Hyperbolic Triangle Groups
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Hyperbolic Reflection Groups
Uspekhi Mat. N auk 40:1 (1985), 29 66 Russian Math. Surveys 40:1 (1985), 31 75 Hyperbolic reflection groups E.B. Vinberg CONTENTS Introduction 31 Chapter I. Acute angled polytopes in Lobachevskii spaces 39 § 1. The G ram matrix of a convex polytope 39 §2. The existence theorem for an acute angled polytope with given Gram 42 matrix §3. Determination of the combinatorial structure of an acute angled 46 polytope from its Gram matrix §4. Criteria for an acute angled polytope to be bounded and to have finite 50 volume Chapter II. Crystallographic reflection groups in Lobachevskii spaces 57 §5. The language of Coxeter schemes. Construction of crystallographic 57 reflection groups §6. The non existence of discrete reflection groups with bounded 67 fundamental polytope in higher dimensional Lobachevskii spaces References 71 Introduction 1. Let X" be the « dimensional Euclidean space Ε", the « dimensional sphere S", or the « dimensional Lobachevskii space Λ". A convex polytope PCX" bounded by hyperplanes //,·, i G / , is said to be a Coxeter polytope if for all /, / G / , i Φ j, the hyperplanes //, and Hj are disjoint or form a dihedral angle of π/rijj, wh e r e «,y G Ζ and η,γ > 2. (We have in mind a dihedral angle containing P.) If Ρ is a Coxeter polytope, then the group Γ of motions of X" generated by the reflections Λ, in the hyperplanes Hj is discrete, and Ρ is a fundamental polytope for it. This means that the polytopes yP, y G Γ, do not have pairwise common interior points and cover X"; that is, they form a tessellation for X". -
On Discrete Generalised Triangle Groups
Proceedings of the Edinburgh Mathematical Society (1995) 38, 397-412 © ON DISCRETE GENERALISED TRIANGLE GROUPS by M. HAGELBERG, C. MACLACHLAN and G. ROSENBERGER (Received 29th October 1993) A generalised triangle group has a presentation of the form where R is a cyclically reduced word involving both x and y. When R=xy, these classical triangle groups have representations as discrete groups of isometries of S2, R2, H2 depending on In this paper, for other words R, faithful discrete representations of these groups in Isom + H3 = PSL(2,C) are considered with particular emphasis on the case /? = [x, y] and also on the relationship between the Euler characteristic x and finite covolume representations. 1991 Mathematics subject classification: 20H15. 1. Introduction In this article, we consider generalised triangle groups, i.e. groups F with a presentation of the form where R(x,y) is a cyclically reduced word in the free product on x,y which involves both x and y. These groups have been studied for their group theoretical interest [8, 7, 13], for topological reasons [2], and more recently for their connections with hyperbolic 3-manifolds and orbifolds [12, 10]. Here we will be concerned with faithful discrete representations p:T-*PSL(2,C) with particular emphasis on the cases where the Kleinian group p(F) has finite covolume. In Theorem 3.2, we give necessary conditions on the group F so that it should admit such a faithful discrete representation of finite covolume. For certain generalised triangle groups where the word R(x,y) has a specified form, faithful discrete representations as above have been constructed by Helling-Mennicke- Vinberg [12] and by the first author [11]. -
The Magic Square of Reflections and Rotations
