Instanton Counting on Compact Manifolds
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1. INTRODUCTION 1.1. Introductory Remarks on Supersymmetry. 1.2
1. INTRODUCTION 1.1. Introductory remarks on supersymmetry. 1.2. Classical mechanics, the electromagnetic, and gravitational fields. 1.3. Principles of quantum mechanics. 1.4. Symmetries and projective unitary representations. 1.5. Poincar´esymmetry and particle classification. 1.6. Vector bundles and wave equations. The Maxwell, Dirac, and Weyl - equations. 1.7. Bosons and fermions. 1.8. Supersymmetry as the symmetry of Z2{graded geometry. 1.1. Introductory remarks on supersymmetry. The subject of supersymme- try (SUSY) is a part of the theory of elementary particles and their interactions and the still unfinished quest of obtaining a unified view of all the elementary forces in a manner compatible with quantum theory and general relativity. Supersymme- try was discovered in the early 1970's, and in the intervening years has become a major component of theoretical physics. Its novel mathematical features have led to a deeper understanding of the geometrical structure of spacetime, a theme to which great thinkers like Riemann, Poincar´e,Einstein, Weyl, and many others have contributed. Symmetry has always played a fundamental role in quantum theory: rotational symmetry in the theory of spin, Poincar´esymmetry in the classification of elemen- tary particles, and permutation symmetry in the treatment of systems of identical particles. Supersymmetry is a new kind of symmetry which was discovered by the physicists in the early 1970's. However, it is different from all other discoveries in physics in the sense that there has been no experimental evidence supporting it so far. Nevertheless an enormous effort has been expended by many physicists in developing it because of its many unique features and also because of its beauty and coherence1. -
Projective Unitary Representations of Infinite Dimensional Lie Groups
Projective unitary representations of infinite dimensional Lie groups Bas Janssens and Karl-Hermann Neeb January 5, 2015 Abstract For an infinite dimensional Lie group G modelled on a locally convex Lie algebra g, we prove that every smooth projective unitary represen- tation of G corresponds to a smooth linear unitary representation of a Lie group extension G] of G. (The main point is the smooth structure on G].) For infinite dimensional Lie groups G which are 1-connected, regular, and modelled on a barrelled Lie algebra g, we characterize the unitary g-representations which integrate to G. Combining these results, we give a precise formulation of the correspondence between smooth pro- jective unitary representations of G, smooth linear unitary representations of G], and the appropriate unitary representations of its Lie algebra g]. Contents 1 Representations of locally convex Lie groups 5 1.1 Smooth functions . 5 1.2 Locally convex Lie groups . 6 2 Projective unitary representations 7 2.1 Unitary representations . 7 2.2 Projective unitary representations . 7 3 Integration of Lie algebra representations 8 3.1 Derived representations . 9 3.2 Globalisation of Lie algebra representations . 10 3.2.1 Weak and strong topology on V . 11 3.2.2 Regular Lie algebra representations . 15 4 Projective unitary representations and central extensions 20 5 Smoothness of projective representations 25 5.1 Smoothness criteria . 25 5.2 Structure of the set of smooth rays . 26 1 6 Lie algebra extensions and cohomology 28 7 The main theorem 31 8 Covariant representations 33 9 Admissible derivations 36 9.1 Admissible derivations . -
Unitary Group - Wikipedia
Unitary group - Wikipedia https://en.wikipedia.org/wiki/Unitary_group Unitary group In mathematics, the unitary group of degree n, denoted U( n), is the group of n × n unitary matrices, with the group operation of matrix multiplication. The unitary group is a subgroup of the general linear group GL( n, C). Hyperorthogonal group is an archaic name for the unitary group, especially over finite fields. For the group of unitary matrices with determinant 1, see Special unitary group. In the simple case n = 1, the group U(1) corresponds to the circle group, consisting of all complex numbers with absolute value 1 under multiplication. All the unitary groups contain copies of this group. The unitary group U( n) is a real Lie group of dimension n2. The Lie algebra of U( n) consists of n × n skew-Hermitian matrices, with the Lie bracket