Lattice Gauge Theory for Physics Beyond the Standard Model
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Localization at Large N †
NORDITA-2013-97 UUITP-21/13 Localization at Large N † J.G. Russo1;2 and K. Zarembo3;4;5 1 Instituci´oCatalana de Recerca i Estudis Avan¸cats(ICREA), Pg. Lluis Companys, 23, 08010 Barcelona, Spain 2 Department ECM, Institut de Ci`enciesdel Cosmos, Universitat de Barcelona, Mart´ıFranqu`es,1, 08028 Barcelona, Spain 3Nordita, KTH Royal Institute of Technology and Stockholm University, Roslagstullsbacken 23, SE-106 91 Stockholm, Sweden 4Department of Physics and Astronomy, Uppsala University SE-751 08 Uppsala, Sweden 5Institute of Theoretical and Experimental Physics, B. Cheremushkinskaya 25, 117218 Moscow, Russia [email protected], [email protected] Abstract We review how localization is used to probe holographic duality and, more generally, non-perturbative dynamics of four-dimensional N = 2 supersymmetric gauge theories in the planar large-N limit. 1 Introduction 5 String theory on AdS5 × S gives a holographic description of the superconformal N = 4 Yang- arXiv:1312.1214v1 [hep-th] 4 Dec 2013 Mills (SYM) through the AdS/CFT correspondence [1]. This description is exact, it maps 5 correlation functions in SYM, at any coupling, to string amplitudes in AdS5 × S . Gauge- string duality for less supersymmetric and non-conformal theories is at present less systematic, and is mostly restricted to the classical gravity approximation, which in the dual field theory corresponds to the extreme strong-coupling regime. For this reason, any direct comparison of holography with the underlying field theory requires non-perturbative input on the field-theory side. There are no general methods, of course, but in the basic AdS/CFT context a variety of tools have been devised to gain insight into the strong-coupling behavior of N = 4 SYM, †Talk by K.Z. -
Casimir Effect on the Lattice: U (1) Gauge Theory in Two Spatial Dimensions
Casimir effect on the lattice: U(1) gauge theory in two spatial dimensions M. N. Chernodub,1, 2, 3 V. A. Goy,4, 2 and A. V. Molochkov2 1Laboratoire de Math´ematiques et Physique Th´eoriqueUMR 7350, Universit´ede Tours, 37200 France 2Soft Matter Physics Laboratory, Far Eastern Federal University, Sukhanova 8, Vladivostok, 690950, Russia 3Department of Physics and Astronomy, University of Gent, Krijgslaan 281, S9, B-9000 Gent, Belgium 4School of Natural Sciences, Far Eastern Federal University, Sukhanova 8, Vladivostok, 690950, Russia (Dated: September 8, 2016) We propose a general numerical method to study the Casimir effect in lattice gauge theories. We illustrate the method by calculating the energy density of zero-point fluctuations around two parallel wires of finite static permittivity in Abelian gauge theory in two spatial dimensions. We discuss various subtle issues related to the lattice formulation of the problem and show how they can successfully be resolved. Finally, we calculate the Casimir potential between the wires of a fixed permittivity, extrapolate our results to the limit of ideally conducting wires and demonstrate excellent agreement with a known theoretical result. I. INTRODUCTION lattice discretization) described by spatially-anisotropic and space-dependent static permittivities "(x) and per- meabilities µ(x) at zero and finite temperature in theories The influence of the physical objects on zero-point with various gauge groups. (vacuum) fluctuations is generally known as the Casimir The structure of the paper is as follows. In Sect. II effect [1{3]. The simplest example of the Casimir effect is we review the implementation of the Casimir boundary a modification of the vacuum energy of electromagnetic conditions for ideal conductors and propose its natural field by closely-spaced and perfectly-conducting parallel counterpart in the lattice gauge theory. -
Hamiltonian Dynamics of Yang-Mills Fields on a Lattice