THE MAGIC SQUARE OF REFLECTIONS AND ROTATIONS RAGNAR-OLAF BUCHWEITZ†, ELEONORE FABER, AND COLIN INGALLS Dedicated to the memories of two great geometers, H.M.S. Coxeter and Peter Slodowy ABSTRACT. We show how Coxeter’s work implies a bijection between complex reflection groups of rank two and real reflection groups in O(3). We also consider this magic square of reflections and rotations in the framework of Clifford algebras: we give an interpretation using (s)pin groups and explore these groups in small dimensions. CONTENTS 1. Introduction 2 2. Prelude: the groups 2 3. The Magic Square of Rotations and Reflections 4 Reflections, Take One 4 The Magic Square 4 Historical Note 8 4. Quaternions 10 5. The Clifford Algebra of Euclidean 3–Space 12 6. The Pin Groups for Euclidean 3–Space 13 7. Reflections 15 8. General Clifford algebras 15 Quadratic Spaces 16 Reflections, Take two 17 Clifford Algebras 18 Real Clifford Algebras 23 Cl0,1 23 Cl1,0 24 Cl0,2 24 Cl2,0 25 Cl0,3 25 9. Acknowledgements 25 References 25 Date: October 22, 2018. 2010 Mathematics Subject Classification. 20F55, 15A66, 11E88, 51F15 14E16 . Key words and phrases. Finite reflection groups, Clifford algebras, Quaternions, Pin groups, McKay correspondence. R.-O.B. and C.I. were partially supported by their respective NSERC Discovery grants, and E.F. acknowl- edges support of the European Union’s Horizon 2020 research and innovation programme under the Marie Skłodowska-Curie grant agreement No 789580. All three authors were supported by the Mathematisches Forschungsinstitut Oberwolfach through the Leibniz fellowship program in 2017, and E.F and C.I. -
Hyperbolic Geometry
Hyperbolic Geometry David Gu Yau Mathematics Science Center Tsinghua University Computer Science Department Stony Brook University [email protected] September 12, 2020 David Gu (Stony Brook University) Computational Conformal Geometry September 12, 2020 1 / 65 Uniformization Figure: Closed surface uniformization. David Gu (Stony Brook University) Computational Conformal Geometry September 12, 2020 2 / 65 Hyperbolic Structure Fundamental Group Suppose (S; g) is a closed high genus surface g > 1. The fundamental group is π1(S; q), represented as −1 −1 −1 −1 π1(S; q) = a1; b1; a2; b2; ; ag ; bg a1b1a b ag bg a b : h ··· j 1 1 ··· g g i Universal Covering Space universal covering space of S is S~, the projection map is p : S~ S.A ! deck transformation is an automorphism of S~, ' : S~ S~, p ' = '. All the deck transformations form the Deck transformation! group◦ DeckS~. ' Deck(S~), choose a pointq ~ S~, andγ ~ S~ connectsq ~ and '(~q). The 2 2 ⊂ projection γ = p(~γ) is a loop on S, then we obtain an isomorphism: Deck(S~) π1(S; q);' [γ] ! 7! David Gu (Stony Brook University) Computational Conformal Geometry September 12, 2020 3 / 65 Hyperbolic Structure Uniformization The uniformization metric is ¯g = e2ug, such that the K¯ 1 everywhere. ≡ − 2 Then (S~; ¯g) can be isometrically embedded on the hyperbolic plane H . The On the hyperbolic plane, all the Deck transformations are isometric transformations, Deck(S~) becomes the so-called Fuchsian group, −1 −1 −1 −1 Fuchs(S) = α1; β1; α2; β2; ; αg ; βg α1β1α β αg βg α β : h ··· j 1 1 ··· g g i The Fuchsian group generators are global conformal invariants, and form the coordinates in Teichm¨ullerspace. -
Arxiv:Math/0306105V2
A bound for the number of automorphisms of an arithmetic Riemann surface BY MIKHAIL BELOLIPETSKY Sobolev Institute of Mathematics, Novosibirsk, 630090, Russia e-mail: [email protected] AND GARETH A. JONES Faculty of Mathematical Studies, University of Southampton, Southampton, SO17 1BJ e-mail: [email protected] Abstract We show that for every g ≥ 2 there is a compact arithmetic Riemann surface of genus g with at least 4(g − 1) automorphisms, and that this lower bound is attained by infinitely many genera, the smallest being 24. 1. Introduction Schwarz [17] proved that the automorphism group of a compact Riemann surface of genus g ≥ 2 is finite, and Hurwitz [10] showed that its order is at most 84(g − 1). This bound is sharp, by which we mean that it is attained for infinitely many g, and the least genus of such an extremal surface is 3. However, it is also well known that there are infinitely many genera for which the bound 84(g − 1) is not attained. It therefore makes sense to consider the maximal order N(g) of the group of automorphisms of any Riemann surface of genus g. Accola [1] and Maclachlan [14] independently proved that N(g) ≥ 8(g +1). This bound is also sharp, and according to p. 93 of [2], Paul Hewitt has shown that the least genus attaining it is 23. Thus we have the following sharp bounds for N(g) with g ≥ 2: 8(g + 1) ≤ N(g) ≤ 84(g − 1). arXiv:math/0306105v2 [math.GR] 21 Nov 2004 We now consider these bounds from an arithmetic point of view, defining arithmetic Riemann surfaces to be those which are uniformized by arithmetic Fuchsian groups. -