given by the commutator. The general unitary group (also called the group of unitary similitudes ) consists of all matrices A such that A∗A is a nonzero multiple of the identity matrix, and is just the product of the unitary group with the group of all positive multiples of the identity matrix. Contents Properties Topology Related groups 2-out-of-3 property Special unitary and projective unitary groups G-structure: almost Hermitian Generalizations Indefinite forms Finite fields Degree-2 separable algebras Algebraic groups Unitary group of a quadratic module Polynomial invariants Classifying space See also Notes References Properties Since the determinant of a unitary matrix is a complex number with norm 1, the determinant gives a group 1 of 7 2/23/2018, 10:13 AM Unitary group - Wikipedia https://en.wikipedia.org/wiki/Unitary_group homomorphism The kernel of this homomorphism is the set of unitary matrices with determinant 1. -
UC Riverside UC Riverside Previously Published Works
UC Riverside UC Riverside Previously Published Works Title Universal topological quantum computation from a superconductor-abelian quantum hall heterostructure Permalink https://escholarship.org/uc/item/3nm3m6f2 Journal Physical Review X, 4(1) ISSN 2160-3308 Authors Mong, RSK Clarke, DJ Alicea, J et al. Publication Date 2014 DOI 10.1103/PhysRevX.4.011036 Peer reviewed eScholarship.org Powered by the California Digital Library University of California Universal topological quantum computation from a superconductor/Abelian quantum Hall heterostructure Roger S. K. Mong,1 David J. Clarke,1 Jason Alicea,1 Netanel H. Lindner,1 Paul Fendley,2 Chetan Nayak,3, 4 Yuval Oreg,5 Ady Stern,5 Erez Berg,5 Kirill Shtengel,6, 7 and Matthew P. A. Fisher4 1Department of Physics, California Institute of Technology, Pasadena, CA 91125, USA 2Department of Physics, University of Virginia, Charlottesville, VA 22904, USA 3Microsoft Research, Station Q, University of California, Santa Barbara, CA 93106, USA 4Department of Physics, University of California, Santa Barbara, CA 93106, USA 5Department of Condensed Matter Physics, Weizmann Institute of Science, Rehovot, 76100, Israel 6Department of Physics and Astronomy, University of California, Riverside, California 92521, USA 7Institute for Quantum Information, California Institute of Technology, Pasadena, CA 91125, USA Non-Abelian anyons promise to reveal spectacular features of quantum mechanics that could ultimately pro- vide the foundation for a decoherence-free quantum computer. A key breakthrough in the pursuit of these exotic particles originated from Read and Green’s observation that the Moore-Read quantum Hall state and a (relatively simple) two-dimensional p + ip superconductor both support so-called Ising non-Abelian anyons. -
The Unitary Group in Its Strong Topology Martin Schottenloher Mathematisches Institut LMU M¨Unchen Theresienstr
The Unitary Group In Its Strong Topology Martin Schottenloher Mathematisches Institut LMU M¨unchen Theresienstr. 39, 80333 M¨unchen [email protected], +49 89 21804435 Abstract. The unitary group U(H) on an infinite dimensional complex Hilbert space H in its strong topology is a topological group and has some further nice properties, e.g. it is metrizable and contractible if H is separa- ble. As an application Hilbert bundles are classified by homotopy. Keywords: Unitary Operator, Strong Operator Topology, Topological Group, Infinite Dimensional Lie Group, Contractibility, Hilbert bundle, Classifying Space 2000 Mathematics Subject Classification: 51 F 25, 22 A 10, 22 E 65, 55 R 35, 57 T 20 It is easy to show and well-known that the unitary group U(H) – the group of all unitary operators H→Hon a complex Hilbert space H – is a topological group with respect to the norm topology on U(H). However, for many purposes in mathematics the norm topology is too strong. For example, for a compact topological group G with Haar measure μ the left regular representation on H = L2(G, μ) −1 L : G → U(H),g → Lg : H→H,Lgf(x)=f(g x) is continuous for the strong topology on U(H),butL is not continuous when U(H) is equipped with the norm topology, except for finite G. This fact makes the norm topology on U(H) useless in representation theory and its applications as well as in many areas of physics or topology. The continuity property which is mostly used in case of a topological space W and a general Hilbert space H and which seems to be more natural is the continuity of a left action on H Φ:W ×H→H, in particular, in case of a left action of a topological group G on H: Note that the above left regular representation is continuous as a map: L : G ×H→H. -
