C. PROPOSAL DESCRIPTION Integrable Models and Applications
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Spring 2011 Prizes and Awards
Spring 2011 Prizes and Awards APS Announces Spring 2011 Prize and Award Recipients Forty-three prizes and awards will be presented during special sessions at three spring meetings of the Society: the 2011 March Meeting, March 21-25, in Dallas, TX, the 2011 April Meeting, April 30-May 3, in Anaheim, CA, and the 2011 Atomic, Molecular and Optical Physics Meeting, June 13-14, in Atlanta, GA. Citations and biographical information for each recipient follow. The Apker Award recipients appeared in the December 2010 issue of APS News (http://www.aps.org/programs/honors/ awards/apker.cfm). Additional biographical information and appropriate web links can be found at the APS website (http://www.aps.org/programs/honors/index.cfm). Nominations for most of next year’s prizes and awards are now being accepted. For details, see page 8 of this insert. Will Allis Prize for the joined the University of Illinois at Hughes Medical Institute. Her Physik Department of the Technical University at Study of Ionized Gases Chicago, and Argonne National lab develops advanced optical Munchen. Herbert Spohn is most widely known Laboratory in 1987. Research imaging techniques, in particular through his work on interacting stochastic particle Frank Isakson Prize for contributions include the observa- single-molecule and super-reso- systems. He strived for a deeper understanding of Optical Effects in Solids tion of conformal invariance at the lution imaging methods, to study how macroscopic laws emerge from the underly- Ising critical point, the Luttinger problems of biomedical interest. ing motion of atoms. Andrei Sakharov Prize scaling of the Fermi volume in Zhuang received her B.S. -
Uwaterloo Latex Thesis Template
The Vertex Algebra Vertex by Miroslav Rapˇc´ak A thesis presented to the University of Waterloo in fulfillment of the thesis requirement for the degree of Doctor of Philosophy in Physics Waterloo, Ontario, Canada, 2019 c Miroslav Rapˇc´ak2019 Examining Committee Membership The following served on the Examining Committee for this thesis. The decision of the Examining Committee is by majority vote. Supervisor: Davide Gaiotto Perimeter Institute for Theoretical Physics Co-supervisor: Jaume Gomis Perimeter Institute for Theoretical Physics Committee Member: Niayesh Afshordi University of Waterloo, Department of Physics and Astronomy Committee Member: Kevin Costello Perimeter Institute for Theoretical Physics Internal/External Member: Benoit Charbonneau University of Waterloo, Department of Pure Mathematics External Examiner: Rajesh Gopakumar International Centre for Theoretical Sciences in Bangalore ii Author's Declaration: I hereby declare that I am the sole author of this thesis. This is a true copy of the thesis, including any required final revisions, as accepted by my examiners. I understand that my thesis may be made electronically available to the public. iii Abstract This thesis reviews some aspects of a large class of vertex operator algebras labelled by (p; q) webs colored by non-negative integers associated to faces of the web diagrams [1,2,3,4]. Such vertex operator algebras conjecturally correspond to two mutually dual setups in gauge theory. First, they appear as a subsector of local operators living on two- dimensional junctions of half-BPS interfaces in four-dimensional = 4 super Yang-Mills theory. Secondly, they are AGT dual to = 2 gauge theories supportedN on four-cycles inside toric Calabi-Yau three-folds. -
Conformal and Nearly Conformal Theories at Large N
Conformal and Nearly Conformal Theories at Large N Grigory M. Tarnopolskiy A Dissertation Presented to the Faculty of Princeton University in Candidacy for the Degree of Doctor of Philosophy Recommended for Acceptance by the Department of Physics Advisers: Professors Igor R. Klebanov and Alexander M. Polyakov September 2017 c Copyright by Grigory M. Tarnopolskiy, 2017. All rights reserved. Abstract In this thesis we present new results in conformal and nearly conformal field theories in various dimensions. In chapter two, we study different properties of the conformal Quantum Electrodynamics (QED) in continuous dimension d. At first we study conformal QED using large Nf methods, where Nf is the number of massless fermions. We compute its sphere free energy as a function of d, ignoring the terms of order 1=Nf and higher. For finite Nf we use the expansion. Next we use a large Nf diagrammatic approach to calculate the leading corrections to CT , the coefficient of the two-point function of the stress-energy tensor, and CJ , the coefficient of the two- point function of the global symmetry current. We present explicit formulae as a function of d and check them versus the expectations in 2 and 4 dimensions. − In chapter three, we discuss vacuum stability in 1 + 1 dimensional conformal field theories with external background fields. We show that the vacuum decay rate is given by a non-local two-form. This two-form is a boundary term that must be added to the effective in/out Lagrangian. The two-form is expressed in terms of a Riemann-Hilbert decomposition for background gauge fields, and is given by its novel “functional” version in the gravitational case. -
Spring 1999 Honors and Awards
