Lie Groups and Representations Spring 2021
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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, . -
Lie Algebras Associated with Generalized Cartan Matrices
LIE ALGEBRAS ASSOCIATED WITH GENERALIZED CARTAN MATRICES BY R. V. MOODY1 Communicated by Charles W. Curtis, October 3, 1966 1. Introduction. If 8 is a finite-dimensional split semisimple Lie algebra of rank n over a field $ of characteristic zero, then there is associated with 8 a unique nXn integral matrix (Ay)—its Cartan matrix—which has the properties Ml. An = 2, i = 1, • • • , n, M2. M3. Ay = 0, implies An = 0. These properties do not, however, characterize Cartan matrices. If (Ay) is a Cartan matrix, it is known (see, for example, [4, pp. VI-19-26]) that the corresponding Lie algebra, 8, may be recon structed as follows: Let e y fy hy i = l, • • • , n, be any Zn symbols. Then 8 is isomorphic to the Lie algebra 8 ((A y)) over 5 defined by the relations Ml = 0, bifj] = dyhy If or all i and j [eihj] = Ajid [f*,] = ~A„fy\ «<(ad ej)-A>'i+l = 0,1 /,(ad fà-W = (J\ii i 7* j. In this note, we describe some results about the Lie algebras 2((Ay)) when (Ay) is an integral square matrix satisfying Ml, M2, and M3 but is not necessarily a Cartan matrix. In particular, when the further condition of §3 is imposed on the matrix, we obtain a reasonable (but by no means complete) structure theory for 8(04t/)). 2. Preliminaries. In this note, * will always denote a field of char acteristic zero. An integral square matrix satisfying Ml, M2, and M3 will be called a generalized Cartan matrix, or g.c.m. -
Hyperbolic Weyl Groups and the Four Normed Division Algebras
Hyperbolic Weyl Groups and the Four Normed Division Algebras Alex Feingold1, Axel Kleinschmidt2, Hermann Nicolai3 1 Department of Mathematical Sciences, State University of New York Binghamton, New York 13902–6000, U.S.A. 2 Physique Theorique´ et Mathematique,´ Universite´ Libre de Bruxelles & International Solvay Institutes, Boulevard du Triomphe, ULB – CP 231, B-1050 Bruxelles, Belgium 3 Max-Planck-Institut fur¨ Gravitationsphysik, Albert-Einstein-Institut Am Muhlenberg¨ 1, D-14476 Potsdam, Germany – p. Introduction Presented at Illinois State University, July 7-11, 2008 Vertex Operator Algebras and Related Areas Conference in Honor of Geoffrey Mason’s 60th Birthday – p. Introduction Presented at Illinois State University, July 7-11, 2008 Vertex Operator Algebras and Related Areas Conference in Honor of Geoffrey Mason’s 60th Birthday – p. Introduction Presented at Illinois State University, July 7-11, 2008 Vertex Operator Algebras and Related Areas Conference in Honor of Geoffrey Mason’s 60th Birthday “The mathematical universe is inhabited not only by important species but also by interesting individuals” – C. L. Siegel – p. Introduction (I) In 1983 Feingold and Frenkel studied the rank 3 hyperbolic Kac–Moody algebra = A++ with F 1 y y @ y Dynkin diagram @ 1 0 1 − Weyl Group W ( )= w , w , w wI = 2, wI wJ = mIJ F h 1 2 3 || | | | i 2 1 0 − 2(αI , αJ ) Cartan matrix [AIJ ]= 1 2 2 = − − (αJ , αJ ) 0 2 2 − 2 3 2 Coxeter exponents [mIJ ]= 3 2 ∞ 2 2 ∞ – p. Introduction (II) The simple roots, α 1, α0, α1, span the − 1 Root lattice Λ( )= α = nI αI n 1,n0,n1 Z F − ∈ ( I= 1 ) X− – p. -
Semisimple Q-Algebras in Algebraic Combinatorics
Semisimple Q-algebras in algebraic combinatorics Allen Herman (Regina) Group Ring Day, ICTS Bangalore October 21, 2019 I.1 Coherent Algebras and Association Schemes Definition 1 (D. Higman 1987). A coherent algebra (CA) is a subalgebra CB of Mn(C) defined by a special basis B, which is a collection of non-overlapping 01-matrices that (1) is a closed set under the transpose, (2) sums to J, the n × n all 1's matrix, and (3) contains a subset ∆ of diagonal matrices summing I , the identity matrix. The standard basis B of a CA in Mn(C) is precisely the set of adjacency matrices of a coherent configuration (CC) of order n and rank