${\Mathbb Z} 2\Times {\Mathbb Z} 2 $-Graded Parastatistics In
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Probability and Statistics, Parastatistics, Boson, Fermion, Parafermion, Hausdorff Dimension, Percolation, Clusters
Applied Mathematics 2018, 8(1): 5-8 DOI: 10.5923/j.am.20180801.02 Why Fermions and Bosons are Observable as Single Particles while Quarks are not? Sencer Taneri Private Researcher, Turkey Abstract Bosons and Fermions are observable in nature while Quarks appear only in triplets for matter particles. We find a theoretical proof for this statement in this paper by investigating 2-dim model. The occupation numbers q are calculated by a power law dependence of occupation probability and utilizing Hausdorff dimension for the infinitely small mesh in the phase space. The occupation number for Quarks are manipulated and found to be equal to approximately three as they are Parafermions. Keywords Probability and Statistics, Parastatistics, Boson, Fermion, Parafermion, Hausdorff dimension, Percolation, Clusters There may be particles that obey some kind of statistics, 1. Introduction generally called parastatistics. The Parastatistics proposed in 1952 by H. Green was deduced using a quantum field The essential difference in classical and quantum theory (QFT) [2, 3]. Whenever we discover a new particle, descriptions of N identical particles is in their individuality, it is almost certain that we attribute its behavior to the rather than in their indistinguishability [1]. Spin of the property that it obeys some form of parastatistics and the particle is one of its intrinsic physical quantity that is unique maximum occupation number q of a given quantum state to its individuality. The basis for how the quantum states for would be a finite number that could assume any integer N identical particles will be occupied may be taken as value as 1<q <∞ (see Table 1). -
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). -
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. -
Physics Abstracts CLASSIFICATION and CONTENTS (PACC)
Physics Abstracts CLASSIFICATION AND CONTENTS (PACC) 0000 general 0100 communication, education, history, and philosophy 0110 announcements, news, and organizational activities 0110C announcements, news, and awards 0110F conferences, lectures, and institutes 0110H physics organizational activities 0130 physics literature and publications 0130B publications of lectures(advanced institutes, summer schools, etc.) 0130C conference proceedings 0130E monographs, and collections 0130K handbooks and dictionaries 0130L collections of physical data, tables 0130N textbooks 0130Q reports, dissertations, theses 0130R reviews and tutorial papers;resource letters 0130T bibliographies 0140 education 0140D course design and evaluation 0140E science in elementary and secondary school 0140G curricula, teaching methods,strategies, and evaluation 0140J teacher training 0150 educational aids(inc. equipment,experiments and teaching approaches to subjects) 0150F audio and visual aids, films 0150H instructional computer use 0150K testing theory and techniques 0150M demonstration experiments and apparatus 0150P laboratory experiments and apparatus 0150Q laboratory course design,organization, and evaluation 0150T buildings and facilities 0155 general physics 0160 biographical, historical, and personal notes 0165 history of science 0170 philosophy of science 0175 science and society 0190 other topics of general interest 0200 mathematical methods in physics 0210 algebra, set theory, and graph theory 0220 group theory(for algebraic methods in quantum mechanics, see -
Lectures on Supersymmetry and Superstrings 1 General Superalgebra