Honors and Awards Spring 1999 Physicists to Be Honored at APS Centennial Meeting Thirty-one APS prizes and awards keley and faculty senior scientist at the Alexander Zamolodchikov was born on 1999 HERBERT P. BROIDA PRIZE will be presented during a special cer- Lawrence Berkeley National Laboratory. the 18th of September of 1952 in Dubna, He received his Ph.D. degree in physics emonial session at the APS Centennial Terry A. Miller USSR. He received his education from Meeting, to be held later this month in in 1976 from the University of Califor- Moscow Institute of Physics and Tech- The Ohio State University nia at Berkeley. After working at the IBM Atlanta, Georgia. Citations and bio- nology, which he graduated in 1975 as Watson Research Center, the AT&T Bell graphical information for each Nuclear Physics Engineer. In 1978 he re- Citation: “For his far-ranging contributions Laboratories at Murray Hill, and the recipient follow. Additional biographi- to spectroscopy and chemical physics of University of Pennsylvania, he joined ceived PhD in Physics from Institute of cal information and appropriate Web diatomics and radicals, his development the UC Berkeley faculty in 1980. His re- Experimental and Theoretical Physics in links can be found at the APS Web site of methods for plasma diagnostics, and for search interests are on the electronic and Moscow, USSR. From 1978 he is a mem- [http://www.aps.org]. Nominations his stewardship of the Ohio State Spectros- structural properties of solids, surfaces, ber of L.D.Landau Institute in for most of next year’s prizes and copy Conference.” clusters, and nanotubes, and on many- Chernogolovka, and from 1990, a Pro- awards are now being accepted. -
Lectures on Liouville Theory and Matrix Models
Lectures on Liouville Theory and Matrix Models Alexei Zamolodchikov and Alexander Zamolodchikov Lecture1. Introduction 1. The Liouville gravity 1. Theory of gravity. Since Einstein the term gravity means the dynamic theory of the space-time metric structure. This dynamics may be either classical (classical gravity) or quantum, in which case we talk about quantum gravity. The main dynamical variable is the components of the metric tensor gab(x): In general this theory of gravity is very complicated structure, both from mathematical point of view and conceptually. Even in classical gravity the equations of motion imposed on the metric are highly non-linear and lead to soluthions which typically develop singu- larities where the space-time becomes highly curved and the classical Einstein theory itself fails to describe the physics near such singularities. In quantum gravity the situation is much worse, especially from the point of view of interpretations. Having lost the calssical \rigid" space-time frame to settle his experimental equipment, the virtual observer feels himself somewhat \dissolved" and is forced to look for new interpretational possibilities. The simplest (and quite common) solutionis to forget about coordinates and consider only coordinate-independent observables. Such approach, which can be called the topological gravity in some extended sense, is reasonably consistent and su®ers from the only problem: how to make contact with the semiclassical limit, where, as each of us know, the everyday life has apparently nothing to do with the topological gravity. Anyhow, the problem of in- terpretations, the problem of correct choice of observables, is still of primary importance in quantum gravity. -
2017-2018 Perimeter Institute Annual Report English
WE ARE ALL PART OF THE EQUATION 2018 ANNUAL REPORT VISION To create the world's foremost centre for foundational theoretical physics, uniting public and private partners, and the world's best scientific minds, in a shared enterprise to achieve breakthroughs that will transform our future CONTENTS Welcome ............................................ 2 Message from the Board Chair ........................... 4 Message from the Institute Director ....................... 6 Research ............................................ 8 The Powerful Union of AI and Quantum Matter . 10 Advancing Quantum Field Theory ...................... 12 Progress in Quantum Fundamentals .................... 14 From the Dawn of the Universe to the Dawn of Multimessenger Astronomy .............. 16 Honours, Awards, and Major Grants ...................... 18 Recruitment .........................................20 Training the Next Generation ............................ 24 Catalyzing Rapid Progress ............................. 26 A Global Leader ......................................28 Educational Outreach and Public Engagement ............. 30 Advancing Perimeter’s Mission ......................... 36 Supporting – and Celebrating – Women in Physics . 38 Thanks to Our Supporters .............................. 40 Governance .........................................42 Financials ..........................................46 Looking Ahead: Priorities and Objectives for the Future . 51 Appendices .........................................52 This report covers the activities -
Introductory Lecture Quantum Field Theory (QFT) Was Born As A
