Algebraic Groups Lecture Notes
Total Page:16
File Type:pdf, Size:1020Kb

Load more
Recommended publications
-
Mathematics 1
Mathematics 1 MAA 4103 Introduction to Advanced Calculus for Engineers and Physical MATHEMATICS Scientists 2 3 Credits Grading Scheme: Letter Grade Not all courses are offered every semester. Refer to the schedule of Continues the advanced calculus for engineers and physical scientists courses for each term's specific offerings. sequence. Theory of integration, transcendental functions and infinite More Info (http://registrar.ufl.edu/soc/) series. MAA 4102 is not recommended for those who plan to do graduate work in mathematics; these students should take MAA 4212. Credit will Unless otherwise indicated in the course description, all courses at the be given for, at most, one of MAA 4103, MAA 4212 and MAA 5105. University of Florida are taught in English, with the exception of specific Prerequisite: MAA 4102 with minimum grade of C. foreign language courses. MAA 4211 Advanced Calculus 1 3 Credits Department Information Grading Scheme: Letter Grade Advanced treatment of limits, differentiation, integration and series. Graduates from the Department of Mathematics might take a job Includes calculus of functions of several variables. Credit will be given for, that uses their math major in an area like statistics, biomathematics, at most, one of MAA 4211, MAA 4102 and MAA 5104. operations research, actuarial science, mathematical modeling, Prerequisite: MAS 4105 with minimum grade of C. cryptography, or mathematics education. Or they might continue into graduate school leading to a research career. Professional schools in MAA 4212 Advanced Calculus 2 3 Credits business, law, and medicine appreciate mathematics majors because of Grading Scheme: Letter Grade the analytical and problem solving skills developed in the math courses. -
The Jouanolou-Thomason Homotopy Lemma
The Jouanolou-Thomason homotopy lemma Aravind Asok February 9, 2009 1 Introduction The goal of this note is to prove what is now known as the Jouanolou-Thomason homotopy lemma or simply \Jouanolou's trick." Our main reason for discussing this here is that i) most statements (that I have seen) assume unncessary quasi-projectivity hypotheses, and ii) most applications of the result that I know (e.g., in homotopy K-theory) appeal to the result as merely a \black box," while the proof indicates that the construction is quite geometric and relatively explicit. For simplicity, throughout the word scheme means separated Noetherian scheme. Theorem 1.1 (Jouanolou-Thomason homotopy lemma). Given a smooth scheme X over a regular Noetherian base ring k, there exists a pair (X;~ π), where X~ is an affine scheme, smooth over k, and π : X~ ! X is a Zariski locally trivial smooth morphism with fibers isomorphic to affine spaces. 1 Remark 1.2. In terms of an A -homotopy category of smooth schemes over k (e.g., H(k) or H´et(k); see [MV99, x3]), the map π is an A1-weak equivalence (use [MV99, x3 Example 2.4]. Thus, up to A1-weak equivalence, any smooth k-scheme is an affine scheme smooth over k. 2 An explicit algebraic form Let An denote affine space over Spec Z. Let An n 0 denote the scheme quasi-affine and smooth over 2m Spec Z obtained by removing the fiber over 0. Let Q2m−1 denote the closed subscheme of A (with coordinates x1; : : : ; x2m) defined by the equation X xixm+i = 1: i Consider the following simple situation. -
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]). -
Affine Reflection Group Codes
Affine Reflection Group Codes Terasan Niyomsataya1, Ali Miri1,2 and Monica Nevins2 School of Information Technology and Engineering (SITE)1 Department of Mathematics and Statistics2 University of Ottawa, Ottawa, Canada K1N 6N5 email: {tniyomsa,samiri}@site.uottawa.ca, [email protected] Abstract This paper presents a construction of Slepian group codes from affine reflection groups. The solution to the initial vector and nearest distance problem is presented for all irreducible affine reflection groups of rank n ≥ 2, for varying stabilizer subgroups. Moreover, we use a detailed analysis of the geometry of affine reflection groups to produce an efficient decoding algorithm which is equivalent to the maximum-likelihood decoder. Its complexity depends only on the dimension of the vector space containing the codewords, and not on the number of codewords. We give several examples of the decoding algorithm, both to demonstrate its correctness and to show how, in small rank cases, it may be further streamlined by exploiting additional symmetries of the group. 1 1 Introduction Slepian [11] introduced group codes whose codewords represent a finite set of signals combining coding and modulation, for the Gaussian channel. A thorough survey of group codes can be found in [8]. The codewords lie on a sphere in n−dimensional Euclidean space Rn with equal nearest-neighbour distances. This gives congruent maximum-likelihood (ML) decoding regions, and hence equal error probability, for all codewords. Given a group G with a representation (action) on Rn, that is, an 1Keywords: Group codes, initial vector problem, decoding schemes, affine reflection groups 1 orthogonal n × n matrix Og for each g ∈ G, a group code generated from G is given by the set of all cg = Ogx0 (1) n for all g ∈ G where x0 = (x1, . -
