Concerning the Linear Action of Discrete Subgroups of SL(2,R) on the Plane
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ORTHOGONAL GROUP of CERTAIN INDEFINITE LATTICE Chang Heon Kim* 1. Introduction Given an Even Lattice M in a Real Quadratic Space
JOURNAL OF THE CHUNGCHEONG MATHEMATICAL SOCIETY Volume 20, No. 1, March 2007 ORTHOGONAL GROUP OF CERTAIN INDEFINITE LATTICE Chang Heon Kim* Abstract. We compute the special orthogonal group of certain lattice of signature (2; 1). 1. Introduction Given an even lattice M in a real quadratic space of signature (2; n), Borcherds lifting [1] gives a multiplicative correspondence between vec- tor valued modular forms F of weight 1¡n=2 with values in C[M 0=M] (= the group ring of M 0=M) and meromorphic modular forms on complex 0 varieties (O(2) £ O(n))nO(2; n)=Aut(M; F ). Here NM denotes the dual lattice of M, O(2; n) is the orthogonal group of M R and Aut(M; F ) is the subgroup of Aut(M) leaving the form F stable under the natural action of Aut(M) on M 0=M. In particular, if the signature of M is (2; 1), then O(2; 1) ¼ H: O(2) £ O(1) and Borcherds' theory gives a lifting of vector valued modular form of weight 1=2 to usual one variable modular form on Aut(M; F ). In this sense in order to work out Borcherds lifting it is important to ¯nd appropriate lattice on which our wanted modular group acts. In this article we will show: Theorem 1.1. Let M be a 3-dimensional even lattice of all 2 £ 2 integral symmetric matrices, that is, ½µ ¶ ¾ AB M = j A; B; C 2 Z BC Received December 30, 2006. 2000 Mathematics Subject Classi¯cation: Primary 11F03, 11H56. -
ON the SHELLABILITY of the ORDER COMPLEX of the SUBGROUP LATTICE of a FINITE GROUP 1. Introduction We Will Show That the Order C
TRANSACTIONS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 353, Number 7, Pages 2689{2703 S 0002-9947(01)02730-1 Article electronically published on March 12, 2001 ON THE SHELLABILITY OF THE ORDER COMPLEX OF THE SUBGROUP LATTICE OF A FINITE GROUP JOHN SHARESHIAN Abstract. We show that the order complex of the subgroup lattice of a finite group G is nonpure shellable if and only if G is solvable. A by-product of the proof that nonsolvable groups do not have shellable subgroup lattices is the determination of the homotopy types of the order complexes of the subgroup lattices of many minimal simple groups. 1. Introduction We will show that the order complex of the subgroup lattice of a finite group G is (nonpure) shellable if and only if G is solvable. The proof of nonshellability in the nonsolvable case involves the determination of the homotopy type of the order complexes of the subgroup lattices of many minimal simple groups. We begin with some history and basic definitions. It is assumed that the reader is familiar with some of the rudiments of algebraic topology and finite group theory. No distinction will be made between an abstract simplicial complex ∆ and an arbitrary geometric realization of ∆. Maximal faces of a simplicial complex ∆ will be called facets of ∆. Definition 1.1. A simplicial complex ∆ is shellable if the facets of ∆ can be ordered σ1;::: ,σn so that for all 1 ≤ i<k≤ n thereexistssome1≤ j<kand x 2 σk such that σi \ σk ⊆ σj \ σk = σk nfxg. The list σ1;::: ,σn is called a shelling of ∆. -
7 LATTICE POINTS and LATTICE POLYTOPES Alexander Barvinok
7 LATTICE POINTS AND LATTICE POLYTOPES Alexander Barvinok INTRODUCTION Lattice polytopes arise naturally in algebraic geometry, analysis, combinatorics, computer science, number theory, optimization, probability and representation the- ory. They possess a rich structure arising from the interaction of algebraic, convex, analytic, and combinatorial properties. In this chapter, we concentrate on the the- ory of lattice polytopes and only sketch their numerous applications. We briefly discuss their role in optimization and polyhedral combinatorics (Section 7.1). In Section 7.2 we discuss the decision problem, the problem of finding whether a given polytope contains a lattice point. In Section 7.3 we address the counting