22 Introductory Lecture Introductory Lecture Presenting a brief review of the history of the subject. — The modern perspective. Quantum field theory (QFT) was born as a consistent theory for a uni- fied description of physical phenomena in which both, quantum-mechanical aspects and relativistic aspects, are important. In historical reviews it is always difficult to draw a “red line” that would separate “before” and “af- ter.” Nevertheless, in this case it would be fair to say that QFT began † emerging when theorists first posed the question of electromagnetic radi- ation in atoms in the framework of quantum mechanics. The pioneers in this issue were Max Born and Pascual Jordan, in 1925. In 1926, Max Born, Werner Heisenberg and Pascual Jordan formulated the quantum theory of the electromagnetic field neglecting polarization and sources to obtain what today would be called a free field theory. In order to quantize this theory, they used the canonical quantization procedure. In 1927, Paul Dirac pub- lished his fundamental paper “The Quantum Theory of the Emission and Absorption of Radiation.” In this paper (which was communicated to the Proceedings of the Royal Society by Niels Bohr) Dirac gave the first com- plete and consistent treatment of this problem. Thus, quantum field theory emerged, unavoidably, from the quantum treatment of the only known clas- sical field, i.e. electromagnetism. Dirac’s paper in 1927 heralded a revolution in theoretical physics which he himself continued in 1928 extending relativistic theory to electrons. The Dirac equation replaced Schr¨odinger’s equation for cases where electron en- ergies and momenta were too high for a nonrelativistic treatment. -
Superconformal Algebra and Manifolds of G2 Holonomy
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server WIS/06/02–JAN–DPP January 24, 2002 Unitary minimal models of (3=2; 3=2; 2) superconformal algebraSW and manifolds of G2 holonomy Boris Noyvert e-mail: [email protected] Department of Particle Physics, Weizmann Institute of Science, 76100, Rehovot, Israel. Abstract The (3=2; 3=2; 2) superconformal algebra is a algebra with two free parameters.SW It consists of 3 superconformal currentsW of spins 3=2, 3=2 and 2. The algebra is proved to be the symmetry algebra of the coset su(2) su(2) su(2) 1 ⊕su(2)⊕ . At the central charge c =102 the algebra coincides with the superconformal algebra associated to manifolds of G2 holonomy. The unitary minimal models of the (3=2; 3=2; 2) algebra and their fusion SW structure are found. The spectrum of unitary representations of the G2 holonomy algebra is obtained. Contents 1 Introduction 1 2 Structure of the (3=2; 3=2; 2) algebra 3 SW 3 Coset construction 4 3.1Preliminarydiscussion........................... 4 3.2Explicitconstruction............................ 5 4 N =1 superconformal subalgebras 7 5 Highest weight representations 10 5.1NSsector.................................. 11 5.2Ramondsector............................... 12 5.3Firsttwistedsector............................. 13 5.4Secondtwistedsector............................ 14 6 Minimal models 14 6.1Unitaryrepresentations........................... 14 6.2Fusionrules................................. 17 6.3Examples.................................. 19 6.3.1 c =3=2, λ =0model........................ 19 6.3.2 c =9=4, λ =0model........................ 19 7 Spectrum of the G2 conformal algebra 20 8 Summary 23 Appendix 24 A OPEs of the (3=2; 3=2; 2)algebra.................. -
Instantons and Chiral Anomalies in Quantum Field Theory
Instantons and Chiral Anomalies in Quantum Field Theory Viktor G. Matyas June, 2017 The University of Manchester School of Physics and Astronomy Abstract Functional methods are developed in order to study the non-perturbative aspects of Yang-Mills theories. The path integral formulation of quantum mechanics is derived and then used to build a functional formal- ism for quantum field theory. Based on these methods, the BPST instanton solution is derived and used to study the vacuum structure of pure Yang-Mills theories. Then after discussing fermionic functional meth- ods, the anomaly in the axial current of massless quantum electrodynamics is deduced. This derivation requires renormalization, and so a gauge invariant cut-off regulator introduced and used to to eliminate the divergences. 1 Contents 1 Introduction 3 2 The Path Integral Formulation3 2.1 Time Evolution in Quantum Mechanics......................... 3 2.2 Path Integrals in Quantum Mechanics.......................... 4 2.3 Path Integrals in Quantum Field Theory........................ 6 3 Bosonic Quantum Field Theory7 3.1 Free Scalar Fields..................................... 7 4 Fermions and Spinor Fields 10 4.1 The Lorentz Group.................................... 10 4.2 Spinors and Spinor Representations........................... 11 4.3 Dirac and Weyl Spinors ................................. 13 5 Fermionic Quantum Field Theory 14 5.1 Grassman Analysis.................................... 14 5.2 The Fermionic Oscillator................................. 16 5.3 Free Spinor Fields..................................... 17 6 Gauge and Yang-Mills Theories 17 6.1 Basics of Yang-Mills Theories .............................. 17 6.2 Euclidean Formulation of Field Theory......................... 18 7 Instantons and Θ-Vacua in Yang-Mills Theories 19 7.1 Self Duality and The BPST Instanton.......................... 21 7.2 Θ-Vacua and CP Violation............................... -
Front Matter