Lectures on supersymmetry and superstrings Thomas Mohaupt Abstract: These are informal notes on some mathematical aspects of su- persymmetry, based on two ‘Mathematics and Theoretical Physics Meetings’ in the Autumn Term 2009.1 First super vector spaces, Lie superalgebras and su- percommutative associative superalgebras are briefly introduced together with superfunctions and superspaces. After a review of the Poincar´eLie algebra we discuss Poincar´eLie superalgebras and introduce Minkowski superspaces. As a minimal example of a supersymmetric model we discuss the free scalar superfield in two-dimensional N = (1, 1) supersymmetry (this is more or less copied from [1]). We briefly discuss the concept of chiral supersymmetry in two dimensions. None of the material is original. We give references for further reading. Some ‘bonus material’ on (super-)conformal field theories, (super-)string theories and symmetric spaces is included. These are topics which will play a role in future meetings, or which came up briefly during discussions. 1 General superalgebra Definition: A super vector space V is a vector space with a decomposition V = V V 0 ⊕ 1 and a map (parity map) ˜ : (V V ) 0 Z · 0 ∪ 1 −{ } → 2 which assigns even or odd parity to every homogeneous element. Notation: a V a˜ =0 , ‘even’ , b V ˜b = 1 ‘odd’ . ∈ 0 → ∈ 1 → Definition: A Lie superalgebra g (also called super Lie algebra) is a super vector space g = g g 0 ⊕ 1 together with a bracket respecting the grading: [gi , gj] gi j ⊂ + (addition of index mod 2), which is required to be Z2 graded anti-symmetric: ˜ [a,b]= ( 1)a˜b[b,a] − − (multiplication of parity mod 2), and to satisfy a Z2 graded Jacobi identity: ˜ [a, [b,c]] = [[a,b],c] + ( 1)a˜b[b, [a,c]] . -
The Conventionality of Parastatistics
The Conventionality of Parastatistics David John Baker Hans Halvorson Noel Swanson∗ March 6, 2014 Abstract Nature seems to be such that we can describe it accurately with quantum theories of bosons and fermions alone, without resort to parastatistics. This has been seen as a deep mystery: paraparticles make perfect physical sense, so why don't we see them in nature? We consider one potential answer: every paraparticle theory is physically equivalent to some theory of bosons or fermions, making the absence of paraparticles in our theories a matter of convention rather than a mysterious empirical discovery. We argue that this equivalence thesis holds in all physically admissible quantum field theories falling under the domain of the rigorous Doplicher-Haag-Roberts approach to superselection rules. Inadmissible parastatistical theories are ruled out by a locality- inspired principle we call Charge Recombination. Contents 1 Introduction 2 2 Paraparticles in Quantum Theory 6 ∗This work is fully collaborative. Authors are listed in alphabetical order. 1 3 Theoretical Equivalence 11 3.1 Field systems in AQFT . 13 3.2 Equivalence of field systems . 17 4 A Brief History of the Equivalence Thesis 20 4.1 The Green Decomposition . 20 4.2 Klein Transformations . 21 4.3 The Argument of Dr¨uhl,Haag, and Roberts . 24 4.4 The Doplicher-Roberts Reconstruction Theorem . 26 5 Sharpening the Thesis 29 6 Discussion 36 6.1 Interpretations of QM . 44 6.2 Structuralism and Haecceities . 46 6.3 Paraquark Theories . 48 1 Introduction Our most fundamental theories of matter provide a highly accurate description of subatomic particles and their behavior. -
Dimension Formula for Graded Lie Algebras and Its Applications
TRANSACTIONS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 351, Number 11, Pages 4281–4336 S 0002-9947(99)02239-4 Article electronically published on June 29, 1999 DIMENSION FORMULA FOR GRADED LIE ALGEBRAS AND ITS APPLICATIONS SEOK-JIN KANG AND MYUNG-HWAN KIM Abstract. In this paper, we investigate the structure of infinite dimensional Lie algebras L = α Γ Lα graded by a countable abelian semigroup Γ sat- isfying a certain finiteness∈ condition. The Euler-Poincar´e principle yields the denominator identitiesL for the Γ-graded Lie algebras, from which we derive a dimension formula for the homogeneous subspaces Lα (α Γ). Our dimen- sion formula enables us to study the structure of the Γ-graded2 Lie algebras in a unified way. We will discuss some interesting applications of our dimension formula to the various classes of graded Lie algebras such as free Lie algebras, Kac-Moody algebras, and generalized Kac-Moody algebras. We will also dis- cuss the relation of graded Lie algebras and the product identities for formal power series. Introduction In [K1] and [Mo1], Kac and Moody independently introduced a new class of Lie algebras, called Kac-Moody algebras, as a generalization of finite dimensional simple Lie algebras over C. These algebras are ususally infinite dimensional, and are defined by the generators and relations associated with generalized Cartan matrices, which is similar to Serre’s presentation of complex semisimple Lie algebras. In [M], by generalizing Weyl’s denominator identity to the affine root system, Macdonald obtained a new family of combinatorial identities, including Jacobi’s triple product identity as the simplest case. -
