Z-Graded Lie Superalgebras of Infinite Depth and Finite Growth 547
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3. Some Commutative Algebra Definition 3.1. Let R Be a Ring. We
3. Some commutative algebra Definition 3.1. Let R be a ring. We say that R is graded, if there is a direct sum decomposition, M R = Rn; n2N where each Rn is an additive subgroup of R, such that RdRe ⊂ Rd+e: The elements of Rd are called the homogeneous elements of order d. Let R be a graded ring. We say that an R-module M is graded if there is a direct sum decomposition M M = Mn; n2N compatible with the grading on R in the obvious way, RdMn ⊂ Md+n: A morphism of graded modules is an R-module map φ: M −! N of graded modules, which respects the grading, φ(Mn) ⊂ Nn: A graded submodule is a submodule for which the inclusion map is a graded morphism. A graded ideal I of R is an ideal, which when considered as a submodule is a graded submodule. Note that the kernel and cokernel of a morphism of graded modules is a graded module. Note also that an ideal is a graded ideal iff it is generated by homogeneous elements. Here is the key example. Example 3.2. Let R be the polynomial ring over a ring S. Define a direct sum decomposition of R by taking Rn to be the set of homogeneous polynomials of degree n. Given a graded ideal I in R, that is an ideal generated by homogeneous elements of R, the quotient is a graded ring. We will also need the notion of localisation, which is a straightfor- ward generalisation of the notion of the field of fractions. -
Introduction to Supersymmetry(1)
Introduction to Supersymmetry(1) J.N. Tavares Dep. Matem¶aticaPura, Faculdade de Ci^encias,U. Porto, 4000 Porto TQFT Club 1Esta ¶euma vers~aoprovis¶oria,incompleta, para uso exclusivo nas sess~oesde trabalho do TQFT club CONTENTS 1 Contents 1 Supersymmetry in Quantum Mechanics 2 1.1 The Supersymmetric Oscillator . 2 1.2 Witten Index . 4 1.3 A fundamental example: The Laplacian on forms . 7 1.4 Witten's proof of Morse Inequalities . 8 2 Supergeometry and Supersymmetry 13 2.1 Field Theory. A quick review . 13 2.2 SuperEuclidean Space . 17 2.3 Reality Conditions . 18 2.4 Supersmooth functions . 18 2.5 Supermanifolds . 21 2.6 Lie Superalgebras . 21 2.7 Super Lie groups . 26 2.8 Rigid Superspace . 27 2.9 Covariant Derivatives . 30 3 APPENDIX. Cli®ord Algebras and Spin Groups 31 3.1 Cli®ord Algebras . 31 Motivation. Cli®ord maps . 31 Cli®ord Algebras . 33 Involutions in V .................................. 35 Representations . 36 3.2 Pin and Spin groups . 43 3.3 Spin Representations . 47 3.4 U(2), spinors and almost complex structures . 49 3.5 Spinc(4)...................................... 50 Chiral Operator. Self Duality . 51 2 1 Supersymmetry in Quantum Mechanics 1.1 The Supersymmetric Oscillator i As we will see later the \hermitian supercharges" Q®, in the N extended SuperPoincar¶eLie Algebra obey the anticommutation relations: i j m ij fQ®;Q¯g = 2(γ C)®¯± Pm (1.1) m where ®; ¯ are \spinor" indices, i; j 2 f1; ¢ ¢ ¢ ;Ng \internal" indices and (γ C)®¯ a bilinear form in the spinor indices ®; ¯. When specialized to 0-space dimensions ((1+0)-spacetime), then since P0 = H, relations (1.1) take the form (with a little change in notations): fQi;Qjg = 2±ij H (1.2) with N \Hermitian charges" Qi; i = 1; ¢ ¢ ¢ ;N. -
Inönü–Wigner Contraction and D = 2 + 1 Supergravity
Eur. Phys. J. C (2017) 77:48 DOI 10.1140/epjc/s10052-017-4615-1 Regular Article - Theoretical Physics Inönü–Wigner contraction and D = 2 + 1 supergravity P. K. Concha1,2,a, O. Fierro3,b, E. K. Rodríguez1,2,c 1 Departamento de Ciencias, Facultad de Artes Liberales, Universidad Adolfo Ibáñez, Av. Padre Hurtado 750, Viña del Mar, Chile 2 Instituto de Ciencias Físicas y Matemáticas, Universidad Austral de Chile, Casilla 567, Valdivia, Chile 3 Departamento de Matemática y Física Aplicadas, Universidad Católica de la Santísima Concepción, Alonso de Rivera 2850, Concepción, Chile Received: 25 November 2016 / Accepted: 5 January 2017 / Published online: 25 January 2017 © The Author(s) 2017. This article is published