DUKE-TH-92-40 Hamiltonian Dynamics of Yang-Mills Fields on a Lattice T.S. Bir´o Institut f¨ur Theoretische Physik, Justus-Liebig-Universit¨at, D-6300 Giessen, Germany C. Gong and B. M¨uller Department of Physics, Duke University, Durham, NC 27708 A. Trayanov NCSC, Research Triangle Park, NC 27709 (Dated: July 2, 2018) Abstract We review recent results from studies of the dynamics of classical Yang-Mills fields on a lattice. We discuss the numerical techniques employed in solving the classical lattice Yang-Mills equations in real time, and present results exhibiting the universal chaotic behavior of nonabelian gauge theories. The complete spectrum of Lyapunov exponents is determined for the gauge group SU(2). We survey results obtained for the SU(3) gauge theory and other nonlinear field theories. We also discuss the relevance of these results to the problem of thermalization in gauge theories. arXiv:nucl-th/9306002v2 6 Jun 2005 1 I. INTRODUCTION Knowledge of the microscopic mechanisms responsible for the local equilibration of energy and momentum carried by nonabelian gauge fields is important for our understanding of non-equilibrium processes occurring in the very early universe and in relativistic nuclear collisions. Prime examples for such processes are baryogenesis during the electroweak phase transition, the creation of primordial fluctuations in the density of galaxies in cosmology, and the formation of a quark-gluon plasma in heavy-ion collisions. Whereas transport and equilibration processes have been extensively investigated in the framework of perturbative quantum field theory, rigorous non-perturbative studies of non- abelian gauge theories have been limited to systems at thermal equilibrium. -
Two-Dimensional N=(2, 2) Lattice Gauge Theories with Matter in Higher
Preprint typeset in JHEP style - HYPER VERSION DESY-14-030 Two-dimensional N = (2, 2) Lattice Gauge Theories with Matter in Higher Representations Anosh Joseph John von Neumann Institute for Computing NIC, Platanenallee 6, 15738 Zeuthen, GERMANY Deutsches Elektronen-Synchrotron DESY, Platanenallee 6, 15738 Zeuthen, GERMANY E-mail: [email protected] Abstract: We construct two-dimensional N = (2, 2) supersymmetric gauge theories on a Euclidean spacetime lattice with matter in the two-index symmetric and anti-symmetric representations of SU(Nc) color group. These lattice theories preserve a subset of the su- percharges exact at finite lattice spacing. The method of topological twisting is used to construct such theories in the continuum and then the geometric discretization scheme is used to formulate them on the lattice. The lattice theories obtained this way are gauge- invariant, free from fermion doubling problem and exact supersymmetric at finite lattice spacing. We hope that these lattice constructions further motivate the nonperturbative ex- plorations of models inspired by technicolor, orbifolding and orientifolding in string theories and the Corrigan-Ramond limit. arXiv:1403.4390v2 [hep-lat] 18 Jun 2014 Keywords: Field Theories in Lower Dimensions, Lattice Quantum Field Theory, Supersymmetric Gauge Theory, Extended Supersymmetry. Contents 1. Introduction 1 2. N = (2, 2) Theories with Adjoint Matter 3 3. N = (2, 2) Theories with Two-index Matter 4 4. Lattice Theories 6 5. Fine Tuning and Simulation on the Lattice 9 6. Discussion and Comments 11 1. Introduction Supersymmetric Yang-Mills (SYM) theories are interesting classes of theories by them- selves. They also serve as starting points for constructions of many phenomenologically relevant models. -
QUANTUM INFORMATION METHODS for LATTICE GAUGE THEORIES EREZ ZOHAR A
Next Steps in Quantum Science for HEP, Fermilab, September 2018 QUANTUM INFORMATION METHODS FOR LATTICE GAUGE THEORIES EREZ ZOHAR a Theory Group, Max Planck Institute of Quantum Optics (MPQ) Max Planck – Harvard Quantum Optics Research Center (MPHQ) Based on works with (in alphabetical order): Julian Bender (MPQ) Michele Burrello (MPQ Copenhagen) J. Ignacio Cirac (MPQ) Patrick Emonts (MPQ) Alessandro Farace (MPQ) Benni Reznik (TAU) Thorsten Wahl (MPQ Oxford) Gauge Theories are challenging: • Involve non-perturbative physics • Confinement of quarks hadronic spectrum • Exotic phases of QCD (color superconductivity, quark-gluon plasma) Gauge Theories are challenging: • Involve non-perturbative physics • Confinement of quarks hadronic spectrum • Exotic phases of QCD (color superconductivity, quark-gluon plasma) Hard to treat experimentally (strong forces) Gauge Theories are challenging: • Involve non-perturbative physics • Confinement of quarks hadronic spectrum • Exotic phases of QCD (color superconductivity, quark-gluon plasma) Hard to treat experimentally (strong forces) Hard to treat analytically (non perturbative) Gauge Theories are challenging: • Involve non-perturbative physics • Confinement of quarks hadronic spectrum • Exotic phases of QCD (color superconductivity, quark-gluon plasma) Hard to treat experimentally (strong forces) Hard to treat analytically (non perturbative) Lattice Gauge Theory (Wilson, Kogut-Susskind…) Gauge Theories are challenging: • Involve non-perturbative physics • Confinement of quarks hadronic -