Hopf Rings in Algebraic Topology
HOPF RINGS IN ALGEBRAIC TOPOLOGY W. STEPHEN WILSON Abstract. These are colloquium style lecture notes about Hopf rings in al- gebraic topology. They were designed for use by non-topologists and graduate students but have been found helpful for those who want to start learning about Hopf rings. They are not “up to date,” nor are then intended to be, but instead they are intended to be introductory in nature. Although these are “old” notes, Hopf rings are thriving and these notes give a relatively painless introduction which should prepare the reader to approach the current litera- ture. This is a brief survey about Hopf rings: what they are, how they arise, examples, and how to compute them. There are very few proofs. The bulk of the technical details can be found in either [RW77] or [Wil82], but a “soft” introduction to the material is difficult to find. Historically, Hopf algebras go back to the early days of our subject matter, homotopy theory and algebraic topology. They arise naturally from the homology of spaces with multiplications on them, i.e. H-spaces, or “Hopf” spaces. In our language, this homology is a group object in the category of coalgebras. Hopf algebras have become objects of study in their own right, e.g. [MM65] and [Swe69]. They were also able to give great insight into complicated structures such as with Milnor’s work on the Steenrod algebra [Mil58]. However, when spaces have more structure than just a multiplication, their homology produces even richer algebraic stuctures. In particular, with the development of generalized cohomology theories, we have seen that the spaces which classify them have a structure mimicking that of a graded ring. -
The Tate–Oort Group Scheme Top
The Tate{Oort group scheme TOp Miles Reid In memory of Igor Rostislavovich Shafarevich, from whom we have all learned so much Abstract Over an algebraically closed field of characteristic p, there are 3 group schemes of order p, namely the ordinary cyclic group Z=p, the multiplicative group µp ⊂ Gm and the additive group αp ⊂ Ga. The Tate{Oort group scheme TOp of [TO] puts these into one happy fam- ily, together with the cyclic group of order p in characteristic zero. This paper studies a simplified form of TOp, focusing on its repre- sentation theory and basic applications in geometry. A final section describes more substantial applications to varieties having p-torsion in Picτ , notably the 5-torsion Godeaux surfaces and Calabi{Yau 3-folds obtained from TO5-invariant quintics. Contents 1 Introduction 2 1.1 Background . 3 1.2 Philosophical principle . 4 2 Hybrid additive-multiplicative group 5 2.1 The algebraic group G ...................... 5 2.2 The given representation (B⊕2)_ of G .............. 6 d ⊕2 _ 2.3 Symmetric power Ud = Sym ((B ) ).............. 6 1 3 Construction of TOp 9 3.1 Group TOp in characteristic p .................. 9 3.2 Group TOp in mixed characteristic . 10 3.3 Representation theory of TOp . 12 _ 4 The Cartier dual (TOp) 12 4.1 Cartier duality . 12 4.2 Notation . 14 4.3 The algebra structure β : A_ ⊗ A_ ! A_ . 14 4.4 The Hopf algebra structure δ : A_ ! A_ ⊗ A_ . 16 5 Geometric applications 19 5.1 Background . 20 2 5.2 Plane cubics C3 ⊂ P with free TO3 action . -
Algebra & Number Theory
Algebra & Number Theory Volume 7 2013 No. 7 Hopf monoids from class functions on unitriangular matrices Marcelo Aguiar, Nantel Bergeron and Nathaniel Thiem msp ALGEBRA AND NUMBER THEORY 7:7 (2013) msp dx.doi.org/10.2140/ant.2013.7.1743 Hopf monoids from class functions on unitriangular matrices Marcelo Aguiar, Nantel Bergeron and Nathaniel Thiem We build, from the collection of all groups of unitriangular matrices, Hopf monoids in Joyal’s category of species. Such structure is carried by the collection of class function spaces on those groups and also by the collection of superclass function spaces in the sense of Diaconis and Isaacs. Superclasses of unitriangular matrices admit a simple description from which we deduce a combinatorial model for the Hopf monoid of superclass functions in terms of the Hadamard product of the Hopf monoids of linear orders and of set partitions. This implies a recent result relating the Hopf algebra of superclass functions on unitriangular matrices to symmetric functions in noncommuting variables. We determine the algebraic structure of the Hopf monoid: it is a free monoid in species with the canonical Hopf structure. As an application, we derive certain estimates on the number of conjugacy classes of unitriangular matrices. Introduction A Hopf monoid (in Joyal’s category of species) is an algebraic structure akin to that of a Hopf algebra. Combinatorial structures that compose and decompose give rise to Hopf monoids. These objects are the subject of[Aguiar and Mahajan 2010, Part II]. The few basic notions and examples needed for our purposes are reviewed in Section 1, including the Hopf monoids of linear orders, set partitions, and simple graphs and the Hadamard product of Hopf monoids. -
