Lie group, and let r be a discrete subgroup of G such that G/P has finite volume. The main result of this paper is that the left ring of P is a Type II1 von Neumann algebra. This result in turn is applied to solve, in some generality, a problem in dynamical systems posed by I. M. Gelfand. INTRODUCTION If G is a locally compact unimodular group, let Y(G) be the von Neumann algebra generated by left translations L(a) (a in G) on L2(G). Let I’ be a discrete subgroup of G, and let p be a measure on G/r which is invariant under the natural action of G. The measure class of p is uniquely determined. If f is in L2(G/F), let (V4f)W = flu-’ - 4. The following problem is of interest in dynamical systems (cf. Gelfand [3]). Let &?(G, r) be the von Neumann algebra on L2(G) @ L2(G/.F) generated by L(a) @ V(u) (u in G) and I @ M(4) (here 4 is in L”(G/r, p) and (&Z(+)f)(x) = ~$(x)f(x), for all f in L2(G/r)). -
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. -
Discrete Groups and Simple C*-Algebras 1 Introduction
Discrete groups and simple C*-algebras by Erik Bedos* Department of Mathematics University of Oslo P.O.Box 1053, Blindern 0316 Oslo 3, Norway 1 Introduction Let G denote a discrete group and let us say that G is C* -simple if the reduced group C* -algebra associated with G is simple. We notice im mediately that there is no interest in considering here the full group C* algebra associated with G, because it is simple if and only if G is trivial. Since Powers in 1975 ([26]) proved that all non-abelian free groups are C* simple, the class of C* -simple groups has been considerably enlarged (see [1,2,6,7,12,13,14,16,24] as a sample!), and two important subclasses are the so-called weak Powers groups ([6,13]; see section 4 for definition and ex amples) and the groups of Akemann-Lee type ([1,2]), which are groups possessing a normal non-abelian free subgroup with trivial centralizer. The problem of giving an intrisic characterization of C* -simple groups is still open. It is known that a C* -simple group has no normal amenable subgroup other than the trivial one ([24; proposition 1.6]) and is ICC (since the center of the associated reduced group C* -algebra must be the scalars). One may of course wonder if the converse is true. On the other hand, most C* -simple groups are known to have a unique trace, i.e. the canonical trace on the reduced group C* -algebra· is unique, which naturally raises the problem whether this is always true or not ([13; §2, question (2)]). -
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. -
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. -
Introduction to Affine Grassmannians
Introduction to Affine Grassmannians Sara Billey University of Washington http://www.math.washington.edu/∼billey Connections for Women: Algebraic Geometry and Related Fields January 23, 2009 0-0 Philosophy “Combinatorics is the equivalent of nanotechnology in mathematics.” 0-1 Outline 1. Background and history of Grassmannians 2. Schur functions 3. Background and history of Affine Grassmannians 4. Strong Schur functions and k-Schur functions 5. The Big Picture New results based on joint work with • Steve Mitchell (University of Washington) arXiv:0712.2871, 0803.3647 • Sami Assaf (MIT), preprint coming soon! 0-2 Enumerative Geometry Approximately 150 years ago. Grassmann, Schubert, Pieri, Giambelli, Severi, and others began the study of enumerative geometry. Early questions: • What is the dimension of the intersection between two general lines in R2? • How many lines intersect two given lines and a given point in R3? • How many lines intersect four given lines in R3 ? Modern questions: • How many points are in the intersection of 2,3,4,. Schubert varieties in general position? 0-3 Schubert Varieties A Schubert variety is a member of a family of projective varieties which is defined as the closure of some orbit under a group action in a homogeneous space G/H. Typical properties: • They are all Cohen-Macaulay, some are “mildly” singular. • They have a nice torus action with isolated fixed points. • This family of varieties and their fixed points are indexed by combinatorial objects; e.g. partitions, permutations, or Weyl group elements. 0-4 Schubert Varieties “Honey, Where are my Schubert varieties?” Typical contexts: • The Grassmannian Manifold, G(n, d) = GLn/P . -
Discreteness Properties of Translation Numbers in Solvable Groups
DISCRETENESS PROPERTIES OF TRANSLATION NUMBERS IN SOLVABLE GROUPS GREGORY R. CONNER Abstract. We define a group to be translation proper if it carries a left- invariant metric in which the translation numbers of the non-torsion elements are nonzero and translation discrete if they are bounded away from zero. The main results of this paper are that a translation proper solvable group of finite virtual cohomological dimension is metabelian-by-finite, and that a translation discrete solvable group of finite virtual cohomological dimension, m, is a finite m extension of Z . 1. Introduction The notion of a translation number comes from Riemannian geometry. Suppose M is a compact Riemannian manifold of nonpositive sectional curvature and Mf is its universal cover, enjoying the metric induced from M. Then the covering transformation group acts as isometries on Mf. Under these conditions any covering transformation of Mf fixes a geodesic line. Since a geodesic line is isometric to R, a covering transformation must translate each point of such a fixed geodesic line by a constant amount which is called the translation number of the covering transformation. This notion can be abstracted. Let G be a group which is equipped with a metric, d, which is invariant under left multiplication by elements of G, i.e., d(xy, xz)=d(y,z) ∀ x, y, z ∈ G. We then say that d is a left-invariant group metric k k (or a metric for brevity) on G. Let kk: G −→ Z be defined by x = d(x, 1G). To fix ideas, one may consider a finitely generated group equipped with a word metric. -
3.4 Discrete Groups
3.4 Discrete groups Lemma 3.4.1. Let Λ be a subgroup of R2, and let ~a;~b be two elements of Λ that are linearly independent as vectors in R2. Suppose that the paralleogram spanned by ~a and ~b contains no other elements of Λ other than ~0;~a;~b and ~a +~b. Then Λ is the group Λ = fm~a + n~b j m; n 2 Zg: (3.4) Proof. The plane is tiled up with copies of the parallellogram P spanned by the four vectors ~0;~a;~b;~a+~b. The vertices of these parallellograms are m~a+n~b for some integers m and n. Since Λ is a group all these vertices are in Λ. If Λ is not the group fm~a + n~b j m; n 2 Zg, then there exists an element x 2 Λ not in located at any of the vertices of the parallellograms. Since these parallellograms tile the whole plane there exist m and n such that x is contained in the parallellogram m~a + n~b; (m + 1)~a + n~b; m~a + (n + 1)~b and (m + 1)~a + (n + 1)~b. The element x0 = x − m~a − n~b is in the group Λ, and in the first paralleogram P . By assumption x0 is one of the four vertices of P , and it follows that also x is an vertex of the parallellograms. Hence Λ is the group fm~a + n~b j m; n 2 Zg. Definition 3.4.2. A subgroup Λ of R2 is called a lattice if there exists an > 0 such that every non-zero element ~a 2 Λ has length j~aj > .