The 1/N Expansion for Lattice Gauge Theories
The 1/N expansion for lattice gauge theories Sourav Chatterjee Sourav Chatterjee The 1/N expansion for lattice gauge theories Yang–Mills theories ◮ Maxwell’s equations are a set of four equations that describe the behavior of an electromagnetic field. ◮ Hermann Weyl showed that these four equations are actually the Euler–Lagrange equations for an elegant minimization problem. ◮ In modern parlance, Maxwell’s equations minimize the Yang–Mills functional for the gauge group U(1). ◮ Physicists later realized that two of the other three fundamental forces of nature — the weak force and the strong force — can also be modeled by similar equations: one needs to simply change the group U(1) to some other group (SU(3) for the strong force, SU(2) for the weak force). This led to the formulation of the Standard Model. ◮ Equations obtained by minimizing Yang–Mills functionals over the space of connections of a principal bundle. Sourav Chatterjee The 1/N expansion for lattice gauge theories Connection form ◮ A quantum YM theory starts with a compact Lie group, called the gauge group. ◮ In this talk, the gauge group is SO(N). ◮ Recall that the Lie algebra so(N) of the Lie group SO(N) is the set of all N × N skew-symmetric matrices. ◮ An SO(N) connection form on Rd is a smooth map from Rd into so(N)d . ◮ If A is a SO(N) connection form, its value A(x) at a point x is a d-tuple (A1(x),..., Ad (x)) of skew-symmetric matrices. ◮ d In the language of differential forms, A = j=1 Aj dxj . -
Two Dimensional Supersymmetric Models and Some of Their Thermodynamic Properties from the Context of Sdlcq
TWO DIMENSIONAL SUPERSYMMETRIC MODELS AND SOME OF THEIR THERMODYNAMIC PROPERTIES FROM THE CONTEXT OF SDLCQ DISSERTATION Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy in the Graduate School of The Ohio State University By Yiannis Proestos, B.Sc., M.Sc. ***** The Ohio State University 2007 Dissertation Committee: Approved by Stephen S. Pinsky, Adviser Stanley L. Durkin Adviser Gregory Kilcup Graduate Program in Robert J. Perry Physics © Copyright by Yiannis Proestos 2007 ABSTRACT Supersymmetric Discrete Light Cone Quantization is utilized to derive the full mass spectrum of two dimensional supersymmetric theories. The thermal properties of such models are studied by constructing the density of states. We consider pure super Yang–Mills theory without and with fundamentals in large-Nc approximation. For the latter we include a Chern-Simons term to give mass to the adjoint partons. In both of the theories we find that the density of states grows exponentially and the theories have a Hagedorn temperature TH . For the pure SYM we find that TH at infi- 2 g Nc nite resolution is slightly less than one in units of π . In this temperature range, q we find that the thermodynamics is dominated by the massless states. For the system with fundamental matter we consider the thermal properties of the mesonic part of the spectrum. We find that the meson-like sector dominates the thermodynamics. We show that in this case TH grows with the gauge coupling. The temperature and coupling dependence of the free energy for temperatures below TH are calculated. As expected, the free energy for weak coupling and low temperature grows quadratically with the temperature. -
Les Houches Lectures on Supersymmetric Gauge Theories
