Some Questions About Semisimple Lie Groups Originating in Matrix Theory
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On the Holographic S–Matrix
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server On the Holographic S{matrix I.Ya.Aref’eva Steklov Mathematical Institute, Russian Academy of Sciences Gubkin St.8, GSP-1, 117966, Moscow, Russia Centro Vito Volterra, Universita di Roma Tor Vergata, Italy [email protected] Abstract The recent proposal by Polchinski and Susskind for the holographic flat space S– matrix is discussed. By using Feynman diagrams we argue that in principle all the information about the S–matrix in the interacting field theory in the bulk of the anti- de Sitter space is encoded into the data on the timelike boundary. The problem of locality of interpolating field is discussed and it is suggested that the interpolating field lives in a quantum Boltzmannian Hilbert space. 1 According to the holographic principle [1, 2] one should describe a field theory on a manifold M which includes gravity by a theory which lives on the boundary of M.Two prominent examples of the holography are the Matrix theory [3] and the AdS/CFT corre- spondence [4, 5, 6]. The relation between quantum gravity in the anti-de Sitter space and the gauge theory on the boundary could be useful for better understanding of both theories. In principle CFT might teach us about quantum gravity in the bulk of AdS. Correlation functions in the Euclidean formulation are the subject of intensive study (see for example [7]-[21]). The AdS/CFT correspondence in the Lorentz formulation is considered in [22]-[29]. -
Maximality of Hyperspecial Compact Subgroups Avoiding Bruhat–Tits Theory Tome 67, No 1 (2017), P
R AN IE N R A U L E O S F D T E U L T I ’ I T N S ANNALES DE L’INSTITUT FOURIER Marco MACULAN Maximality of hyperspecial compact subgroups avoiding Bruhat–Tits theory Tome 67, no 1 (2017), p. 1-21. <http://aif.cedram.org/item?id=AIF_2017__67_1_1_0> © Association des Annales de l’institut Fourier, 2017, Certains droits réservés. Cet article est mis à disposition selon les termes de la licence CREATIVE COMMONS ATTRIBUTION – PAS DE MODIFICATION 3.0 FRANCE. http://creativecommons.org/licenses/by-nd/3.0/fr/ L’accès aux articles de la revue « Annales de l’institut Fourier » (http://aif.cedram.org/), implique l’accord avec les conditions générales d’utilisation (http://aif.cedram.org/legal/). cedram Article mis en ligne dans le cadre du Centre de diffusion des revues académiques de mathématiques http://www.cedram.org/ Ann. Inst. Fourier, Grenoble 67, 1 (2017) 1-21 MAXIMALITY OF HYPERSPECIAL COMPACT SUBGROUPS AVOIDING BRUHAT–TITS THEORY by Marco MACULAN Abstract. — Let k be a complete non-archimedean field (non trivially valued). Given a reductive k-group G, we prove that hyperspecial subgroups of G(k) (i.e. those arising from reductive models of G) are maximal among bounded subgroups. The originality resides in the argument: it is inspired by the case of GLn and avoids all considerations on the Bruhat–Tits building of G. Résumé. — Soit k un corps non-archimédien complet et non trivialement va- lué. Étant donné un k-groupe réductif G, nous démontrons que les sous-groupes hyperspéciaux de G(k) (c’est-à-dire ceux qui proviennent des modèles réductifs de G) sont maximaux parmi les sous-groupes bornés. -
The Classical Groups and Domains 1. the Disk, Upper Half-Plane, SL 2(R