Arxiv:1305.5974V1 [Math-Ph]
INTRODUCTION TO SPORADIC GROUPS for physicists Luis J. Boya∗ Departamento de F´ısica Te´orica Universidad de Zaragoza E-50009 Zaragoza, SPAIN MSC: 20D08, 20D05, 11F22 PACS numbers: 02.20.a, 02.20.Bb, 11.24.Yb Key words: Finite simple groups, sporadic groups, the Monster group. Juan SANCHO GUIMERA´ In Memoriam Abstract We describe the collection of finite simple groups, with a view on physical applications. We recall first the prime cyclic groups Zp, and the alternating groups Altn>4. After a quick revision of finite fields Fq, q = pf , with p prime, we consider the 16 families of finite simple groups of Lie type. There are also 26 extra “sporadic” groups, which gather in three interconnected “generations” (with 5+7+8 groups) plus the Pariah groups (6). We point out a couple of physical applications, in- cluding constructing the biggest sporadic group, the “Monster” group, with close to 1054 elements from arguments of physics, and also the relation of some Mathieu groups with compactification in string and M-theory. ∗[email protected] arXiv:1305.5974v1 [math-ph] 25 May 2013 1 Contents 1 Introduction 3 1.1 Generaldescriptionofthework . 3 1.2 Initialmathematics............................ 7 2 Generalities about groups 14 2.1 Elementarynotions............................ 14 2.2 Theframeworkorbox .......................... 16 2.3 Subgroups................................. 18 2.4 Morphisms ................................ 22 2.5 Extensions................................. 23 2.6 Familiesoffinitegroups ......................... 24 2.7 Abeliangroups .............................. 27 2.8 Symmetricgroup ............................. 28 3 More advanced group theory 30 3.1 Groupsoperationginspaces. 30 3.2 Representations.............................. 32 3.3 Characters.Fourierseries . 35 3.4 Homological algebra and extension theory . 37 3.5 Groupsuptoorder16.......................... -
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. -
C. PROPOSAL DESCRIPTION Integrable Models and Applications
C. PROPOSAL DESCRIPTION Integrable models and applications: from strings to condensed matter EUCLID | European Collaboration Linking Integrability with other Disciplines Coordinating node Member 1 - U.York - York-Mons [Ed Corrigan ] Bulgaria Member 2 - INRNE.Sofia - Sofia [Ivan Todorov ] France Member 3 - CNRS.Site Alpes - Annecy{Saclay [Paul Sorba ] Member 4 - ENS.Lyon - Lyon{Jussieu [Jean-Michel Maillet ] Member 5 - LPM.Montpellier - Montpellier{Tours [Vladimir Fateev ] Germany Member 6 - FU.Berlin - Berlin [Andreas Fring ] Member 7 - PI.Bonn - Bonn{Hannover [Vladimir Rittenberg ] Hungary Member 8 - ELTE.Budapest - Budapest{Szeged [L´azl´oPalla ] Italy Member 9 - INFN.Bologna - Bologna{Firenze{Torino [Francesco Ravanini ] Member 10 - SISSA.Trieste - Trieste [Giuseppe Mussardo ] Spain Member 11 - U.Santiago - Santiago de Compostela{Madrid{Bilbao [Luis Miramontes ] UK Member 12 - U.Durham - Durham{Heriot-Watt [Patrick Dorey ] Member 13 - KCL.London - KCL{Swansea{Cambridge [G´erard Watts ] EUCLID 2 1a. RESEARCH TOPIC Quantum field theory has grown from its beginnings in the 1940s into one of the most significant areas in modern theoretical physics. In particle physics, it underpins the standard model of the electromagnetic, weak and strong interactions, and is a major ingredient of string theory, currently the most promising candidate for an extension of the standard model to incorporate gravity. In statistical mechanics, the vital r^oleof quantum-field-theoretic techniques has been recognised since the work of Wilson in the late 1960s. The ever-increasing use of the methods of quantum field theory in condensed matter physics demonstrates the growing practical importance of the subject, and at the same time provides a vital source of fresh ideas and inspirations for those working in more abstract directions. -
Universal Topological Quantum Computation from a Superconductor-Abelian Quantum Hall Heterostructure