problem, the problem of counting all lattice points in a given polytope. The asymptotic problem (Section 7.4) explores the behavior of the number of lattice points in a varying polytope (for example, if a dilation is applied to the polytope). Finally, in Section 7.5 we discuss problems with quantifiers. These problems are natural generalizations of the decision and counting problems. Whenever appropriate we address algorithmic issues. For general references in the area of computational complexity/algorithms see [AB09]. We summarize the computational complexity status of our problems in Table 7.0.1. TABLE 7.0.1 Computational complexity of basic problems. PROBLEM NAME BOUNDED DIMENSION UNBOUNDED DIMENSION Decision problem polynomial NP-hard Counting problem polynomial #P-hard Asymptotic problem polynomial #P-hard∗ Problems with quantifiers unknown; polynomial for ∀∃ ∗∗ NP-hard ∗ in bounded codimension, reduces polynomially to volume computation ∗∗ with no quantifier alternation, polynomial time 7.1 INTEGRAL POLYTOPES IN POLYHEDRAL COMBINATORICS We describe some combinatorial and computational properties of integral polytopes. -
INTEGER POINTS and THEIR ORTHOGONAL LATTICES 2 to Remove the Congruence Condition
INTEGER POINTS ON SPHERES AND THEIR ORTHOGONAL LATTICES MENNY AKA, MANFRED EINSIEDLER, AND URI SHAPIRA (WITH AN APPENDIX BY RUIXIANG ZHANG) Abstract. Linnik proved in the late 1950’s the equidistribution of in- teger points on large spheres under a congruence condition. The congru- ence condition was lifted in 1988 by Duke (building on a break-through by Iwaniec) using completely different techniques. We conjecture that this equidistribution result also extends to the pairs consisting of a vector on the sphere and the shape of the lattice in its orthogonal complement. We use a joining result for higher rank diagonalizable actions to obtain this conjecture under an additional congruence condition. 1. Introduction A theorem of Legendre, whose complete proof was given by Gauss in [Gau86], asserts that an integer D can be written as a sum of three squares if and only if D is not of the form 4m(8k + 7) for some m, k N. Let D = D N : D 0, 4, 7 mod8 and Z3 be the set of primitive∈ vectors { ∈ 6≡ } prim in Z3. Legendre’s Theorem also implies that the set 2 def 3 2 S (D) = v Zprim : v 2 = D n ∈ k k o is non-empty if and only if D D. This important result has been refined in many ways. We are interested∈ in the refinement known as Linnik’s problem. Let S2 def= x R3 : x = 1 . For a subset S of rational odd primes we ∈ k k2 set 2 D(S)= D D : for all p S, D mod p F× . -
Commensurators of Finitely Generated Non-Free Kleinian Groups. 1
Commensurators of finitely generated non-free Kleinian groups. C. LEININGER D. D. LONG A.W. REID We show that for any finitely generated torsion-free non-free Kleinian group of the first kind which is not a lattice and contains no parabolic elements, then its commensurator is discrete. 57M07 1 Introduction Let G be a group and Γ1; Γ2 < G. Γ1 and Γ2 are called commensurable if Γ1 \Γ2 has finite index in both Γ1 and Γ2 . The Commensurator of a subgroup Γ < G is defined to be: −1 CG(Γ) = fg 2 G : gΓg is commensurable with Γg: When G is a semi-simple Lie group, and Γ a lattice, a fundamental dichotomy es- tablished by Margulis [26], determines that CG(Γ) is dense in G if and only if Γ is arithmetic, and moreover, when Γ is non-arithmetic, CG(Γ) is again a lattice. Historically, the prominence of the commensurator was due in large part to its density in the arithmetic setting being closely related to the abundance of Hecke operators attached to arithmetic lattices. These operators are fundamental objects in the theory of automorphic forms associated to arithmetic lattices (see [38] for example). More recently, the commensurator of various classes of groups has come to the fore due to its growing role in geometry, topology and geometric group theory; for example in classifying lattices up to quasi-isometry, classifying graph manifolds up to quasi- isometry, and understanding Riemannian metrics admitting many “hidden symmetries” (for more on these and other topics see [2], [4], [17], [18], [25], [34] and [37]). -
