The Structure of Superqubit States
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Arxiv:2009.05574V4 [Hep-Th] 9 Nov 2020 Predict a New Massless Spin One Boson [The ‘Lorentz’ Boson] Which Should Be Looked for in Experiments
Trace dynamics and division algebras: towards quantum gravity and unification Tejinder P. Singh Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai 400005, India e-mail: [email protected] Accepted for publication in Zeitschrift fur Naturforschung A on October 4, 2020 v4. Submitted to arXiv.org [hep-th] on November 9, 2020 ABSTRACT We have recently proposed a Lagrangian in trace dynamics at the Planck scale, for unification of gravitation, Yang-Mills fields, and fermions. Dynamical variables are described by odd- grade (fermionic) and even-grade (bosonic) Grassmann matrices. Evolution takes place in Connes time. At energies much lower than Planck scale, trace dynamics reduces to quantum field theory. In the present paper we explain that the correct understanding of spin requires us to formulate the theory in 8-D octonionic space. The automorphisms of the octonion algebra, which belong to the smallest exceptional Lie group G2, replace space- time diffeomorphisms and internal gauge transformations, bringing them under a common unified fold. Building on earlier work by other researchers on division algebras, we propose the Lorentz-weak unification at the Planck scale, the symmetry group being the stabiliser group of the quaternions inside the octonions. This is one of the two maximal sub-groups of G2, the other one being SU(3), the element preserver group of octonions. This latter group, coupled with U(1)em, describes the electro-colour symmetry, as shown earlier by Furey. We arXiv:2009.05574v4 [hep-th] 9 Nov 2020 predict a new massless spin one boson [the `Lorentz' boson] which should be looked for in experiments. -
NP As Minimization of Degree 4 Polynomial, Integration Or Grassmann Number Problem, and New Graph Isomorphism Problem Approac
1 P?=NP as minimization of degree 4 polynomial, integration or Grassmann number problem, and new graph isomorphism problem approaches Jarek Duda Jagiellonian University, Golebia 24, 31-007 Krakow, Poland, Email: [email protected] Abstract—While the P vs NP problem is mainly approached problem, vertex cover problem, independent set problem, form the point of view of discrete mathematics, this paper subset sum problem, dominating set problem and graph proposes reformulations into the field of abstract algebra, ge- coloring problem. All of them stay in widely understood ometry, fourier analysis and of continuous global optimization - which advanced tools might bring new perspectives and field of discrete mathematics, like combinatorics, graph approaches for this question. The first one is equivalence of theory, logic. satisfaction of 3-SAT problem with the question of reaching The unsuccessfulness of a half century search for zero of a nonnegative degree 4 multivariate polynomial (sum the answer might suggest to try to look out of this of squares), what could be tested from the perspective of relatively homogeneous field - try to apply advances algebra by using discriminant. It could be also approached as a continuous global optimization problem inside [0; 1]n, of more distant fields of mathematics, like abstract for example in physical realizations like adiabatic quantum algebra fluent in working with the ring of polynomials, computers. However, the number of local minima usually use properties of multidimensional geometry, or other grows exponentially. Reducing to degree 2 polynomial plus continuous mathematics including numerical methods n constraints of being in f0; 1g , we get geometric formulations perfecting approaches for common problem of continuous as the question if plane or sphere intersects with f0; 1gn. -
Gaussian Operator Bases for Correlated Fermions