with open access at Springerlink.com Abstract We present a generalization of the standard cannot always be obtained by rescaling the gauge fields and Inönü–Wigner contraction by rescaling not only the gener- considering some limit as in the (anti)commutation relations. ators of a Lie superalgebra but also the arbitrary constants In particular it is well known that, in the presence of the exotic appearing in the components of the invariant tensor. The Lagrangian, the Poincaré limit cannot be applied to a (p, q) procedure presented here allows one to obtain explicitly the AdS CS supergravity [7]. This difficulty can be overcome Chern–Simons supergravity action of a contracted superal- extending the osp (2, p) ⊗ osp (2, q) superalgebra by intro- gebra. In particular we show that the Poincaré limit can be ducing the automorphism generators so (p) and so (q) [9]. performed to a D = 2 + 1 (p, q) AdS Chern–Simons super- In such a case, the IW contraction can be applied and repro- gravity in presence of the exotic form. -
Supergravity Backgrounds and Symmetry Superalgebras
Turkish Journal of Physics Turk J Phys (2016) 40: 113 { 126 http://journals.tubitak.gov.tr/physics/ ⃝c TUB¨ ITAK_ Review Article doi:10.3906/fiz-1510-8 Supergravity backgrounds and symmetry superalgebras Umit¨ ERTEM∗ School of Mathematics, College of Science and Engineering, The University of Edinburgh, Edinburgh, United Kingdom Received: 12.10.2015 • Accepted/Published Online: 08.12.2015 • Final Version: 27.04.2016 Abstract: We consider the bosonic sectors of supergravity theories in ten and eleven dimensions corresponding to the low energy limits of string theories and M-theory. The solutions of supergravity field equations are known as supergravity backgrounds and the number of preserved supersymmetries in those backgrounds are determined by Killing spinors. We provide some examples of supergravity backgrounds that preserve different fractions of supersymmetry. An important invariant for the characterization of supergravity backgrounds is their Killing superalgebras, which are constructed out of Killing vectors and Killing spinors of the background. After constructing Killing superalgebras of some special supergravity backgrounds, we discuss the possibilities of the extensions of these superalgebras to include the higher degree hidden symmetries of the background. Key words: Supergravity backgrounds, Killing spinors, Killing superalgebras 1. Introduction The unification of fundamental forces of nature is one of the biggest aims in modern theoretical physics. The most promising approaches for that aim include the ten-dimensional supersymmetric string theories and their eleven-dimensional unification called M-theory. There are five different string theories in ten dimensions: type I, type IIA and IIB, and heterotic E8 × E8 and SO(32) theories. However, some dualities called T-duality, S-duality, and U-duality between strong coupling and weak coupling limits of these theories can be defined and these dualities can give rise to one unified M-theory in eleven dimensions [1, 2, 3, 4]. -
Representations of Centrally Extended Lie Superalgebra $\Mathfrak {Psl}(2
Representations of centrally extended Lie superalgebra psl(2|2) Takuya Matsumoto and Alexander Molev Abstract The symmetries provided by representations of the centrally extended Lie su- peralgebra psl(2|2) are known to play an important role in the spin chain models originated in the planar anti-de Sitter/conformal field theory correspondence and one- dimensional Hubbard model. We give a complete description of finite-dimensional irreducible representations of this superalgebra thus extending the work of Beisert which deals with a generic family of representations. Our description includes a new class of modules with degenerate eigenvalues of the central elements. Moreover, we construct explicit bases in all irreducible representations by applying the techniques of Mickelsson–Zhelobenko algebras. arXiv:1405.3420v2 [math.RT] 15 Sep 2014 Institute for Theoretical Physics and Spinoza