Z-Graded Lie Superalgebras of Infinite Depth and Finite Growth 547
Ann. Scuola Norm. Sup. Pisa Cl. Sci. (5) Vol. I (2002), pp. 545-568 Z-graded Lie Superalgebras of Infinite Depth and Finite Growth NICOLETTA CANTARINI Abstract. In 1998 Victor Kac classified infinite-dimensional Z-graded Lie su- peralgebras of finite depth. We construct new examples of infinite-dimensional Lie superalgebras with a Z-gradation of infinite depth and finite growth and clas- sify Z-graded Lie superalgebras of infinite depth and finite growth under suitable hypotheses. Mathematics Subject Classification (2000): 17B65 (primary), 17B70 (secondary). Introduction Simple finite-dimensional Lie superalgebras were classified by V. G. Kac in [K2]. In the same paper Kac classified the finite-dimensional, Z-graded Lie superalgebras under the hypotheses of irreducibility and transitivity. The classification of infinite-dimensional, Z-graded Lie superalgebras of finite depth is also due to V. G. Kac [K3] and is deeply related to the classifi- cation of linearly compact Lie superalgebras. We recall that finite depth implies finite growth. This naturally leads to investigate infinite-dimensional, Z-graded Lie super- algebras of infinite depth and finite growth. The hypothesis of finite growth is central to the problem; indeed, it is well known that it is not possible to classify Z-graded Lie algebras (and thus Lie superalgebras) of any growth (see [K1], [M]). The only known examples of infinite-dimensional, Z-graded Lie superalgebras of finite growth and infinite depth are given by contragredient Lie superalgebras which were classified by V. G. Kac in [K2] in the case of finite dimension and by J.W. van de Leur in the general case [vdL]. -
Graded Lie Algebras and Representations of Supersymmetry Algebras Physics 251 Group Theory and Modern Physics
Graded Lie Algebras and Representations of Supersymmetry Algebras Physics 251 Group Theory and Modern Physics Jaryd Franklin Ulbricht June 14, 2017 J. F. Ulbricht Graded Lie Algebras and SUSY June 14, 2017 1 / 50 Overview 1 Introduction and Definitions Linear Vector Spaces Linear Algebras Lie Algebras 2 Graded Algebras Graded Lie Algebras 3 Supersymmetry Lie Superalgebras Superspace Supersymmetry Algebras 4 Representations of Supersymmetry Algebras Boson and Fermion Number Constructing Massive Representations Constructing Massless Representations J. F. Ulbricht Graded Lie Algebras and SUSY June 14, 2017 2 / 50 How do we construct a graded algebra? It's actually much easier than you think Graded Lie Algebras What is a graded algebra? J. F. Ulbricht Graded Lie Algebras and SUSY June 14, 2017 3 / 50 It's actually much easier than you think Graded Lie Algebras What is a graded algebra? How do we construct a graded algebra? J. F. Ulbricht Graded Lie Algebras and SUSY June 14, 2017 3 / 50 Graded Lie Algebras What is a graded algebra? How do we construct a graded algebra? It's actually much easier than you think J. F. Ulbricht Graded Lie Algebras and SUSY June 14, 2017 3 / 50 Graded Lie Algebras su (2) J. F. Ulbricht Graded Lie Algebras and SUSY June 14, 2017 4 / 50 Graded Lie Algebras su (2) J. F. Ulbricht Graded Lie Algebras and SUSY June 14, 2017 4 / 50 Graded Lie Algebras so (3) J. F. Ulbricht Graded Lie Algebras and SUSY June 14, 2017 5 / 50 Graded Lie Algebras so (3) J. F. Ulbricht Graded Lie Algebras and SUSY June 14, 2017 5 / 50 Graded Lie Algebras E6 J. -
Arxiv:1806.10485V2 [Math.RA] 13 Mar 2019 Product 1.2
