Supersymmetric Quantum Mechanics and Path Integrals
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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. -
Supergravity and Its Legacy Prelude and the Play
Supergravity and its Legacy Prelude and the Play Sergio FERRARA (CERN – LNF INFN) Celebrating Supegravity at 40 CERN, June 24 2016 S. Ferrara - CERN, 2016 1 Supergravity as carved on the Iconic Wall at the «Simons Center for Geometry and Physics», Stony Brook S. Ferrara - CERN, 2016 2 Prelude S. Ferrara - CERN, 2016 3 In the early 1970s I was a staff member at the Frascati National Laboratories of CNEN (then the National Nuclear Energy Agency), and with my colleagues Aurelio Grillo and Giorgio Parisi we were investigating, under the leadership of Raoul Gatto (later Professor at the University of Geneva) the consequences of the application of “Conformal Invariance” to Quantum Field Theory (QFT), stimulated by the ongoing Experiments at SLAC where an unexpected Bjorken Scaling was observed in inclusive electron- proton Cross sections, which was suggesting a larger space-time symmetry in processes dominated by short distance physics. In parallel with Alexander Polyakov, at the time in the Soviet Union, we formulated in those days Conformal invariant Operator Product Expansions (OPE) and proposed the “Conformal Bootstrap” as a non-perturbative approach to QFT. S. Ferrara - CERN, 2016 4 Conformal Invariance, OPEs and Conformal Bootstrap has become again a fashionable subject in recent times, because of the introduction of efficient new methods to solve the “Bootstrap Equations” (Riccardo Rattazzi, Slava Rychkov, Erik Tonni, Alessandro Vichi), and mostly because of their role in the AdS/CFT correspondence. The latter, pioneered by Juan Maldacena, Edward Witten, Steve Gubser, Igor Klebanov and Polyakov, can be regarded, to some extent, as one of the great legacies of higher dimensional Supergravity. -
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. -
Hep-Ph/9811291
CERN-TH/98-354 hep-ph/9811291 Quantum Gravity and Extra Dimensions at High-Energy Colliders Gian F. Giudice, Riccardo Rattazzi, and James D. Wells Theory Division, CERN CH-1211 Geneva 23, Switzerland Abstract Recently it has been pointed out that the characteristic quantum-gravity scale could be as low as the weak scale in theories with gravity propagating in higher dimensions. The observed smallness of Newton’s constant is a consequence of the large compactified volume of the extra dimensions. We investigate the consequences of this supposition for high-energy collider experiments. We do this by first compactifying the higher dimen- sional theory and constructing a 3 + 1-dimensional low-energy effective field theory of the graviton Kaluza-Klein excitations and their interactions with ordinary matter. We then consider graviton production processes, and select γ+ E and jet+ E signatures 6 6 for careful study. We find that both a 1 TeV e+e− collider and the CERN LHC will be able to reliably and perturbatively probe the fundamental gravity scale up to several arXiv:hep-ph/9811291v2 13 Mar 2000 TeV, with the precise value depending on the number of extra dimensions. Similarly, searches at LEP2 and the Tevatron are able to probe this scale up to approximately 1 TeV. We also discuss virtual graviton exchange, which induces local dimension-eight operators associated with the square of the energy-momentum tensor. We estimate the size of such operators and study their effects on ff¯ γγ observables. → CERN-TH/98-354 November 1998 Contents 1 Introduction 1 2 The Kaluza-Klein Excitations of the Graviton 7 3 Feynman Rules 14 4 Graviton Production Processes 18 5 Virtual Graviton Exchange 21 6 Graviton Production and Collider Experiments 24 6.1 e+e− andMuonColliders............................ -
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 -
Jhep05(1999)013
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server Received: March 30, 1999, Accepted: May 11, 1999 HYPER VERSION Sparticle masses from the superconformal anomaly Alex Pomarol∗ Theory Division, CERN CH-1211 Geneva 23, Switzerland JHEP05(1999)013 E-mail: [email protected] Riccardo Rattazzi INFN and Scuola Normale Superiore I-56100 Pisa, Italy E-mail: [email protected] Abstract: We discuss a recently proposed scenario where the sparticle masses are purely mediated by gravity through the superconformal anomaly. This scenario ele- gantly evades the supersymmetric flavor problem since soft masses, like the anomaly, are not directly sensitive to ultraviolet physics. However, its minimal incarnation fails by predicting tachyonic sleptons. We study the conditions for