Feature Matching and Heat Flow in Centro-Affine Geometry
Symmetry, Integrability and Geometry: Methods and Applications SIGMA 16 (2020), 093, 22 pages Feature Matching and Heat Flow in Centro-Affine Geometry Peter J. OLVER y, Changzheng QU z and Yun YANG x y School of Mathematics, University of Minnesota, Minneapolis, MN 55455, USA E-mail: [email protected] URL: http://www.math.umn.edu/~olver/ z School of Mathematics and Statistics, Ningbo University, Ningbo 315211, P.R. China E-mail: [email protected] x Department of Mathematics, Northeastern University, Shenyang, 110819, P.R. China E-mail: [email protected] Received April 02, 2020, in final form September 14, 2020; Published online September 29, 2020 https://doi.org/10.3842/SIGMA.2020.093 Abstract. In this paper, we study the differential invariants and the invariant heat flow in centro-affine geometry, proving that the latter is equivalent to the inviscid Burgers' equa- tion. Furthermore, we apply the centro-affine invariants to develop an invariant algorithm to match features of objects appearing in images. We show that the resulting algorithm com- pares favorably with the widely applied scale-invariant feature transform (SIFT), speeded up robust features (SURF), and affine-SIFT (ASIFT) methods. Key words: centro-affine geometry; equivariant moving frames; heat flow; inviscid Burgers' equation; differential invariant; edge matching 2020 Mathematics Subject Classification: 53A15; 53A55 1 Introduction The main objective in this paper is to study differential invariants and invariant curve flows { in particular the heat flow { in centro-affine geometry. In addition, we will present some basic applications to feature matching in camera images of three-dimensional objects, comparing our method with other popular algorithms. -
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]. -
The Affine Group of a Lie Group
THE AFFINE GROUP OF A LIE GROUP JOSEPH A. WOLF1 1. If G is a Lie group, then the group Aut(G) of all continuous auto- morphisms of G has a natural Lie group structure. This gives the semi- direct product A(G) = G-Aut(G) the structure of a Lie group. When G is a vector group R", A(G) is the ordinary affine group A(re). Follow- ing L. Auslander [l ] we will refer to A(G) as the affine group of G, and regard it as a transformation group on G by (g, a): h-^g-a(h) where g, hEG and aGAut(G) ; in the case of a vector group, this is the usual action on A(») on R". If B is a compact subgroup of A(n), then it is well known that B has a fixed point on R", i.e., that there is a point xGR" such that b(x)=x for every bEB. For A(ra) is contained in the general linear group GL(« + 1, R) in the usual fashion, and B (being compact) must be conjugate to a subgroup of the orthogonal group 0(w + l). This conjugation can be done leaving fixed the (« + 1, w + 1)-place matrix entries, and is thus possible by an element of k(n). This done, the translation-parts of elements of B must be zero, proving the assertion. L. Auslander [l] has extended this theorem to compact abelian subgroups of A(G) when G is connected, simply connected and nil- potent. We will give a further extension. -
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)). -
Map Composition Generalized to Coherent Collections of Maps
Front. Math. China 2015, 10(3): 547–565 DOI 10.1007/s11464-015-0435-5 Map composition generalized to coherent collections of maps Herng Yi CHENG1, Kang Hao CHEONG1,2 1 National University of Singapore High School of Mathematics and Science, Singapore 129957, Singapore 2 Tanglin Secondary School, Singapore 127391, Singapore c Higher Education Press and Springer-Verlag Berlin Heidelberg 2015 Abstract Relation algebras give rise to partial algebras on maps, which are generalized to partial algebras on polymaps while preserving the properties of relation union and composition. A polymap is defined as a map with every point in the domain associated with a special set of maps. Polymaps can be represented as small subcategories of Set∗, the category of pointed sets. Map composition and the counterpart of relation union for maps are generalized to polymap composition and sum. Algebraic structures and categories of polymaps are investigated. Polymaps present the unique perspective of an algebra that can retain many of its properties when its elements (maps) are augmented with collections of other elements. Keywords Relation algebra, partial algebra, composition MSC 08A02 1 Introduction This paper considers partial algebras on maps (similar to those defined in [15]), constructed in analogy to relation algebras [5,12,16]. The sum of two maps f0 : X0 → Y0 and f1 : X1 → Y1 is defined if the union of their graphs is a functional binary relation R ⊆ (X0 ∪ X1) × (Y0 ∪ Y1), in which case the sum is the map (f0 + f1): X0 ∪ X1 → Y0 ∪ Y1 with graph R. This is defined similarly to the union operation + from [10].