Cambridge University Press 978-1-108-42991-7 — Topological and Non-Topological Solitons in Scalar Field Theories Yakov M. Shnir Frontmatter More Information TOPOLOGICAL AND NON-TOPOLOGICAL SOLITONS IN SCALAR FIELD THEORIES Solitons emerge in various nonlinear systems – from nonlinear optics and con- densed matter to nuclear physics, cosmology, and supersymmetric theories – as stable, localized configurations behaving in many ways like particles. This book provides an introduction to integrable and non-integrable scalar field models with topological and non-topological soliton solutions. It brings together discussion of solitary waves and construction of soliton solutions in various models and provides a discussion of solitons using simple model examples, including the Kortenweg–de Vries system, the sine-Gordon model, kinks, oscillons, skyrmions, and hopfions. The classical field theory of the scalar field in various spatial dimensions is used throughout to present related concepts, at technical and conceptual levels. Providing a comprehensive introduction to the description and construction of solitons, this book is ideal for researchers and graduate students in mathematics and theoretical physics. Yakov M. Shnir is the leading researcher at the Bogoliubov Laboratory of Theoretical Physics of the Joint Institute for Nuclear Research, in Dubna, Russia, and a part-time professor of theoretical physics at Belarusian State University in Minsk, Belarus. His research focuses on topological and non-topological solitons in classical field theory in flat and curved space-time. He has been involved in many of the recent developments in this area, in particular in investigating chaotic structures in the dynamics of solitons, construction of knotted solutions in the Bose–Einstein condensate, and analysis of thermodynamic properties of hairy black holes. -
New High Energy Theory Center Allen Robbins (1979-1995)
173 Chapter Thirteen New High Energy Theory Center Allen Robbins (1979-1995) Rutgers University In the spring of 1982, President Bloustein appointed a new exec- utive vice-president, T. Alexander Pond. This appointment was destined to have an enormous impact on the University as a whole, and the Physics Department in particular. Because of his background in physics, Pond was given a tenured appointment as Professor of Physics. He received his Ph.D. degree from Princeton in 1953 where he carried out positron exper- iments. Following his degree, Pond served for two years as Instructor at Princeton, and then went to Washington University, St. Louis for nine years. In 1962 he went to SUNY Stony Brook, where he was Chairman of the Department of Physics (1962-68) and played a major role in building the department there. He was then Executive Vice-President at Stony Brook (1968-80). At Rutgers he became Executive Vice President and Chief Academic Officer (1982-91). A major thrust in the development of academic and scientific facil- ities in the State began shortly after the appointment of Alec Pond as Executive Vice-President in 1982. The result would be a significant en- hancement of academic programs at Rutgers, especially in the sciences. In particular there would be a 50% increase in the size of the Physics Depart- ment, and the addition of distinguished faculty members who would dra- matically enhance the reputation of the Department. In 1982, Governor Thomas Kean established a Commission on Science and Technology for the State of New Jersey. President Bloustein was a member of that Commission. -
Introduction
Cambridge University Press 978-0-521-19084-8 - Advanced Topics in Quantum Field Theory: A Lecture Course M. Shifman Excerpt More information Introduction Presenting a brief review of the history of the subject. — The modern perspective. Quantum field theory (QFT) was born as a consistent theory for a unified description of physical phenomena in which both quantum-mechanical aspects and relativistic aspects are important. In historical reviews it is always difficult to draw a line that would separate “before” and “after.”1 Nevertheless, it would be fair to say that QFT began to emerge when theorists first posed the question of how to describe the electromagnetic radiation in atoms in the framework of quantum mechanics. The pioneers in this subject were Max Born and Pascual Jordan, in 1925. In 1926 Max Born, Werner Heisenberg, and Pascual Jordan formulated a quantum theory of the electromagnetic field, neglecting polarization and sources to obtain what today would be called a free field theory. In order to quantize this theory they used the canonical quantization procedure. In 1927 Paul Dirac published his fundamentalpaper “The quantum theory ofthe emission and absorption ofradiation.” In this paper (which was communicated to the Proceedings of the Royal Society by Niels Bohr), Dirac gave the first complete and consistent treatment of the problem. Thus quantum field theory emerged inevitably, from the quantum treatment of the only known classical field, i.e. the electromagnetic field. Dirac’s paper in 1927 heralded a revolution in theoretical physics which he himself continued in 1928, extending relativistic theory to electrons. The Dirac equation replaced Schrödinger’s equation for cases where electron energies and momenta were too high for a nonrelativistic treatment.