r = jBj. > B = B =) CB is semisimple. When ∆ = fI g, B is the set of adjacency matrices of an association scheme (AS). Allen Herman (Regina) Semisimple Q-algebras in Algebraic Combinatorics I.2 Example: Basic matrix of an AS An AS or CC can be illustrated by its basic matrix. Here we give the basic matrix of an AS with standard basis B = fb0; b1; :::; b7g: 2 012344556677 3 6 103244556677 7 6 7 6 230166774455 7 6 7 6 321066774455 7 6 7 6 447701665523 7 6 7 d 6 7 X 6 447710665532 7 ibi = 6 7 6 556677012344 7 i=0 6 7 6 556677103244 7 6 7 6 774455230166 7 6 7 6 774455321066 7 6 7 4 665523447701 5 665532447710 Allen Herman (Regina) Semisimple Q-algebras in Algebraic Combinatorics I.3 Example: Basic matrix of a CC of order 10 and j∆j = 2 2 0 123232323 3 6 1 032323232 7 6 7 6 4567878787 7 6 7 6 5476787878 7 d 6 7 X 6 4587678787 7 ibi = 6 7 6 5478767878 7 i=0 6 7 6 4587876787 7 6 7 6 5478787678 7 6 7 4 4587878767 5 5478787876 ∆ = fb0; b6g, δ(b0) = δ(b6) = 1 Diagonal block valencies: δ(b1) = 1, δ(b7) = 4, δ(b8) = 3; Off diagonal block valencies: row valencies: δr (b2) = δr (b3) = 4, δr (b4) = δr (b5) = 1 column valencies: δc (b2) = δc (b3) = 1, δc (b4) = δc (b5) = 4. -
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. -
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. -
Completely Integrable Gradient Flows
Commun. Math. Phys. 147, 57-74 (1992) Communications in Maltlematical Physics Springer-Verlag 1992 Completely Integrable Gradient Flows Anthony M. Bloch 1'*, Roger W. Brockett 2'** and Tudor S. Ratiu 3'*** 1 Department of Mathematics, The Ohio State University, Columbus, OH 43210, USA z Division of Applied Sciences, Harvard University, Cambridge, MA 02138, USA 3 Department of Mathematics, University of California, Santa Cruz, CA 95064, USA Received December 6, 1990, in revised form July 11, 1991 Abstract. In this paper we exhibit the Toda lattice equations in a double bracket form which shows they are gradient flow equations (on their isospectral set) on an adjoint orbit of a compact Lie group. Representations for the flows are given and a convexity result associated with a momentum map is proved. Some general properties of the double bracket equations are demonstrated, including a discussion of their invariant subspaces, and their function as a Lie algebraic sorter. O. Introduction In this paper we present details of the proofs and applications of the results on the generalized Toda lattice equations announced in [7]. One of our key results is exhibiting the Toda equations in a double bracket form which shows directly that they are gradient flow equations (on their isospectral set) on an adjoint orbit of a compact Lie group. This system, which is gradient with respect to the normal metric on the orbit, is quite different from the repre- sentation of the Toda flow as a gradient system on N" in Moser's fundamental paper [27]. In our representation the same set of equations is thus Hamiltonian and a gradient flow on the isospectral set. -
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. -
Symmetries, Fields and Particles. Examples 1
Michaelmas Term 2016, Mathematical Tripos Part III Prof. N. Dorey Symmetries, Fields and Particles. Examples 1. 1. O(n) consists of n × n real matrices M satisfying M T M = I. Check that O(n) is a group. U(n) consists of n × n complex matrices U satisfying U†U = I. Check similarly that U(n) is a group. Verify that O(n) and SO(n) are the subgroups of real matrices in, respectively, U(n) and SU(n). By considering how U(n) matrices act on vectors in Cn, and identifying Cn with R2n, show that U(n) is a subgroup of SO(2n). 2. Show that for matrices M ∈ O(n), the first column of M is an arbitrary unit vector, the second is a unit vector orthogonal to the first, ..., the kth column is a unit vector orthogonal to the span of the previous ones, etc. Deduce the dimension of O(n). By similar reasoning, determine the dimension of U(n). Show that any column of a unitary matrix U is not in the (complex) linear span of the remaining columns. 3. Consider the real 3 × 3 matrix, R(n,θ)ij = cos θδij + (1 − cos θ)ninj − sin θǫijknk 3 where n = (n1, n2, n3) is a unit vector in R . Verify that n is an eigenvector of R(n,θ) with eigenvalue one. Now choose an orthonormal basis for R3 with basis vectors {n, m, m˜ } satisfying, m · m = 1, m · n = 0, m˜ = n × m. By considering the action of R(n,θ) on these basis vectors show that this matrix corre- sponds to a rotation through an angle θ about an axis parallel to n and check that it is an element of SO(3). -