Groups with Identical Subgroup Lattices in All Powers
GROUPS WITH IDENTICAL SUBGROUP LATTICES IN ALL POWERS KEITH A. KEARNES AND AGNES´ SZENDREI Abstract. Suppose that G and H are groups with cyclic Sylow subgroups. We show that if there is an isomorphism λ2 : Sub (G × G) ! Sub (H × H), then there k k are isomorphisms λk : Sub (G ) ! Sub (H ) for all k. But this is not enough to force G to be isomorphic to H, for we also show that for any positive integer N there are pairwise nonisomorphic groups G1; : : : ; GN defined on the same finite set, k k all with cyclic Sylow subgroups, such that Sub (Gi ) = Sub (Gj ) for all i; j; k. 1. Introduction To what extent is a finite group determined by the subgroup lattices of its finite direct powers? Reinhold Baer proved results in 1939 implying that an abelian group G is determined up to isomorphism by Sub (G3) (cf. [1]). Michio Suzuki proved in 1951 that a finite simple group G is determined up to isomorphism by Sub (G2) (cf. [10]). Roland Schmidt proved in 1981 that if G is a finite, perfect, centerless group, then it is determined up to isomorphism by Sub (G2) (cf. [6]). Later, Schmidt proved in [7] that if G has an elementary abelian Hall normal subgroup that equals its own centralizer, then G is determined up to isomorphism by Sub (G3). It has long been open whether every finite group G is determined up to isomorphism by Sub (G3). (For more information on this problem, see the books [8, 11].) One may ask more generally to what extent a finite algebraic structure (or algebra) is determined by the subalgebra lattices of its finite direct powers. -
Groups with Almost Modular Subgroup Lattice Provided by Elsevier - Publisher Connector
Journal of Algebra 243, 738᎐764Ž. 2001 doi:10.1006rjabr.2001.8886, available online at http:rrwww.idealibrary.com on View metadata, citation and similar papers at core.ac.uk brought to you by CORE Groups with Almost Modular Subgroup Lattice provided by Elsevier - Publisher Connector Francesco de Giovanni and Carmela Musella Dipartimento di Matematica e Applicazioni, Uni¨ersita` di Napoli ‘‘Federico II’’, Complesso Uni¨ersitario Monte S. Angelo, Via Cintia, I 80126, Naples, Italy and Yaroslav P. Sysak1 Institute of Mathematics, Ukrainian National Academy of Sciences, ¨ul. Tereshchenki¨ska 3, 01601 Kie¨, Ukraine Communicated by Gernot Stroth Received November 14, 2000 DEDICATED TO BERNHARD AMBERG ON THE OCCASION OF HIS 60TH BIRTHDAY 1. INTRODUCTION A subgroup of a group G is called modular if it is a modular element of the lattice ᑦŽ.G of all subgroups of G. It is clear that everynormal subgroup of a group is modular, but arbitrarymodular subgroups need not be normal; thus modularitymaybe considered as a lattice generalization of normality. Lattices with modular elements are also called modular. Abelian groups and the so-called Tarski groupsŽ i.e., infinite groups all of whose proper nontrivial subgroups have prime order. are obvious examples of groups whose subgroup lattices are modular. The structure of groups with modular subgroup lattice has been described completelybyIwasawa wx4, 5 and Schmidt wx 13 . For a detailed account of results concerning modular subgroups of groups, we refer the reader towx 14 . 1 This work was done while the third author was visiting the Department of Mathematics of the Universityof Napoli ‘‘Federico II.’’ He thanks the G.N.S.A.G.A. -
The Theory of Lattice-Ordered Groups