(June 8, 2018) The Classical Groups and Domains Paul Garrett [email protected] http:=/www.math.umn.edu/egarrett/ The complex unit disk D = fz 2 C : jzj < 1g has four families of generalizations to bounded open subsets in Cn with groups acting transitively upon them. Such domains, defined more precisely below, are bounded symmetric domains. First, we recall some standard facts about the unit disk, the upper half-plane, the ambient complex projective line, and corresponding groups acting by linear fractional (M¨obius)transformations. Happily, many of the higher- dimensional bounded symmetric domains behave in a manner that is a simple extension of this simplest case. 1. The disk, upper half-plane, SL2(R), and U(1; 1) 2. Classical groups over C and over R 3. The four families of self-adjoint cones 4. The four families of classical domains 5. Harish-Chandra's and Borel's realization of domains 1. The disk, upper half-plane, SL2(R), and U(1; 1) The group a b GL ( ) = f : a; b; c; d 2 ; ad − bc 6= 0g 2 C c d C acts on the extended complex plane C [ 1 by linear fractional transformations a b az + b (z) = c d cz + d with the traditional natural convention about arithmetic with 1. But we can be more precise, in a form helpful for higher-dimensional cases: introduce homogeneous coordinates for the complex projective line P1, by defining P1 to be a set of cosets u 1 = f : not both u; v are 0g= × = 2 − f0g = × P v C C C where C× acts by scalar multiplication. -
A Note on Six-Dimensional Gauge Theories
ILL-(TH)-97-09 hep-th/9712168 A Note on Six-Dimensional Gauge Theories Robert G. Leigh∗† and Moshe Rozali‡ Department of Physics University of Illinois at Urbana-Champaign Urbana, IL 61801 July 9, 2018 Abstract We study the new “gauge” theories in 5+1 dimensions, and their non- commutative generalizations. We argue that the θ-term and the non-commutative torus parameters appear on an equal footing in the non-critical string theories which define the gauge theories. The use of these theories as a Matrix descrip- tion of M-theory on T 5, as well as a closely related realization as 5-branes in type IIB string theory, proves useful in studying some of their properties. arXiv:hep-th/9712168v2 14 Apr 1998 ∗U.S. Department of Energy Outstanding Junior Investigator †e-mail: [email protected] ‡e-mail: [email protected] 0 1 Introduction Matrix theory[1] is an attempt at a non-perturbative formulation of M-theory in the lightcone frame. Compactifying it on a torus T d has been shown to be related to the large N limit of Super-Yang-Mills (SYM) theory in d + 1 dimensions[2]. This description is necessarily only partial for d > 3, since the SYM theory is then not renormalizable. The SYM theory is defined, for d = 4 by the (2,0) superconformal field theory in 5+1 dimensions [3, 4], and for d = 5 by a non-critical string theory in 5+1 dimensions [4, 5]. The situation of compactifications to lower dimensions is unclear for now (for recent reviews see [7, 8]). -
Random Matrix Theory in Physics
RANDOM MATRIX THEORY IN PHYSICS π π Thomas Guhr, Lunds Universitet, Lund, Sweden p(W)(s) = s exp s2 : (2) 2 − 4 As shown in Figure 2, the Wigner surmise excludes de- Introduction generacies, p(W)(0) = 0, the levels repel each other. This is only possible if they are correlated. Thus, the Poisson We wish to study energy correlations of quantum spec- law and the Wigner surmise reflect the absence or the tra. Suppose the spectrum of a quantum system has presence of energy correlations, respectively. been measured or calculated. All levels in the total spec- trum having the same quantum numbers form one par- ticular subspectrum. Its energy levels are at positions 1.0 xn; n = 1; 2; : : : ; N, say. We assume that N, the num- ber of levels in this subspectrum, is large. With a proper ) s smoothing procedure, we obtain the level density R1(x), ( 0.5 i.e. the probability density of finding a level at the energy p x. As indicated in the top part of Figure 1, the level density R1(x) increases with x for most physics systems. 0.0 In the present context, however, we are not so interested 0 1 2 3 in the level density. We want to measure the spectral cor- s relations independently of it. Hence, we have to remove FIG. 2. Wigner surmise (solid) and Poisson law (dashed). the level density from the subspectrum. This is referred to as unfolding. We introduce a new dimensionless en- Now, the question arises: If these correlation patterns ergy scale ξ such that dξ = R (x)dx. -