Cross-Ratio Dynamics on Ideal Polygons
Cross-ratio dynamics on ideal polygons Maxim Arnold∗ Dmitry Fuchsy Ivan Izmestievz Serge Tabachnikovx Abstract Two ideal polygons, (p1; : : : ; pn) and (q1; : : : ; qn), in the hyperbolic plane or in hyperbolic space are said to be α-related if the cross-ratio [pi; pi+1; qi; qi+1] = α for all i (the vertices lie on the projective line, real or complex, respectively). For example, if α = 1, the respec- − tive sides of the two polygons are orthogonal. This relation extends to twisted ideal polygons, that is, polygons with monodromy, and it descends to the moduli space of M¨obius-equivalent polygons. We prove that this relation, which is, generically, a 2-2 map, is completely integrable in the sense of Liouville. We describe integrals and invari- ant Poisson structures, and show that these relations, with different values of the constants α, commute, in an appropriate sense. We inves- tigate the case of small-gons, describe the exceptional ideal polygons, that possess infinitely many α-related polygons, and study the ideal polygons that are α-related to themselves (with a cyclic shift of the indices). Contents 1 Introduction 3 ∗Department of Mathematics, University of Texas, 800 West Campbell Road, Richard- son, TX 75080; [email protected] yDepartment of Mathematics, University of California, Davis, CA 95616; [email protected] zDepartment of Mathematics, University of Fribourg, Chemin du Mus´ee 23, CH-1700 Fribourg; [email protected] xDepartment of Mathematics, Pennsylvania State University, University Park, PA 16802; [email protected] 1 1.1 Motivation: iterations of evolutes . .3 1.2 Plan of the paper and main results . -
Reflection Groups 3
Lecture Notes Reflection Groups Dr Dmitriy Rumynin Anna Lena Winstel Autumn Term 2010 Contents 1 Finite Reflection Groups 3 2 Root systems 6 3 Generators and Relations 14 4 Coxeter group 16 5 Geometric representation of W (mij) 21 6 Fundamental chamber 28 7 Classification 34 8 Crystallographic Coxeter groups 43 9 Polynomial invariants 46 10 Fundamental degrees 54 11 Coxeter elements 57 1 Finite Reflection Groups V = (V; h ; i) - Euclidean Vector space where V is a finite dimensional vector space over R and h ; i : V × V −! R is bilinear, symmetric and positiv definit. n n P Example: (R ; ·): h(αi); (βi)i = αiβi i=1 Gram-Schmidt theory tells that for all Euclidean vector spaces, there exists an isometry (linear n bijective and 8 x; y 2 V : T (x) · T (y) = hx; yi) T : V −! R . In (V; h ; i) you can • measure length: jjxjj = phx; xi hx;yi • measure angles: xyc = arccos jjx||·||yjj • talk about orthogonal transformations O(V ) = fT 2 GL(V ): 8 x; y 2 V : hT x; T yi = hx; yig ≤ GL(V ) T 2 GL(V ). Let V T = fv 2 V : T v = vg the fixed points of T or the 1-eigenspace. Definition. T 2 GL(V ) is a reflection if T 2 O(V ) and dim V T = dim V − 1. Lemma 1.1. Let T be a reflection, x 2 (V T )? = fv : 8 w 2 V T : hv; wi = 0g; x 6= 0. Then 1. T (x) = −x hx;zi 2. 8 z 2 V : T (z) = z − 2 hx;xi · x Proof. -
Regular Elements of Finite Reflection Groups
Inventiones math. 25, 159-198 (1974) by Springer-Veriag 1974 Regular Elements of Finite Reflection Groups T.A. Springer (Utrecht) Introduction If G is a finite reflection group in a finite dimensional vector space V then ve V is called regular if no nonidentity element of G fixes v. An element ge G is regular if it has a regular eigenvector (a familiar example of such an element is a Coxeter element in a Weyl group). The main theme of this paper is the study of the properties and applications of the regular elements. A review of the contents follows. In w 1 we recall some known facts about the invariant theory of