The Theory ofLattice-Ordered Groups Mathematics and Its Applications Managing Editor: M. HAZEWINKEL Centre for Mathematics and Computer Science, Amsterdam, The Netherlands Volume 307 The Theory of Lattice-Ordered Groups by V. M. Kopytov Institute ofMathematics, RussianAcademyof Sciences, Siberian Branch, Novosibirsk, Russia and N. Ya. Medvedev Altai State University, Bamaul, Russia Springer-Science+Business Media, B.Y A C.I.P. Catalogue record for this book is available from the Library ofCongress. ISBN 978-90-481-4474-7 ISBN 978-94-015-8304-6 (eBook) DOI 10.1007/978-94-015-8304-6 Printed on acid-free paper All Rights Reserved © 1994 Springer Science+Business Media Dordrecht Originally published by Kluwer Academic Publishers in 1994. Softcover reprint ofthe hardcover Ist edition 1994 No part of the material protected by this copyright notice may be reproduced or utilized in any form or by any means, electronic or mechanical, including photocopying, recording or by any information storage and retrie val system, without written permission from the copyright owner. Contents Preface IX Symbol Index Xlll 1 Lattices 1 1.1 Partially ordered sets 1 1.2 Lattices .. ..... 3 1.3 Properties of lattices 5 1.4 Distributive and modular lattices. Boolean algebras 6 2 Lattice-ordered groups 11 2.1 Definition of the l-group 11 2.2 Calculations in I-groups 15 2.3 Basic facts . 22 3 Convex I-subgroups 31 3.1 The lattice of convex l-subgroups .......... .. 31 3.2 Archimedean o-groups. Convex subgroups in o-groups. 34 3.3 Prime subgroups 39 3.4 Polars ... ..................... 43 3.5 Lattice-ordered groups with finite Boolean algebra of polars ...................... -
LATTICE DIFFEOMORPHISM INVARIANCE Action of the Metric in the Continuum Limit
Lattice diffeomorphism invariance C. Wetterich Institut f¨ur Theoretische Physik Universit¨at Heidelberg Philosophenweg 16, D-69120 Heidelberg We propose a lattice counterpart of diffeomorphism symmetry in the continuum. A functional integral for quantum gravity is regularized on a discrete set of space-time points, with fermionic or bosonic lattice fields. When the space-time points are positioned as discrete points of a contin- uous manifold, the lattice action can be reformulated in terms of average fields within local cells and lattice derivatives. Lattice diffeomorphism invariance is realized if the action is independent of the positioning of the space-time points. Regular as well as rather irregular lattices are then described by the same action. Lattice diffeomorphism invariance implies that the continuum limit and the quantum effective action are invariant under general coordinate transformations - the basic ingredient for general relativity. In our approach the lattice diffeomorphism invariant actions are formulated without introducing a metric or other geometrical objects as fundamental degrees of freedom. The metric rather arises as the expectation value of a suitable collective field. As exam- ples, we present lattice diffeomorphism invariant actions for a bosonic non-linear sigma-model and lattice spinor gravity. I. INTRODUCTION metric give a reasonable description for the effective gravity theory at long distances. Besides a possible cosmological A quantum field theory for gravity may be based on a constant the curvature scalar is the leading term in such a functional integral. This is well defined, however, only if a derivative expansion for the metric. suitable regularization can be given. At this point major If regularized lattice quantum gravity with a suitable obstacles arise. -
Lattices in Lie Groups
Lattices in Lie groups Dave Witte Morris Lattices in Lie groups 1: Introduction University of Lethbridge, Alberta, Canada http://people.uleth.ca/ dave.morris What is a lattice subgroup? ∼ [email protected] Arithmetic construction of lattices. Abstract Compactness criteria. During this mini-course, the students will learn the Classical simple Lie groups. basic theory of lattices in semisimple Lie groups. Examples will be provided by simple arithmetic constructions. Aspects of the geometric and algebraic structure of lattices will be discussed, and the Superrigidity and Arithmeticity Theorems of Margulis will be described. Dave Witte Morris (U of Lethbridge) Lattices 1: Introduction CIRM, Jan 2019 1 / 18 Dave Witte Morris (U of Lethbridge) Lattices 1: Introduction CIRM, Jan 2019 2 / 18 A simple example. Z2 is a cocompact lattice in R2. 2 2 R is a connected Lie group Replace R with interesting group G. group: (x1,x2) (y1,y2) (x1 y1,x2 y2) + = + + Riemannian manifold (metric space, connected) is a cocompact lattice in G: (discrete subgroup) distance is right-invariant: d(x a, y a) d(x, y) + + = Every pt in G is within bounded distance of . group ops (x y and x) continuous (differentiable) Γ + − g cγ where c is bounded — in cpct set 2 = Z is a discrete subgroup (no accumulation points) compact C G, G C . Γ Every point in R2 is within ∃ ⊆ = G/ is cpct. (gn g ! γn , gnγn g) 2 bdd distance C √2 of Z → Γ ∃{ } → = 2 Z is a cocompact lattice is a latticeΓ in G: Γ Γ ⇒ 2 in R . only require C (or G/ ) to have finite volume. -