decoupling of heavy threshold effects and how these conditions are evaded. We use these results to build a realistic class of models where the non-decoupling effects of ultra-heavy vectorlike matter fields eliminate the tachyons. These models have a flavor invariant superspectrum similar to that of gauge mediated models. They, however, differ in several aspects: the gaugino masses are not unified, the colored sparticles are not much heavier than the others, the µ problem is less severe and the gravitino mass is well above the weak scale, m3=2 & 10 TeV. We also show that in models where an R-symmetry can be gauged, the associated D-term gives rise to soft terms that are similarly insensitive to the ultraviolet. Keywords: Supersymmetry Breaking, Supergravity Models, Supersymmetric Standard Model. ∗On leave of absence from IFAE, Universitat Aut`onoma de Barcelona, E-08193 Bellaterra, Barcelona. -
Dark Matter and Collider Phenomenology of Non-Universal Gaugino Masses
Dark Matter and Collider Phenomenology of Non-Universal Gaugino Masses A dissertation presented by Michael Holmes to The Department of Physics In partial fulfillment of the requirements for the degree of Doctor of Philosophy in the field of Physics Northeastern University Boston, Massachusetts April, 2010 1 c Michael Holmes, 2010 ALL RIGHTS RESERVED 2 Dark Matter and Collider Phenomenology of Non-Universal Gaugino Masses by Michael Holmes ABSTRACT OF DISSERTATION Submitted in partial fulfillment of the requirement for the degree of Doctor of Philosophy in Physics in the Graduate School of Arts and Sciences of Northeastern University, April, 2010 3 Abstract Signals of minimal supersymmetric models with non-universalities in the gaugino sector of the theory are analyzed at the CERN Large Hadron Collider (LHC) and in experiments searching for dark matter. Signals of dark matter including direct and indirect detection are investigated at depth in various supersymmetric frameworks. The parameter space of deflected mirage mediation, in which the soft terms receive contributions from the three main supersymmetry breaking mediation mechanisms, is investigated with emphasis on the neutralino sector and dark matter signals. The potential for non-universal gaugino masses to explain the recent CDMS II data is studied and possible implications for indirect dark matter detection experiments and LHC signatures are considered. Collider implications of non- universalities in the gaugino sector are examined with attention paid to specific signatures which are targeted to track the non-universalities. Further, the complementarity of dark matter and collider measurements is discussed with emphasis on breaking model degeneracies which may arise in LHC data. -
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 . -
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. -
Arxiv:1808.00010V3 [Hep-Ph] 20 Dec 2019
USTC-ICTS-18-13 Positivity bounds on vector boson scattering at the LHC Cen Zhang Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, China Shuang-Yong Zhou Interdisciplinary Center for Theoretical Study, University of Science and Technology of China, Hefei, Anhui 230026, China Weak vector boson scattering (VBS) is a sensitive probe of new physics effects in the electroweak symmetry breaking. Currently, experimental results at the LHC are interpreted in the effective field theory approach, where possible deviations from the Standard Model in the quartic-gauge-boson couplings are often described by 18 dimension-8 operators. By assuming that a UV completion exists, we derive a new set of theoretical constraints on the coefficients of these operators, i.e. certain combinations of coefficients must be positive. These constraints imply that the current effective approach to VBS has a large redundancy: only about 2% of the full parameter space leads to a UV completion. By excluding the remaining unphysical region of the parameter space, these constraints provide guidance for future VBS studies and measurements. Introduction.| After the discovery of the Higgs bo- values. Recently, a novel approach has been developed son [1, 2], the focus of particle physics has turned to the to set theoretical bounds on the Wilson coefficients of mechanism of electroweak symmetry breaking and be- a generic EFT that can be UV completed. Going un- yond. At the Large Hadron Collider (LHC), vector bo- der the name of positivity bounds, this approach only son scattering (VBS) is among the processes most sen- requires a minimum set of assumptions, which are noth- sitive to the electroweak and the Higgs sectors. -
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.