finite linear groups. Then we discuss in w2 some, more or less familiar, facts about finite reflection groups and their invariant theory. w3 deals with the problem of finding the eigenvalues of the elements of a given finite linear group G. It turns out that the explicit knowledge of the algebra R of invariants of G implies a solution to this problem. If G is a reflection group, R has a very simple structure, which enables one to obtain precise results about the eigenvalues and their multiplicities (see 3.4). These results are established by using some standard facts from algebraic geometry. They can also be used to give a proof of the formula for the order of finite Chevalley groups. We shall not go into this here. In the case of eigenvalues of regular elements one can go further, this is discussed in w4. One obtains, for example, a formula for the order of the centralizer of a regular element (see 4.2) and a formula for the eigenvalues of a regular element in an irreducible representation (see 4.5). -
Arxiv:1012.2020V1 [Math.CV]
TRANSITIVITY ON WEIERSTRASS POINTS ZOË LAING AND DAVID SINGERMAN 1. Introduction An automorphism of a Riemann surface will preserve its set of Weier- strass points. In this paper, we search for Riemann surfaces whose automorphism groups act transitively on the Weierstrass points. One well-known example is Klein’s quartic, which is known to have 24 Weierstrass points permuted transitively by it’s automorphism group, PSL(2, 7) of order 168. An investigation of when Hurwitz groups act transitively has been made by Magaard and Völklein [19]. After a section on the preliminaries, we examine the transitivity property on several classes of surfaces. The easiest case is when the surface is hy- perelliptic, and we find all hyperelliptic surfaces with the transitivity property (there are infinitely many of them). We then consider surfaces with automorphism group PSL(2, q), Weierstrass points of weight 1, and other classes of Riemann surfaces, ending with Fermat curves. Basically, we find that the transitivity property property seems quite rare and that the surfaces we have found with this property are inter- esting for other reasons too. 2. Preliminaries Weierstrass Gap Theorem ([6]). Let X be a compact Riemann sur- face of genus g. Then for each point p ∈ X there are precisely g integers 1 = γ1 < γ2 <...<γg < 2g such that there is no meromor- arXiv:1012.2020v1 [math.CV] 9 Dec 2010 phic function on X whose only pole is one of order γj at p and which is analytic elsewhere. The integers γ1,...,γg are called the gaps at p. The complement of the gaps at p in the natural numbers are called the non-gaps at p. -
REFLECTION GROUPS and COXETER GROUPS by Kouver
REFLECTION GROUPS AND COXETER GROUPS by Kouver Bingham A Senior Honors Thesis Submitted to the Faculty of The University of Utah In Partial Fulfillment of the Requirements for the Honors Degree in Bachelor of Science In Department of Mathematics Approved: Mladen Bestviva Dr. Peter Trapa Supervisor Chair, Department of Mathematics ( Jr^FeraSndo Guevara Vasquez Dr. Sylvia D. Torti Department Honors Advisor Dean, Honors College July 2014 ABSTRACT In this paper we give a survey of the theory of Coxeter Groups and Reflection groups. This survey will give an undergraduate reader a full picture of Coxeter Group theory, and will lean slightly heavily on the side of showing examples, although the course of discussion will be based on theory. We’ll begin in Chapter 1 with a discussion of its origins and basic examples. These examples will illustrate the importance and prevalence of Coxeter Groups in Mathematics. The first examples given are the symmetric group <7„, and the group of isometries of the ^-dimensional cube. In Chapter 2 we’ll formulate a general notion of a reflection group in topological space X, and show that such a group is in fact a Coxeter Group. In Chapter 3 we’ll introduce the Poincare Polyhedron Theorem for reflection groups which will vastly expand our understanding of reflection groups thereafter. We’ll also give some surprising examples of Coxeter Groups that section. Then, in Chapter 4 we’ll make a classification of irreducible Coxeter Groups, give a linear representation for an arbitrary Coxeter Group, and use this complete the fact that all Coxeter Groups can be realized as reflection groups with Tit’s Theorem. -