Gaussian operator bases for correlated fermions J. F. Corney and P. D. Drummond ARC Centre of Excellence for Quantum-Atom Optics, University of Queensland, Brisbane 4072, Queensland, Australia. (Dated: 19th October 2018) We formulate a general multi-mode Gaussian operator basis for fermions, to enable a positive phase-space representation of correlated Fermi states. The Gaussian basis extends existing bosonic phase-space methods to Fermi systems and thus enables first-principles dynamical or equilibrium calculations in quantum many-body Fermi systems. We prove the completeness and positivity of the basis, and derive differential forms for products with one- and two-body operators. Because the basis satisfies fermionic superselection rules, the resulting phase space involves only c-numbers, without requiring anti-commuting Grassmann variables. I. INTRODUCTION integrals, except that here the Gaussian basis is used to expand the fermionic states themselves, rather than a In this paper we address the issue of how to represent path integral, which has advantages in terms of giving a highly correlated fermionic states, for the purposes of ef- greater physical understanding and fewer restrictions in ficient calculations in fermionic many-body physics. To the resulting applications. this end, we introduce a normally ordered Gaussian op- To begin, we establish in Sec. II the definition of a erator basis for fermionic density operators. With this Gaussian operator in unnormalised form, and follow this basis, earlier phase-space techniques used to represent in Sec. III with elementary examples of one- and two- atomic transitions[1, 2] can be extended to general Fermi mode Gaussians in order to illustrate the basic structure systems. -
Classical and Quantum Mechanics Via Supermetrics in Time
Noname manuscript No. (will be inserted by the editor) E. GOZZI Classical and Quantum Mechanics via Supermetrics in Time the date of receipt and acceptance should be inserted later Abstract Koopman-von Neumann in the 30’s gave an operatorial formul- ulation of Classical Mechancs. It was shown later on that this formulation could also be written in a path-integral form. We will label this functional ap- proach as CPI (for classical path-integral) to distinguish it from the quantum mechanical one, which we will indicate with QPI. In the CPI two Grassman- nian partners of time make their natural appearance and in this manner time becomes something like a three dimensional supermanifold. Next we intro- duce a metric in this supermanifold and show that a particular choice of the supermetric reproduces the CPI while a different one gives the QPI. Keywords quantum mechanics, classical mechanics, supermetric,path- integral 1 INTRODUCTION. The topic of this conference has been Spin-Statistics. One of the things which is most difficult to accept to our common sense is the anticommuting nature of Fermions. Actually anticommuting variables have a long history that goes back to Grassmann [1] and are not strictly related to spin. Grassmann in- vented them for abstract reasons but he discovered that they are usefull in the description of ruled surfaces. Later on the exterior product introduced arXiv:0910.1812v1 [quant-ph] 9 Oct 2009 by Grassmann was used in the field of differential forms by Cartan. Grass- mannian variables have made their appearance in -
On Supermatrix Operator Semigroups 1. Introduction
Quasigroups and Related Systems 7 (2000), 71 − 88 On supermatrix operator semigroups Steven Duplij Abstract One-parameter semigroups of antitriangle idempotent su- permatrices and corresponding superoperator semigroups are introduced and investigated. It is shown that t-linear idempo- tent superoperators and exponential superoperators are mutu- ally dual in some sense, and the rst give additional to expo- nential dierent solution to the initial Cauchy problem. The corresponding functional equation and analog of resolvent are found for them. Dierential and functional equations for idem- potent (super)operators are derived for their general t power- type dependence. 1. Introduction Operator semigroups [1] play an important role in mathematical physics [2, 3, 4] viewed as a general theory of evolution systems [5, 6, 7]. Its development covers many new elds [8, 9, 10, 11], but one of vital for modern theoretical physics directions supersymmetry and related mathematical structures was not considered before in application to operator semigroup theory. The main dierence between previous considerations is the fact that among building blocks (e.g. elements of corresponding matrices) there exist noninvertible objects (divisors 2000 Mathematics Subject Classication: 25A50, 81Q60, 81T60 Keywords: Cauchy problem, idempotence, semigroup, supermatrix, superspace 72 S. Duplij of zero and nilpotents) which by themselves can form another semi- group. Therefore, we have to take that into account and investigate it properly, which can be called a semigroup × semigroup method. Here we study continuous supermatrix representations of idempo- tent operator semigroups rstly introduced in [12, 13] for bands. Usu- ally matrix semigroups are dened over a eld K [14] (on some non- supersymmetric generalizations of K-representations see [15, 16]). -