Les Houches lectures on supersymmetric gauge theories ∗ D. S. Berman, E. Rabinovici Racah Institute, Hebrew University, Jerusalem, ISRAEL October 22, 2018 Abstract We introduce simple and more advanced concepts that have played a key role in the development of supersymmetric systems. This is done by first describing various supersymmetric quantum mechanics mod- els. Topics covered include the basic construction of supersymmetric field theories, the phase structure of supersymmetric systems with and without gauge particles, superconformal theories and infrared duality in both field theory and string theory. A discussion of the relation of conformal symmetry to a vanishing vacuum energy (cosmological constant) is included. arXiv:hep-th/0210044v2 11 Oct 2002 ∗ These notes are based on lectures delivered by E. Rabinovici at the Les Houches Summer School: Session 76: Euro Summer School on Unity of Fundamental Physics: Gravity, Gauge Theory and Strings, Les Houches, France, 30 Jul - 31 Aug 2001. 1 Contents 1 Introduction 4 2 Supersymmetric Quantum Mechanics 5 2.1 Symmetryandsymmetrybreaking . 13 2.2 A nonrenormalisation theorem . 15 2.3 A two variable realization and flat potentials . 16 2.4 Geometric meaning of the Witten Index . 20 2.5 LandaulevelsandSUSYQM . 21 2.6 Conformal Quantum Mechanics . 23 2.7 Superconformal quantum mechanics . 26 3 Review of Supersymmetric Models 27 3.1 Kinematics ............................ 27 3.2 SuperspaceandChiralfields. 29 3.3 K¨ahler Potentials . 31 3.4 F-terms .............................. 32 3.5 GlobalSymmetries . .. .. .. .. .. .. 32 3.6 The effective potential . 34 3.7 Supersymmetrybreaking. 34 3.8 Supersymmetricgaugetheories . 35 4 Phases of gauge theories 41 5 Supersymmetric gauge theories/ super QCD 43 5.1 Theclassicalmodulispace. -
Pos(LATTICE2018)210
N = 1 Supersymmetric SU(3) Gauge Theory - Towards simulations of Super-QCD PoS(LATTICE2018)210 Björn Wellegehausen∗ Friedrich Schiller University Jena, 07743 Jena, Germany E-mail: [email protected] Andreas Wipf Friedrich Schiller University Jena, 07743 Jena, Germany E-mail: [email protected] N = 1 supersymmetric QCD (SQCD) is a possible building block of theories beyond the standard model. It describes the interaction between gluons and quarks with their superpartners, gluinos and squarks. Since supersymmetry is explicitly broken by the lattice regularization, a careful fine-tuning of operators is necessary to obtain a supersymmetric continuum limit. For the pure gauge sector, N = 1 Supersymmetric Yang-Mills theory, supersymmetry is only broken by a non-vanishing gluino mass. If we add matter fields, this is no longer true and more operators in the scalar squark sector have to be considered for fine-tuning the theory. Guided by a one-loop calculation in lattice perturbation theory, we show that maintaining chiral symmetry in the light sector is nevertheless an important step. Furthermore, we present first preliminary lattice results on the fine-tuning and Ward-identities of SQCD. The 36th Annual International Symposium on Lattice Field Theory - LATTICE2018 22-28 July, 2018 Michigan State University, East Lansing, Michigan, USA. ∗Speaker. c Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 International License (CC BY-NC-ND 4.0). https://pos.sissa.it/ Simulations of Super-QCD Björn Wellegehausen 1. Introduction Supersymmetric gauge theories are an important building block of many models beyond the stan- dard model. -
Lattice Gauge Theories and the Composite Higgs
Lattice gauge theories and the composite Higgs (on behalf of the USQCD BSM group) Snowmass on the Pacific @ KITP Julius Kuti University of California, San Diego Snowmass on the Pacific @ KITP, May 29-31, 2013 1 Large Hadron Collider - CERN primary mission: - Search for Higgs particle - Origin of Electroweak symmetry breaking • A Higgs-like particle is found Is it the Standard Model Higgs? • Or, new strong dynamics? • Composite Goldstone-like Higgs? • SUSY? 2 Large Hadron Collider - CERN primary mission: - Search for Higgs particle - Origin of Electroweak symmetry breaking • A Higgs-like particle is found Is it the Standard Model Higgs? • Or, new strong dynamics? • Composite Goldstone-like Higgs? • SUSY? Primary focus of USQCD BSM effort and this short talk 2 LATTICE GAUGE THEORIES AT THE ENERGY FRONTIER Thomas Appelquist, Richard Brower, Simon Catterall, George Fleming, Joel Giedt, Anna Hasenfratz, Julius Kuti, Ethan Neil, and David Schaich (USQCD Collaboration) (Dated: March 10, 2013) USQCD BSM White Paper - community based effort: 3 1 LATTICE GAUGE