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. -
From Root Systems to Dynkin Diagrams
From root systems to Dynkin diagrams Heiko Dietrich Abstract. We describe root systems and their associated Dynkin diagrams; these notes follow closely the book of Erdman & Wildon (\Introduction to Lie algebras", 2006) and lecture notes of Willem de Graaf (Italy). We briefly describe how root systems arise from Lie algebras. 1. Root systems 1.1. Euclidean spaces. Let V be a finite dimensional Euclidean space, that is, a finite dimensional R-space with inner product ( ; ): V V R, which is bilinear, symmetric, and − − p× ! positive definite. The length of v V is v = (v; v); the angle α between two non-zero 2 jj jj v; w V is defined by cos α = (v;w) . 2 jjvjjjjwjj If v V is non-zero, then the hyperplane perpendicular to v is Hv = w V (w; v) = 0 . 2 f 2 j g The reflection in Hv is the linear map sv : V V which maps v to v and fixes every w Hv; ! − 2 recall that V = Hv Span (v), hence ⊕ R 2(w; v) sv : V V; w w v: ! 7! − (v; v) In the following, for v; w V we write 2 2(w; v) w; v = ; h i (v; v) note that ; is linear only in the first component. An important observation is that each h− −i su leaves the inner product invariant, that is, if v; w V , then (su(v); su(w)) = (v; w). 2 We use this notation throughout these notes. 1.2. Abstract root systems. Definition 1.1. A finite subset Φ V is a root system for V if the following hold: ⊆ (R1)0 = Φ and Span (Φ) = V , 2 R (R2) if α Φ and λα Φ with λ R, then λ 1 , 2 2 2 2 {± g (R3) sα(β) Φ for all α; β Φ, 2 2 (R4) α; β Z for all α; β Φ. -
The Waldspurger Transform of Permutations and Alternating Sign Matrices
Séminaire Lotharingien de Combinatoire 78B (2017) Proceedings of the 29th Conference on Formal Power Article #41, 12 pp. Series and Algebraic Combinatorics (London) The Waldspurger Transform of Permutations and Alternating Sign Matrices Drew Armstrong∗ and James McKeown Department of Mathematics, University of Miami, Coral Gables, FL Abstract. In 2005 J. L. Waldspurger proved the following theorem: Given a finite real reflection group G, the closed positive root cone is tiled by the images of the open weight cone under the action of the linear transformations 1 g. Shortly after this − E. Meinrenken extended the result to affine Weyl groups and then P. V. Bibikov and V. S. Zhgoon gave a uniform proof for a discrete reflection group acting on a simply- connected space of constant curvature. In this paper we show that the Waldspurger and Meinrenken theorems of type A give an interesting new perspective on the combinatorics of the symmetric group. In particular, for each permutation matrix g S we define a non-negative integer 2 n matrix WT(g), called the Waldspurger transform of g. The definition of the matrix WT(g) is purely combinatorial but it turns out that its columns are the images of the fundamental weights under 1 g, expressed in simple root coordinates. The possible − columns of WT(g) (which we call UM vectors) biject to many interesting structures including: unimodal Motzkin paths, abelian ideals in the Lie algebra sln(C), Young diagrams with maximum hook length n, and integer points inside a certain polytope. We show that the sum of the entries of WT(g) is half the entropy of the corresponding permutation g, which is known to equal the rank of g in the MacNeille completion of the Bruhat order.