Institute Utrecht University, Leuvenlaan 4, 3854 CE Utrecht, The Netherlands [email protected] School of Mathematics and Statistics University of Sydney, NSW 2006, Australia [email protected] 1 1 Introduction As discovered by Beisert [1, 2, 3], certain spin chain models originated in the planar anti-de Sitter/conformal field theory (AdS/CFT) correspondence admit hidden symmetries pro- vided by the action of the Yangian Y(g) associated with the centrally extended Lie super- algebra g = psl(2|2) ⋉C3. This is a semi-direct product of the simple Lie superalgebra psl(2|2) of type A(1, 1) and the abelian Lie algebra C3 spanned by elements C, K and P which are central in g. Due to the results of [6], psl(2|2) is distinguished among the basic classical Lie superalgebras by the existence of a three-dimensional central extension. -
Classification of Simple Linearly Compact N-Lie Superalgebras
Classification of simple linearly compact n-Lie superalgebras The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Cantarini, Nicoletta, and Victor G. Kac. “Classification of Simple Linearly Compact n-Lie Superalgebras.” Communications in Mathematical Physics 298.3 (2010): 833–853. Web. As Published http://dx.doi.org/10.1007/s00220-010-1049-0 Publisher Springer-Verlag Version Author's final manuscript Citable link http://hdl.handle.net/1721.1/71610 Terms of Use Creative Commons Attribution-Noncommercial-Share Alike 3.0 Detailed Terms http://creativecommons.org/licenses/by-nc-sa/3.0/ Classification of simple linearly compact n-Lie superalgebras Nicoletta Cantarini∗ Victor G. Kac∗∗ Abstract We classify simple linearly compact n-Lie superalgebras with n> 2 over a field F of charac- teristic 0. The classification is based on a bijective correspondence between non-abelian n-Lie Z n−1 superalgebras and transitive -graded Lie superalgebras of the form L = ⊕j=−1Lj, where dim Ln−1 = 1, L−1 and Ln−1 generate L, and [Lj ,Ln−j−1] = 0 for all j, thereby reducing it to the known classification of simple linearly compact Lie superalgebras and their Z-gradings. The list consists of four examples, one of them being the n+1-dimensional vector product n-Lie algebra, and the remaining three infinite-dimensional n-Lie algebras. Introduction Given an integer n ≥ 2, an n-Lie algebra g is a vector space over a field F, endowed with an n-ary anti-commutative product n Λ g → g , a1 ∧ . -
DIFFERENTIAL ALGEBRA Lecturer: Alexey Ovchinnikov Thursdays 9
DIFFERENTIAL ALGEBRA Lecturer: Alexey Ovchinnikov Thursdays 9:30am-11:40am Website: http://qcpages.qc.cuny.edu/˜aovchinnikov/ e-mail: [email protected] written by: Maxwell Shapiro 0. INTRODUCTION There are two main topics we will discuss in these lectures: (I) The core differential algebra: (a) Introduction: We will begin with an introduction to differential algebraic structures, important terms and notation, and a general background needed for this lecture. (b) Differential elimination: Given a system of polynomial partial differential equations (PDE’s for short), we will determine if (i) this system is consistent, or if (ii) another polynomial PDE is a consequence of the system. (iii) If time permits, we will also discuss algorithms will perform (i) and (ii). (II) Differential Galois Theory for linear systems of ordinary differential equations (ODE’s for short). This subject deals with questions of this sort: Given a system d (?) y(x) = A(x)y(x); dx where A(x) is an n × n matrix, find all algebraic relations that a solution of (?) can possibly satisfy. Hrushovski developed an algorithm to solve this for any A(x) with entries in Q¯ (x) (here, Q¯ is the algebraic closure of Q). Example 0.1. Consider the ODE dy(x) 1 = y(x): dx 2x p We know that y(x) = x is a solution to this equation. As such, we can determine an algebraic relation to this ODE to be y2(x) − x = 0: In the previous example, we solved the ODE to determine an algebraic relation. Differential Galois Theory uses methods to find relations without having to solve. -
Differential Graded Lie Algebras and Deformation Theory