R. Ji, C. Ogle, and B. Ramsey. Relatively Hyperbolic
J. Noncommut. Geom. 4 (2010), 83–124 Journal of Noncommutative Geometry DOI 10.4171/JNCG/50 © European Mathematical Society Relatively hyperbolic groups, rapid decay algebras and a generalization of the Bass conjecture Ronghui Ji, Crichton Ogle, and Bobby Ramsey With an Appendix by Crichton Ogle Abstract. By deploying dense subalgebras of `1.G/ we generalize the Bass conjecture in terms of Connes’ cyclic homology theory. In particular, we propose a stronger version of the `1-Bass Conjecture. We prove that hyperbolic groups relative to finitely many subgroups, each of which posses the polynomial conjugacy bound property and nilpotent periodicity property, satisfy the `1-Stronger-Bass Conjecture. Moreover, we determine the conjugacy bound for relatively hyperbolic groups and compute the cyclic cohomology of the `1-algebra of any discrete group. Mathematics Subject Classification (2010). 46L80, 20F65, 16S34. Keywords. B-bounded cohomology, rapid decay algebras, Bass conjecture. Introduction Let R be a discrete ring with unit. A classical construction of Hattori–Stallings ([Ha], [St]) yields a homomorphism of abelian groups HS a Tr K0 .R/ ! HH0.R/; a where K0 .R/ denotes the zeroth algebraic K-group of R and HH0.R/ D R=ŒR; R its zeroth Hochschild homology group. Precisely, given a projective module P over R, one chooses a free R-module Rn containing P as a direct summand, resulting in a map n Trace EndR.P / ,! EndR.R / D Mn;n.R/ ! HH0.R/: HS One then verifies the equivalence class of Tr .ŒP / ´ Trace..IdP // in HH0.R/ depends only on the isomorphism class of P , is invariant under stabilization, and sends direct sums to sums. -
Arxiv:1711.08410V2
LATTICE ENVELOPES URI BADER, ALEX FURMAN, AND ROMAN SAUER Abstract. We introduce a class of countable groups by some abstract group- theoretic conditions. It includes linear groups with finite amenable radical and finitely generated residually finite groups with some non-vanishing ℓ2- Betti numbers that are not virtually a product of two infinite groups. Further, it includes acylindrically hyperbolic groups. For any group Γ in this class we determine the general structure of the possible lattice embeddings of Γ, i.e. of all compactly generated, locally compact groups that contain Γ as a lattice. This leads to a precise description of possible non-uniform lattice embeddings of groups in this class. Further applications include the determination of possi- ble lattice embeddings of fundamental groups of closed manifolds with pinched negative curvature. 1. Introduction 1.1. Motivation and background. Let G be a locally compact second countable group, hereafter denoted lcsc1. Such a group carries a left-invariant Radon measure unique up to scalar multiple, known as the Haar measure. A subgroup Γ < G is a lattice if it is discrete, and G/Γ carries a finite G-invariant measure; equivalently, if the Γ-action on G admits a Borel fundamental domain of finite Haar measure. If G/Γ is compact, one says that Γ is a uniform lattice, otherwise Γ is a non- uniform lattice. The inclusion Γ ֒→ G is called a lattice embedding. We shall also say that G is a lattice envelope of Γ. The classical examples of lattices come from geometry and arithmetic. Starting from a locally symmetric manifold M of finite volume, we obtain a lattice embedding π1(M) ֒→ Isom(M˜ ) of its fundamental group into the isometry group of its universal covering via the action by deck transformations.