THEORIES AT THE ENERGY FRONTIER Thomas Appelquist, Richard Brower, Simon Catterall, George Fleming, Joel Giedt, Anna Hasenfratz, Julius Kuti, Ethan Neil, and David Schaich (USQCD Collaboration) (Dated: March 10, 2013) USQCD BSM White Paper - community based effort: • to identify most significant lattice results of last few years • to identify major research directions for planning • to describe BSM lattice toolset with phenomenological applications • estimate resources needed for the plan New hardware proposal submitted including USQCD BSM plans 3 1 Introducing USQCD BSM groups with highlighted publications: (approximately 1/5 of USQCD community) select publications of Lattice Strong Dynamics (LSD) collaboration: WW Scattering Parameters via Pseudoscalar Phase Shifts Thomas Appelquist (Yale U.), Ron Babich, Richard C. -
Lattice Gauge Theory a Short Primer
CORE Metadata, citation and similar papers at core.ac.uk Provided by CERN Document Server MS-TPI-00-11 hep-lat/0012005 Lattice Gauge Theory A Short Primer Lectures given at the PSI Zuoz Summer School 2000 G. M¨unster ∗,M.Walzl† Institut f¨ur Theoretische Physik Westf¨∗ alische Wilhelms-Universit¨at Wilhelm-Klemm-Str. 9 D-48149 M¨unster Germany Institut f¨ur Kernphysik (Theorie) † Forschungszentrum J¨ulich D-52425 J¨ulich Germany Abstract In this contribution we give an introduction to the foundations and methods of lattice gauge theory. Starting with a brief dis- cussion of the quantum mechanical path integral, we develop the main ingredients of lattice field theory: functional integrals, Eu- clidean field theory and the space-time discretization of scalar, fermion and gauge fields. Some of the methods used in calcula- tions are reviewed and illustrated by a collection of typical results. ∗Electronic mail address: [email protected] yElectronic mail address: [email protected] 1 Introduction 1.1 Why this Article? These lectures given at the PSI summer school 2000 in Zuoz give an overview of the basic ideas and results of lattice gauge theory for non-experts, with a stress on lattice quantum chromodynamics. This is neither a review of the status nor a survey of recent results in lattice gauge theory. Some typical results are presented for illustrative purposes only. For reviews on recent developments see [1] or the proceedings of the annual LATTICE conferences. To those who ask for a more detailed and in some places more rigorous look at this subject we recommend the literature in [2]. -
Arxiv:1909.07641V1 [Cond-Mat.Quant-Gas] 17 Sep 2019
Realizing a scalable building block of a U(1) gauge theory with cold atomic mixtures Alexander Mil,1 Torsten V. Zache,2 Apoorva Hegde,1 Andy Xia,1 Rohit P. Bhatt,1 Markus K. Oberthaler,1 Philipp Hauke,1, 2 J¨urgenBerges,2 and Fred Jendrzejewski1 1Universit¨atHeidelberg, Kirchhoff-Institut f¨urPhysik, Im Neuenheimer Feld 227, 69120 Heidelberg, Germany 2Universit¨atHeidelberg, Institut f¨urTheoretische Physik, Philosophenweg 16, 69120 Heidelberg, Germany (Dated: September 18, 2019) In the fundamental laws of physics, gauge fields mediate the interaction between charged particles. An example is quantum electrodynamics|the theory of electrons interacting with the electromagnetic field—based on U(1) gauge symmetry. Solving such gauge theories is in general a hard problem for classical computational techniques. While quantum computers suggest a way forward, it is difficult to build large-scale digital quantum devices required for complex simulations. Here, we propose a fully scalable analog quantum simulator of a U(1) gauge theory in one spatial dimension. To engineer the local gauge symmetry, we employ inter-species spin-changing collisions in an atomic mixture. We demonstrate the experimental realization of the elementary building block as a key step towards a platform for large-scale quantum simulations of continuous gauge theories. Continuous gauge symmetries are a cornerstone of our A gauge field matter field fundamental description of quantum physics as encoded in ... ... the Standard Model of Particle Physics. The presence of n-1 n n+1 n+2 a gauge symmetry implies a concerted dynamics of matter building block and gauge fields that is subject to local symmetry con- B bˆ straints at each point in space and time [1].