[Math.DG] 7 Feb 2007 Hoe 1.1
A GEOMETRIC PROOF OF THE KARPELEVICH-MOSTOW’S THEOREM ANTONIO J. DI SCALA AND CARLOS OLMOS Abstract. In this paper we give a geometric proof of the Karpelevich’s theo- rem that asserts that a semisimple Lie subgroup of isometries, of a symmetric space of non compact type, has a totally geodesic orbit. In fact, this is equiv- alent to a well-known result of Mostow about existence of compatible Cartan decompositions. 1. Introduction. In this paper we address the problem of giving a geometric proof of the following theorem of Karpelevich. Theorem 1.1. (Karpelevich [Kar53]) Let M be a Riemannian symmetric space of non positive curvature without flat factor. Then any connected and semisimple subgroup G ⊂ Iso(M) has a totally geodesic orbit G.p ⊂ M. It is well-known that Karpelevich’s theorem is equivalent to the following alge- braic theorem. Theorem 1.2. (Mostow [Mos55, Theorem 6]) Let g′ be a real semisimple Lie algebra of non compact type and let g ⊂ g′ be a semisimple Lie subalgebra. Let g = k⊕p be a Cartan decomposition for g. Then there exists a Cartan decomposition g′ = k′ ⊕ p′ for g′ such that k ⊂ k′ and p ⊂ p′. The proof of the above theorems is very algebraic in nature and uses delicate arguments related to automorphisms of semisimple Lie algebras (see [Oni04] for a modern exposition of Karpelevich’s results). For the real hyperbolic spaces, i.e. when g′ = so(n, 1), there are two geometric arXiv:math/0702201v1 [math.DG] 7 Feb 2007 proofs of Karpelevich’s theorem [DSO01], [BZ04]. -
JT Gravity and Random Matrix Ensembles
JT Gravity And Random Matrix Ensembles Edward Witten Strings 2019, Brussels I will describe an extension of this work (Stanford and EW, \JT Gravity And The Ensembles of Random Matrix Theory," arXiv:1907:xxxxx). We generalized the story to include * time-reversal symmetry * fermions * N = 1 supersymmetry This morning Steve Shenker reported on random matrices and JT gravity (Saad, Shenker, and Stanford, \JT Gravity as a Matrix Integral" arXiv:1903.11115 ). * time-reversal symmetry * fermions * N = 1 supersymmetry This morning Steve Shenker reported on random matrices and JT gravity (Saad, Shenker, and Stanford, \JT Gravity as a Matrix Integral" arXiv:1903.11115 ). I will describe an extension of this work (Stanford and EW, \JT Gravity And The Ensembles of Random Matrix Theory," arXiv:1907:xxxxx). We generalized the story to include * fermions * N = 1 supersymmetry This morning Steve Shenker reported on random matrices and JT gravity (Saad, Shenker, and Stanford, \JT Gravity as a Matrix Integral" arXiv:1903.11115 ). I will describe an extension of this work (Stanford and EW, \JT Gravity And The Ensembles of Random Matrix Theory," arXiv:1907:xxxxx). We generalized the story to include * time-reversal symmetry * N = 1 supersymmetry This morning Steve Shenker reported on random matrices and JT gravity (Saad, Shenker, and Stanford, \JT Gravity as a Matrix Integral" arXiv:1903.11115 ). I will describe an extension of this work (Stanford and EW, \JT Gravity And The Ensembles of Random Matrix Theory," arXiv:1907:xxxxx). We generalized the story to include * time-reversal symmetry * fermions This morning Steve Shenker reported on random matrices and JT gravity (Saad, Shenker, and Stanford, \JT Gravity as a Matrix Integral" arXiv:1903.11115 ). -
Sato-Tate Equidistribution for Families of Hecke-Maass Forms on SL (N, R)/SO