ON JORDAN DOUBLES OF SLOW GROWTH OF LIE SUPERALGEBRAS VICTOR PETROGRADSKY AND I.P. SHESTAKOV Abstract. To an arbitrary Lie superalgebra L we associate its Jordan double J or(L), which is a Jordan su- peralgebra. This notion was introduced by the second author before [45]. Now we study further applications of this construction. First, we show that the Gelfand-Kirillov dimension of a Jordan superalgebra can be an arbitrary number {0}∪[1, +∞]. Thus, unlike the associative and Jordan algebras [23, 25], one hasn’t an analogue of Bergman’s gap (1, 2) for the Gelfand-Kirillov dimension of Jordan superalgebras. Second, using the Lie superalgebra R of [9], we construct a Jordan superalgebra J = J or(R) that is nil finely Z3-graded (moreover, the components are at most one-dimensional), the field being of characteristic not 2. This example is in contrast with non-existence of such examples (roughly speaking, analogues of the Grigorchuk and Gupta-Sidki groups) of Lie algebras in characteristic zero [26] and Jordan algebras in characteristic not 2 [50]. Also, J is just infinite but not hereditary just infinite. A similar Jordan superalgebra of slow polynomial growth was constructed before [39]. The virtue of the present example is that it is of linear growth, of finite width 4, namely, its N-gradation by degree in the generators has components of dimensions {0, 2, 3, 4}, and the sequence of these dimensions is non-periodic. Third, we review constructions of Poisson and Jordan superalgebras of [39] starting with another example of a Lie superalgebra introduced in [32]. -
Graded Modules Over the Simple Lie Algebra Sl2(C)
Graded modules over the simple Lie algebra sl2(C) by c Abdallah A. Shihadeh A thesis submitted to the School of Graduate Studies in partial fulfilment of the requirements for the degree of Doctor of Philosophy Department of Mathematics and Statistics Memorial University of Newfoundland 2019 St. John's Newfoundland Abstract This thesis provides a contribution to the area of group gradings on the simple modules over simple Lie algebras. A complete classification of gradings on finite- dimensional simple modules over arbitrary finite-dimensional simple Lie algebras over algebraically closed fields of characteristic zero, in terms of graded Brauer groups, has been recently given in the papers of A. Elduque and M. Kochetov. Here we concen- trate on infinite-dimensional modules. A complete classification by R. Block of all simple modules over a simple Lie algebra is known only in the case of sl2(C). Thus, we restrict ourselves to the gradings on simple sl2(C)-modules. We first give a full 2 description for the Z- and Z2-gradings of all weight modules over sl2(C). Then we show that Z-gradings do not exist on any torsion-free sl2(C)-modules of finite rank. 2 After this, we treat Z2-gradings on torsion-free modules of various ranks. A construc- tion for these modules was given by V. Bavula, and J. Nilson gave a classification of the torsion-free sl2(C)-modules of rank 1. After giving some, mostly negative, results about the gradings on these latter modules, we construct the first family of simple 2 Z2-graded sl2(C)-modules (of rank 2). -
On the Centre of Graded Lie Algebras Astérisque, Tome 113-114 (1984), P
Astérisque CLAS LÖFWALL On the centre of graded Lie algebras Astérisque, tome 113-114 (1984), p. 263-267 <http://www.numdam.org/item?id=AST_1984__113-114__263_0> © Société mathématique de France, 1984, tous droits réservés. L’accès aux archives de la collection « Astérisque » (http://smf4.emath.fr/ Publications/Asterisque/) implique l’accord avec les conditions générales d’uti- lisation (http://www.numdam.org/conditions). Toute utilisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ ON THE CENTRE OF GRADED LIE ALGEBRAS by Clas Löfwall If a, is a graded Lie algebra over a field k in general, its centre may of course be any abelian graded Lie algebra. But if some restrictions are imposed on a. such as 1) cd(a) (= gldim U(a) ) < °° 2) U(a) = Ext^Ckjk) R local noetherian ring — ft 00 3) a = TT^S ® Q , catQ(S) < what can be said about the centre? Notation. For a graded Lie algebra a , let Z(a.) denote its centre. Felix, Halperin and Thomas have results in case 3) (cf [1]): Suppose dim (a)=0 0 2k-" then for each k>1 , dimQ(Z2n(a)) < cat0(S). n=k In case 1) we have the following result. Theorem 1 Suppose cd(a) = n < <». Then dim^Z(a) _< n and Zo^(a) - 0 . Moreover if dim^zCa) = n , then a is an extension of an abelian Lie algebra on odd generators by its centre Z(a).