Differential graded Lie algebras and Deformation theory Marco Manetti 1 Differential graded Lie algebras Let L be a lie algebra over a fixed field K of characteristic 0. Definition 1. A K-linear map d : L ! L is called a derivation if it satisfies the Leibniz rule d[a; b] = [da; b]+[a; db]. n d P dn Lemma. If d is nilpotent (i.e. d = 0 for n sufficiently large) then e = n≥0 n! : L ! L is an isomorphism of Lie algebras. Proof. Exercise. Definition 2. L is called nilpotent if the descending central series L ⊃ [L; L] ⊃ [L; [L; L]] ⊃ · · · stabilizes at 0. (I.e., if we write [L]2 = [L; L], [L]3 = [L; [L; L]], etc., then [L]n = 0 for n sufficiently large.) Note that in the finite-dimensional case, this is equivalent to the other common definition that for every x 2 L, adx is nilpotent. We have the Baker-Campbell-Hausdorff formula (BCH). Theorem. For every nilpotent Lie algebra L there is an associative product • : L × L ! L satisfying 1. functoriality in L; i.e. if f : L ! M is a morphism of nilpotent Lie algebras then f(a • b) = f(a) • f(b). a P an 2. If I ⊂ R is a nilpotent ideal of the associative unitary K-algebra R and for a 2 I we define e = n≥0 n! 2 R, then ea•b = ea • eb. Heuristically, we can write a • b = log(ea • eb). Proof. Exercise (use the computation of www.mat.uniroma1.it/people/manetti/dispense/BCHfjords.pdf and the existence of free Lie algebras). -
Scientific Report for the Year 2000
The Erwin Schr¨odinger International Boltzmanngasse 9 ESI Institute for Mathematical Physics A-1090 Wien, Austria Scientific Report for the Year 2000 Vienna, ESI-Report 2000 March 1, 2001 Supported by Federal Ministry of Education, Science, and Culture, Austria ESI–Report 2000 ERWIN SCHRODINGER¨ INTERNATIONAL INSTITUTE OF MATHEMATICAL PHYSICS, SCIENTIFIC REPORT FOR THE YEAR 2000 ESI, Boltzmanngasse 9, A-1090 Wien, Austria March 1, 2001 Honorary President: Walter Thirring, Tel. +43-1-4277-51516. President: Jakob Yngvason: +43-1-4277-51506. [email protected] Director: Peter W. Michor: +43-1-3172047-16. [email protected] Director: Klaus Schmidt: +43-1-3172047-14. [email protected] Administration: Ulrike Fischer, Eva Kissler, Ursula Sagmeister: +43-1-3172047-12, [email protected] Computer group: Andreas Cap, Gerald Teschl, Hermann Schichl. International Scientific Advisory board: Jean-Pierre Bourguignon (IHES), Giovanni Gallavotti (Roma), Krzysztof Gawedzki (IHES), Vaughan F.R. Jones (Berkeley), Viktor Kac (MIT), Elliott Lieb (Princeton), Harald Grosse (Vienna), Harald Niederreiter (Vienna), ESI preprints are available via ‘anonymous ftp’ or ‘gopher’: FTP.ESI.AC.AT and via the URL: http://www.esi.ac.at. Table of contents General remarks . 2 Winter School in Geometry and Physics . 2 Wolfgang Pauli und die Physik des 20. Jahrhunderts . 3 Summer Session Seminar Sophus Lie . 3 PROGRAMS IN 2000 . 4 Duality, String Theory, and M-theory . 4 Confinement . 5 Representation theory . 7 Algebraic Groups, Invariant Theory, and Applications . 7 Quantum Measurement and Information . 9 CONTINUATION OF PROGRAMS FROM 1999 and earlier . 10 List of Preprints in 2000 . 13 List of seminars and colloquia outside of conferences . -
Kac-Moody Algebras and Applications
Kac-Moody Algebras and Applications Owen Barrett December 24, 2014 Abstract This article is an introduction to the theory of Kac-Moody algebras: their genesis, their con- struction, basic theorems concerning them, and some of their applications. We first record some of the classical theory, since the Kac-Moody construction generalizes the theory of simple finite-dimensional Lie algebras in a closely analogous way. We then introduce the construction and properties of Kac-Moody algebras with an eye to drawing natural connec- tions to the classical theory. Last, we discuss some physical applications of Kac-Moody alge- bras,includingtheSugawaraandVirosorocosetconstructions,whicharebasictoconformal field theory. Contents 1 Introduction2 2 Finite-dimensional Lie algebras3 2.1 Nilpotency.....................................3 2.2 Solvability.....................................4 2.3 