Conformal Quasicrystals and Holography
Conformal Quasicrystals and Holography Latham Boyle1, Madeline Dickens2 and Felix Flicker2;3 1Perimeter Institute for Theoretical Physics, Waterloo, Ontario N2L 2Y5, Canada, N2L 2Y5 2Department of Physics, University of California, Berkeley, California 94720, USA 3Rudolf Peierls Centre for Theoretical Physics, University of Oxford, Department of Physics, Clarendon Laboratory, Parks Road, Oxford, OX1 3PU, United Kingdom Recent studies of holographic tensor network models defined on regular tessellations of hyperbolic space have not yet addressed the underlying discrete geometry of the boundary. We show that the boundary degrees of freedom naturally live on a novel structure, a conformal quasicrystal, that pro- vides a discrete model of conformal geometry. We introduce and construct a class of one-dimensional conformal quasicrystals, and discuss a higher-dimensional example (related to the Penrose tiling). Our construction permits discretizations of conformal field theories that preserve an infinite discrete subgroup of the global conformal group at the cost of lattice periodicity. I. INTRODUCTION dom [12{24]. Meanwhile, quantum information theory provides a unifying language for these studies in terms of entanglement, quantum circuits, and quantum error A central topic in theoretical physics over the past two correction [25]. decades has been holography: the idea that a quantum These investigations have gradually clarified our un- theory in a bulk space may be precisely dual to another derstanding of the discrete geometry in the bulk. There living on the boundary of that space. The most concrete has been a common expectation, based on an analogy and widely-studied realization of this idea has been the with AdS/CFT [1{3], that TNs living on discretizations AdS/CFT correspondence [1{3], in which a gravitational of a hyperbolic space define a lattice state of a critical theory living in a (d + 1)-dimensional negatively-curved system on the boundary and vice-versa. -
MATH32052 Hyperbolic Geometry
MATH32052 Hyperbolic Geometry Charles Walkden 12th January, 2019 MATH32052 Contents Contents 0 Preliminaries 3 1 Where we are going 6 2 Length and distance in hyperbolic geometry 13 3 Circles and lines, M¨obius transformations 18 4 M¨obius transformations and geodesics in H 23 5 More on the geodesics in H 26 6 The Poincar´edisc model 39 7 The Gauss-Bonnet Theorem 44 8 Hyperbolic triangles 52 9 Fixed points of M¨obius transformations 56 10 Classifying M¨obius transformations: conjugacy, trace, and applications to parabolic transformations 59 11 Classifying M¨obius transformations: hyperbolic and elliptic transforma- tions 62 12 Fuchsian groups 66 13 Fundamental domains 71 14 Dirichlet polygons: the construction 75 15 Dirichlet polygons: examples 79 16 Side-pairing transformations 84 17 Elliptic cycles 87 18 Generators and relations 92 19 Poincar´e’s Theorem: the case of no boundary vertices 97 20 Poincar´e’s Theorem: the case of boundary vertices 102 c The University of Manchester 1 MATH32052 Contents 21 The signature of a Fuchsian group 109 22 Existence of a Fuchsian group with a given signature 117 23 Where we could go next 123 24 All of the exercises 126 25 Solutions 138 c The University of Manchester 2 MATH32052 0. Preliminaries 0. Preliminaries 0.1 Contact details § The lecturer is Dr Charles Walkden, Room 2.241, Tel: 0161 27 55805, Email: [email protected]. My office hour is: WHEN?. If you want to see me at another time then please email me first to arrange a mutually convenient time. 0.2 Course structure § 0.2.1 MATH32052 § MATH32052 Hyperbolic Geoemtry is a 10 credit course.