SATO-TATE EQUIDISTRIBUTION FOR FAMILIES OF HECKE–MAASS FORMS ON SL(n, R)/ SO(n) JASMIN MATZ AND NICOLAS TEMPLIER Abstract. We establish the Sato-Tate equidistribution of Hecke eigenvalues of the family of Hecke–Maass cusp forms on SL(n, Z) SL(n, R)/ SO(n). As part of the proof, we establish a uniform upper-bound for spherical functions on\ semisimple Lie groups which is of independent interest. For each of the principal, symmetric square and exterior square L-functions, we deduce the level dis- tribution with restricted support of the low-lying zeros. We also deduce average estimates toward Ramanujan, including an improvement on the previous literature in the case n = 2. Contents 1. Introduction 1 2. Symmetry type of families and low-lying zeros 12 3. Average bounds towards Ramanujan 15 Part 1. Local theory: Real orbital integrals 18 4. Preliminaries 19 5. Setting for the main estimate 23 6. Bounds for semisimple orbital integrals 26 7. Weighted orbital integrals 29 8. Spherical functions and archimedean test functions 39 Part 2. Global theory: Weyl’s law and equidistribution 44 9. Setup for the Arthur-Selberg trace formula for GL(n) 44 10. Centralizers of semisimple elements 45 11. Coarse and fine geometric expansion 50 12. Bound for p-adic weighted orbital integrals 61 13. Spectral side and conclusion of proof of Theorem 1.1 67 References 72 arXiv:1505.07285v8 [math.NT] 18 May 2020 1. Introduction Hecke–Maass cusp forms are certain eigenfunctions of the Laplace operator on the locally sym- metric space SL(n, Z) SL(n, R)/ SO(n). -
D-Brane Actions and N = 2 Supergravity Solutions
D-Brane Actions and N =2Supergravity Solutions Thesis by Calin Ciocarlie In Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy California Institute of Technology Pasadena, California 2004 (Submitted May 20 , 2004) ii c 2004 Calin Ciocarlie All Rights Reserved iii Acknowledgements I would like to express my gratitude to the people who have taught me Physics throughout my education. My thesis advisor John Schwarz has given me insightful guidance and invaluable advice. I benefited a lot by collaborating with outstanding colleagues: Iosif Bena, Iouri Chepelev, Peter Lee, Jongwon Park. I have also bene- fited from interesting discussions with Vadim Borokhov, Jaume Gomis, Prof. Anton Kapustin, Tristan McLoughlin, Yuji Okawa, and Arkadas Ozakin. I am also thankful to my Physics teacher Violeta Grigorie who’s enthusiasm for Physics is contagious and to my family for constant support and encouragement in my academic pursuits. iv Abstract Among the most remarkable recent developments in string theory are the AdS/CFT duality, as proposed by Maldacena, and the emergence of noncommutative geometry. It has been known for some time that for a system of almost coincident D-branes the transverse displacements that represent the collective coordinates of the system become matrix-valued transforming in the adjoint representation of U(N). From a geometrical point of view this is rather surprising but, as we will see in Chapter 2, it is closely related to the noncommutative descriptions of D-branes. A consequence of the collective coordinates becoming matrix-valued is the ap- pearance of a “dielectric” effect in which D-branes can become polarized into higher- dimensional fuzzy D-branes. -
Homogeneous Spaces with the Cohomology of Sphere Products and Compact Quadrangles
Homogeneous spaces with the cohomology of sphere products and compact quadrangles Dissertation zur Erlangung des naturwissenschaftlichen Doktorgrades der Bayerischen Julius-Maximilians-Universit¨at Wurzburg¨ vorgelegt von Oliver Bletz-Siebert aus Heilbronn Wurzburg¨ 2002 Contents Preface v Notation xi 1 Fibrations and double fibrations 1 1.1 Fibrations . 1 1.2 Double fibrations . 2 2 Lie group actions 11 2.1 Lie theory . 12 2.2 Group actions . 18 2.3 Transitive actions . 21 2.4 Homogeneous spheres . 22 2.5 Almost transitive actions . 26 3 Isoparametric hypersurfaces 33 3.1 Homogeneous hypersurfaces . 33 3.2 Transitive actions on focal manifolds . 35 4 Generalized quadrangles 39 4.1 Geometries and generalized quadrangles . 39 4.2 Homogeneous quadrangles . 42 4.3 Point-homogeneous (1; 2)-quadrangles . 47 4.4 Orthogonal actions . 49 iii iv CONTENTS 4.5 Unitary actions . 51 4.6 Summary . 53 5 Three series of homogeneous spaces 55 5.1 The (5; 4n − 6)-series . 55 5.2 The (7; 4n − 8)-series . 58 5.3 The (3; 2n − 2)-series . 59 6 Rational cohomology 61 6.1 Orientable fibrations . 