Semisimplicity...................................4 2.4 Root systems....................................5 2.4.1 Symmetries................................5 2.4.2 The Weyl group..............................6 2.4.3 Bases...................................6 2.4.4 The Cartan matrix.............................7 2.4.5 Irreducibility...............................7 2.4.6 Complex root systems...........................7 2.5 The structure of semisimple Lie algebras.....................7 2.5.1 Cartan subalgebras............................8 2.5.2 Decomposition of g ............................8 2.5.3 Existence and uniqueness.........................8 2.6 Linear representations of complex semisimple Lie algebras...........9 2.6.1 Weights and primitive elements.....................9 2.7 Irreducible modules with a highest weight....................9 2.8 Finite-dimensional modules............................ 10 3 Kac-Moody algebras 10 3.1 Basic definitions.................................. 10 3.1.1 Construction of the auxiliary Lie algebra................. 11 3.1.2 Construction of the Kac-Moody algebra................. 12 3.1.3 Root space of the Kac-Moody algebra g(A) .............. -
World-Sheet Supersymmetry and Supertargets
Motivation World-Sheet SUSY Lie superalgebras From World-Sheet SUSY to Supertargets Outlook World-sheet supersymmetry and supertargets Peter Browne Rønne University of the Witwatersrand, Johannesburg Chapel Hill, August 19, 2010 arXiv:1006.5874 Thomas Creutzig, PR Motivation World-Sheet SUSY Lie superalgebras From World-Sheet SUSY to Supertargets Outlook Sigma-models on supergroups/cosets The Wess-Zumino-Novikov-Witten (WZNW) model of a Lie supergroup is a CFT with additional affine Lie superalgebra symmetry. Important role in physics • Statistical systems • String theory, AdS/CFT Notoriously hard: Deformations away from WZNW-point Use and explore the rich structure of dualities and correspondences in 2d field theories Motivation World-Sheet SUSY Lie superalgebras From World-Sheet SUSY to Supertargets Outlook Sigma models on supergroups: AdS/CFT The group of global symmetries of the gauge theory and also of the dual string theory is a Lie supergroup G. The dual string theory is described by a two-dimensional sigma model on a superspace. PSU(2; 2j4) AdS × S5 supercoset 5 SO(4; 1) × SO(5) PSU(1; 1j2) AdS × S2 supercoset 2 U(1) × U(1) 3 AdS3 × S PSU(1; 1j2) supergroup 3 3 AdS3 × S × S D(2; 1; α) supergroup Obtained using GS or hybrid formalism. What about RNS formalism? And what are the precise relations? Motivation World-Sheet SUSY Lie superalgebras From World-Sheet SUSY to Supertargets Outlook 3 4 AdS3 × S × T D1-D5 brane system on T 4 with near-horizon limit 3 4 AdS3 × S × T . After S-duality we have N = (1; 1) WS SUSY WZNW model on SL(2) × SU(2) × U4. -
About Lie-Rinehart Superalgebras Claude Roger
About Lie-Rinehart superalgebras Claude Roger To cite this version: Claude Roger. About Lie-Rinehart superalgebras. 2019. hal-02071706 HAL Id: hal-02071706 https://hal.archives-ouvertes.fr/hal-02071706 Preprint submitted on 18 Mar 2019 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. About Lie-Rinehart superalgebras Claude Rogera aInstitut Camille Jordan ,1 , Universit´ede Lyon, Universit´eLyon I, 43 boulevard du 11 novembre 1918, F-69622 Villeurbanne Cedex, France Keywords:Supermanifolds, Lie-Rinehart algebras, Fr¨olicher-Nijenhuis bracket, Nijenhuis-Richardson bracket, Schouten-Nijenhuis bracket. Mathematics Subject Classification (2010): .17B35, 17B66, 58A50 Abstract: We extend to the superalgebraic case the theory of Lie-Rinehart algebras and work out some examples concerning the most popular samples of supermanifolds. 1 Introduction The goal of this article is to discuss some properties of Lie-Rinehart structures in a superalgebraic context. Let's first sketch the classical case; a Lie-Rinehart algebra is a couple (A; L) where L is a Lie algebra on a base field k, A an associative and commutative k-algebra, with two operations 1. (A; L) ! L denoted by (a; X) ! aX, which induces a A-module structure on L, and 2.