Howe Pairs, Supersymmetry, and Ratios of Random Characteristic
HOWE PAIRS, SUPERSYMMETRY, AND RATIOS OF RANDOM CHARACTERISTIC POLYNOMIALS FOR THE UNITARY GROUPS UN by J.B. Conrey, D.W. Farmer & M.R. Zirnbauer Abstract. — For the classical compact Lie groups K UN the autocorrelation functions of ratios of characteristic polynomials (z,w) Det(z≡ k)/Det(w k) are studied with k K as random variable. Basic to our treatment7→ is a property− shared− by the spinor repre- sentation∈ of the spin group with the Shale-Weil representation of the metaplectic group: in both cases the character is the analytic square root of a determinant or the reciprocal thereof. By combining this fact with Howe’s theory of supersymmetric dual pairs (g,K), we express the K-Haar average product of p ratios of characteristic polynomials and q conjugate ratios as a character χ which is associated with an irreducible representation of χ the Lie superalgebra g = gln n for n = p+q. The primitive character is shown to extend | to an analytic radial section of a real supermanifold related to gln n , and is computed by | invoking Berezin’s description of the radial parts of Laplace-Casimir operators for gln n . The final result for χ looks like a natural transcription of the Weyl character formula| to the context of highest-weight representations of Lie supergroups. While several other works have recently reproduced our results in the stable range N max(p,q), the present approach covers the full range of matrix dimensions N N. ≥To make this paper accessible to the non-expert reader, we have included a chapter∈ containing the required background material from superanalysis. -
Geometric Approaches to Quantum Field Theory
GEOMETRIC APPROACHES TO QUANTUM FIELD THEORY A thesis submitted to The University of Manchester for the degree of Doctor of Philosophy in the Faculty of Science and Engineering 2020 Kieran T. O. Finn School of Physics and Astronomy Supervised by Professor Apostolos Pilaftsis BLANK PAGE 2 Contents Abstract 7 Declaration 9 Copyright 11 Acknowledgements 13 Publications by the Author 15 1 Introduction 19 1.1 Unit Independence . 20 1.2 Reparametrisation Invariance in Quantum Field Theories . 24 1.3 Example: Complex Scalar Field . 25 1.4 Outline . 31 1.5 Conventions . 34 2 Field Space Covariance 35 2.1 Riemannian Geometry . 35 2.1.1 Manifolds . 35 2.1.2 Tensors . 36 2.1.3 Connections and the Covariant Derivative . 37 2.1.4 Distances on the Manifold . 38 2.1.5 Curvature of a Manifold . 39 2.1.6 Local Normal Coordinates and the Vielbein Formalism 41 2.1.7 Submanifolds and Induced Metrics . 42 2.1.8 The Geodesic Equation . 42 2.1.9 Isometries . 43 2.2 The Field Space . 44 2.2.1 Interpretation of the Field Space . 48 3 2.3 The Configuration Space . 50 2.4 Parametrisation Dependence of Standard Approaches to Quan- tum Field Theory . 52 2.4.1 Feynman Diagrams . 53 2.4.2 The Effective Action . 56 2.5 Covariant Approaches to Quantum Field Theory . 59 2.5.1 Covariant Feynman Diagrams . 59 2.5.2 The Vilkovisky–DeWitt Effective Action . 62 2.6 Example: Complex Scalar Field . 66 3 Frame Covariance in Quantum Gravity 69 3.1 The Cosmological Frame Problem . -
Super Fuzzy Matrices and Super Fuzzy Models for Social Scientists
SUPER FUZZY MATRICES AND SUPER FUZZY MODELS FOR SOCIAL SCIENTISTS W. B. Vasantha Kandasamy e-mail: [email protected] web: http://mat.iitm.ac.in/~wbv www.vasantha.net Florentin Smarandache e-mail: [email protected] K. Amal e-mail: [email protected] INFOLEARNQUEST Ann Arbor 2008 This book can be ordered in a paper bound reprint from: Books on Demand ProQuest Information & Learning (University of Microfilm International) 300 N. Zeeb Road P.O. Box 1346, Ann Arbor MI 48106-1346, USA Tel.: 1-800-521-0600 (Customer Service) http://wwwlib.umi.com/bod/ Peer reviewers: Dr. S. Osman, Menofia University, Shebin Elkom, Egypt Prof. Valentin Boju, Ph.D., Officer of the Order “Cultural Merit” Category — “Scientific