62 6.2 Spectral sequences . 68 6.3 Rational homotopy and rational cohomology . 74 6.4 Cohomology of some homogeneous spaces . 79 Bibliography 89 Index 94 Preface The homogeneous spaces that have the same (singular) cohomology as spheres were classified by Borel, Bredon, Montgomery and Samelson and by Poncet. This was extended to homogeneous spaces which are simply connected and which have the same rational cohomology as spheres by Onishchik and also by Kramer. Furthermore, Kramer classified the simply connected homoge- neous spaces with the rational cohomology of a sphere product k × m, where 3 ≤ k ≤ m and m is odd; and Wolfrom classified this kind of spaces in the case 2 = k ≤ m with odd m. -
Three Approaches to M-Theory
Three Approaches to M-theory Luca Carlevaro PhD. thesis submitted to obtain the degree of \docteur `es sciences de l'Universit´e de Neuch^atel" on monday, the 25th of september 2006 PhD. advisors: Prof. Jean-Pierre Derendinger Prof. Adel Bilal Thesis comittee: Prof. Matthias Blau Prof. Matthias R. Gaberdiel Universit´e de Neuch^atel Facult´e des Sciences Institut de Physique Rue A.-L. Breguet 1 CH-2001 Neuch^atel Suisse This thesis is based on researches supported the Swiss National Science Foundation and the Commission of the European Communities under contract MRTN-CT-2004-005104. i Mots-cl´es: Th´eorie des cordes, Th´eorie de M(atrice) , condensation de gaugino, brisure de supersym´etrie en th´eorie M effective, effets d'instantons de membrane, sym´etries cach´ees de la supergravit´e, conjecture sur E10 Keywords: String theory, M(atrix) theory, gaugino condensation, supersymmetry breaking in effective M-theory, membrane instanton effects, hidden symmetries in supergravity, E10 con- jecture ii Summary: Since the early days of its discovery, when the term was used to characterise the quantum com- pletion of eleven-dimensional supergravity and to determine the strong-coupling limit of type IIA superstring theory, the idea of M-theory has developed with time into a unifying framework for all known superstring the- ories. This evolution in conception has followed the progressive discovery of a large web of dualities relating seemingly dissimilar string theories, such as theories of closed and oriented strings (type II theories), of closed and open unoriented strings (type I theory), and theories with built in gauge groups (heterotic theories). -
Commuting Tuples in Reductive Groups and Their Maximal Compact Subgroups
Geometry & Topology 17 (2013) 2513–2593 msp Commuting tuples in reductive groups and their maximal compact subgroups ALEXANDRA PETTET JUAN SOUTO Let G be a reductive algebraic group and K G a maximal compact subgroup. We consider the representation spaces Hom.Zk ; K/ and Hom.Zk ; G/ with the topology induced from an embedding into Kk and Gk , respectively. The goal of this paper is to prove that Hom.Zk ; K/ is a strong deformation retract of Hom.Zk ; G/. 20G20; 55P99 1 Introduction k By a commuting k –tuple in a group G we mean a k –tuple .a1;:::; a / G with k 2 aiaj aj ai for all i and j . Observe that any such commuting k –tuple determines D uniquely a homomorphism k n1 nk Z G;.n1;:::; n / a a : ! k 7! 1 k In fact, we obtain in this way a bijection between Hom.Zk ; G/ and the set of commuting k –tuples in G . Suppose now that G is a Lie group and that K G is a closed subgroup. Endowing Hom.Zk ; G/ Gk and Hom.Zk ; K/ Kk with the subspace topology, we consider the embedding (1.1) Hom.Zk ; K/, Hom.Zk ; G/ ! induced by the inclusion of K into G . The goal of this paper is to prove that the map (1.1) is a homotopy equivalence if G is a reductive algebraic group and K G is a maximal compact subgroup. Before stating our main result precisely, recall that a weak retraction of a topological space X to a subspace A is a continuous map F Œ0; 1 X X;.t; x/ Ft .x/ W ! 7! Per me si va ne la cittá dolente, per me si va ne l’etterno dolore, per me si va tra la perduta gente.