Research” MontrealTech — Institut de Techologie de Montreal Director, MontrealTech Press, P.O. Box 78574 Station Wilderton, Montreal, Quebec, H3S2W9, Canada Prof. Mircea Eugen Selariu, Polytech University of Timisoara, Romania. Copyright 2008 by InfoLearnQuest and authors Cover Design and Layout by Kama Kandasamy Many books can be downloaded from the following Digital Library of Science: http://www.gallup.unm.edu/~smarandache/eBooks-otherformats.htm ISBN-10: 1-59973-027-8 ISBN-13: 978-1-59973-027-1 EAN: 9781599730271 Standard Address Number: 297-5092 Printed in the United States of America 2 CONTENTS Preface 5 Chapter One BASIC CONCEPTS 7 1.1 Supermatrices 7 1.2 Introduction of Fuzzy Matrices 65 Chapter Two FUZZY SUPERMATRICES AND THEIR PROPERTIES 75 2.1 Fuzzy Supermatrices and their Properties 75 2.2 Pseudo Symmetric Supermatrices 117 2.3 Special Operations on Fuzzy Super Special Row and Column Matrix 140 Chapter Three INTRODUCTION TO NEW FUZZY SUPER MODELS 167 3.1 New Super Fuzzy Relational Maps (SFRM) Model 167 3.2 New Fuzzy Super Bidirectional Associative Memories (BAM) model 176 3.3 Description of Super Fuzzy Associative Memories 188 3 3.4 Illustration of Super Fuzzy Models 199 3.5 Super FCM Models 236 FURTHER READING 247 INDEX 275 ABOUT THE AUTHORS 279 4 PREFACE The concept of supermatrix for social scientists was first introduced by Paul Horst. -
Interpreting Supersymmetry
Interpreting Supersymmetry David John Baker Department of Philosophy, University of Michigan [email protected] October 7, 2018 Abstract Supersymmetry in quantum physics is a mathematically simple phenomenon that raises deep foundational questions. To motivate these questions, I present a toy model, the supersymmetric harmonic oscillator, and its superspace representation, which adds extra anticommuting dimensions to spacetime. I then explain and comment on three foundational questions about this superspace formalism: whether superspace is a sub- stance, whether it should count as spatiotemporal, and whether it is a necessary pos- tulate if one wants to use the theory to unify bosons and fermions. 1 Introduction Supersymmetry{the hypothesis that the laws of physics exhibit a symmetry that transforms bosons into fermions and vice versa{is a long-standing staple of many popular (but uncon- firmed) theories in particle physics. This includes several attempts to extend the standard model as well as many research programs in quantum gravity, such as the failed supergravity program and the still-ascendant string theory program. Its popularity aside, supersymmetry (SUSY for short) is also a foundationally interesting hypothesis on face. The fundamental equivalence it posits between bosons and fermions is prima facie puzzling, given the very different physical behavior of these two types of particle. And supersymmetry is most naturally represented in a formalism (called superspace) that modifies ordinary spacetime by adding Grassmann-valued anticommuting coordinates. It 1 isn't obvious how literally we should interpret these extra \spatial" dimensions.1 So super- symmetry presents us with at least two highly novel interpretive puzzles. Only two philosophers of science have taken up these questions thus far. -
Observable Algebra
Observable Algebra Merab Gogberashvili Andronikashvili Institute of Physics 6 Tamarashvili Str.,Tbilisi 380077, Georgia E-mail: [email protected] (October 24, 2018) A physical applicability of normed split-algebras, such as hyperbolic numbers, split-quaternions and split-octonions is considered. We argue that the observable geometry can be described by the algebra of split-octonions. In such a picture physical phenomena are described by the ordinary elements of chosen algebra, while zero divisors (the elements of split-algebras corresponding to zero norms) give raise the coordinatization of space-time. It turns to be possible that two fundamental constants (velocity of light and Planck constant) and uncertainty principle have geometrical meaning and appears from the condition of positive definiteness of norms. The property of non-associativity of octonions could correspond to the appearance of fundamental probabilities in four dimensions. Grassmann elements and a non-commutativity of space coordinates, which are widely used in various physical theories, appear naturally in our approach. PACS numbers: 04.50.+h; 11.25.Hf; 01.55.+b I. INTRODUCTION nals), one must be able to introduce a distance between two objects. Introduction of a distance always means Real physical phenomena always expose themselves ex- some comparison of two objects using one of them as an perimentally as a set of measured numbers. In a general etalon. Thus we need an algebra with a unit element. way one can say that the measurement process (even In the algebraic language, these requirements mean simple counting) consists of matching the physical phe- that to describe the geometry of the real world we need a nomenon to be measured with some familiar set of ob- normed composition algebra with the unit element over jects, or the number words. -
Lecture Notes on Supersymmetry
Lecture Notes on Supersymmetry Kevin Zhou [email protected] These notes cover supersymmetry, closely following the Part III and MMathPhys Supersymmetry courses as lectured in 2017/2018 and 2018/2019, respectively. The primary sources were: • Fernando Quevedo's Supersymmetry lecture notes. A short, clear introduction to supersym- metry covering the topics required to formulate the MSSM. Also see Ben Allanach's revised version, which places slightly more emphasis on MSSM phenomenology. • Cyril Closset's Supersymmetry lecture notes. A comprehensive set of supersymmetry lecture notes with more emphasis on theoretical applications. Contains coverage of higher SUSY, and spinors in various dimensions, the dynamics of 4D N = 1 gauge theories, and even a brief overview of supergravity. • Aitchison, Supersymmetry in Particle Physics. A friendly introductory book that covers the basics with a minimum of formalism; for instance, the Wess{Zumino model is introduced without using superfields. Also gives an extensive treatment of subtleties in two-component spinor notation. The last half covers the phenomenology of the MSSM. • Wess and Bagger, Supersymmetry and Supergravity. An incredibly terse book that serves as a useful reference. Most modern sources follow the conventions set here. Many pages consist entirely of equations, with no words. We will use the conventions of Quevedo's lecture notes. As such, the metric is mostly negative, and a few other signs are flipped with respect to Wess and Bagger's conventions. The most recent version is here; please report any errors found to [email protected]. 2 Contents Contents 1 Introduction 3 1.1 Motivation.........................................3 1.2 The Poincare Group....................................6 1.3 Spinors in Four Dimensions................................9 1.4 Supersymmetric Quantum Mechanics.......................... -
Chapter 2: Linear Algebra User's Manual
Preprint typeset in JHEP style - HYPER VERSION Chapter 2: Linear Algebra User's Manual Gregory W. Moore Abstract: An overview of some of the finer points of linear algebra usually omitted in physics courses. May 3, 2021 -TOC- Contents 1. Introduction 5 2. Basic Definitions Of Algebraic Structures: Rings, Fields, Modules, Vec- tor Spaces, And Algebras 6 2.1 Rings 6 2.2 Fields 7 2.2.1 Finite Fields 8 2.3 Modules 8 2.4 Vector Spaces 9 2.5 Algebras 10 3. Linear Transformations 14 4. Basis And Dimension 16 4.1 Linear Independence 16 4.2 Free Modules 16 4.3 Vector Spaces 17 4.4 Linear Operators And Matrices 20 4.5 Determinant And Trace 23 5. New Vector Spaces from Old Ones 24 5.1 Direct sum 24 5.2 Quotient Space 28 5.3 Tensor Product 30 5.4 Dual Space 34 6. Tensor spaces 38 6.1 Totally Symmetric And Antisymmetric Tensors 39 6.2 Algebraic structures associated with tensors 44 6.2.1 An Approach To Noncommutative Geometry 47 7. Kernel, Image, and Cokernel 47 7.1 The index of a linear operator 50 8. A Taste of Homological Algebra 51 8.1 The Euler-Poincar´eprinciple 54 8.2 Chain maps and chain homotopies 55 8.3 Exact sequences of complexes 56 8.4 Left- and right-exactness 56 { 1 { 9. Relations Between Real, Complex, And Quaternionic Vector Spaces 59 9.1 Complex structure on a real vector space 59 9.2 Real Structure On A Complex Vector Space 64 9.2.1 Complex Conjugate Of A Complex Vector Space 66 9.2.2 Complexification 67 9.3 The Quaternions 69 9.4 Quaternionic Structure On A Real Vector Space 79 9.5 Quaternionic Structure On Complex Vector Space 79 9.5.1 Complex Structure On Quaternionic Vector Space 81 9.5.2 Summary 81 9.6 Spaces Of Real, Complex, Quaternionic Structures 81 10.