PHYSICAL REVIEW X 4, 011036 (2014) Universal Topological Quantum Computation from a Superconductor-Abelian Quantum Hall Heterostructure Roger S. K. Mong,1 David J. Clarke,1 Jason Alicea,1 Netanel H. Lindner,1,2 Paul Fendley,3 Chetan Nayak,4,5 Yuval Oreg,6 Ady Stern,6 Erez Berg,6 Kirill Shtengel,7,8 and Matthew P. A. Fisher5 1Department of Physics, California Institute of Technology, Pasadena, California 91125, USA 2Department of Physics, Technion, 32000 Haifa, Israel 3Department of Physics, University of Virginia, Charlottesville, Virginia 22904, USA 4Microsoft Research, Station Q, University of California, Santa Barbara, California 93106, USA 5Department of Physics, University of California, Santa Barbara, California 93106, USA 6Department of Condensed Matter Physics, Weizmann Institute of Science, Rehovot 76100, Israel 7Department of Physics and Astronomy, University of California, Riverside, California 92521, USA 8Institute for Quantum Information, California Institute of Technology, Pasadena, California 91125, USA (Received 2 August 2013; published 12 March 2014) Non-Abelian anyons promise to reveal spectacular features of quantum mechanics that could ultimately provide the foundation for a decoherence-free quantum computer. A key breakthrough in the pursuit of these exotic particles originated from Read and Green’s observation that the Moore-Read quantum Hall state and a (relatively simple) two-dimensional p þ ip superconductor both support so-called Ising non-Abelian anyons. Here, we establish a similar correspondence between the Z3 Read-Rezayi quantum Hall state and a novel two-dimensional superconductor in which charge-2e Cooper pairs are built from fractionalized quasiparticles. In particular, both phases harbor Fibonacci anyons that—unlike Ising anyons—allow for universal topological quantum computation solely through braiding. -
Third Group Cohomology and Gerbes Over Lie Groups
THIRD GROUP COHOMOLOGY AND GERBES OVER LIE GROUPS JOUKO MICKELSSON AND STEFAN WAGNER Abstract The topological classification of gerbes, as principal bundles with the structure group the projective unitary group of a complex Hilbert space, over a topological space H is given 3 by the third cohomology H (H, Z). When H is a topological group the integral cohomology is often related to a locally continuous (or in the case of a Lie group, locally smooth) third group cohomology of H. We shall study in more detail this relation in the case of a group extension 1 N G H 1 when the gerbe is defined by an abelian extension → → → → 1 1 A Nˆ N 1 of N. In particular, when Hs(N, A) vanishes we shall construct a → → → →2 3 N N transgression map Hs(N, A) Hs(H, A ), where A is the subgroup of N-invariants in A and the subscript s denotes→ the locally smooth cohomology. Examples of this relation appear in gauge theory which are discussed in the paper. Keywords: Third group cohomology, gerbe, abelian extension, automorphisms of group extension, crossed module, transgression map, gauge theory. MSC2010: 22E65, 22E67 (primary), 20J06, 57T10 (secondary). 1. Introduction A gerbe over a topological space X is a principal bundle with fiber PU( ), the projective unitary group U( )/S1 of a complex Hilbert space . GerbesH are classified by the integral cohomologyH H3(X, Z). In real life gerbes mostH often come in the following way. We have a vector bundle E over a space Y with model fiber with a free right group action Y N Y with Y/N = X such that the action of NH can be lifted to a projective action× of→N on E. -
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. -
The Unitary Group in Its Strong Topology
Advances in Pure Mathematics, 2018, 8, 508-515 http://www.scirp.org/journal/apm ISSN Online: 2160-0384 ISSN Print: 2160-0368 The Unitary Group in Its Strong Topology Martin Schottenloher Mathematisches Institut, LMU München, Theresienstr 39, München, Germany How to cite this paper: Schottenloher, M. Abstract (2018) The Unitary Group in Its Strong Topology. Advances in Pure Mathematics, The goal of this paper is to confirm that the unitary group U() on an 8, 508-515. infinite dimensional complex Hilbert space is a topological group in its https://doi.org/10.4236/apm.2018.85029 strong topology, and to emphasize the importance of this property for Received: April 4, 2018 applications in topology. In addition, it is shown that U() in its strong Accepted: May 28, 2018 topology is metrizable and contractible if is separable. As an application Published: May 31, 2018 Hilbert bundles are classified by homotopy. Copyright © 2018 by author and Scientific Research Publishing Inc. Keywords This work is licensed under the Creative Unitary Operator, Strong Operator Topology, Topological Group, Infinite Commons Attribution International Dimensional Lie Group, Contractibility, Hilbert Bundle, Classifying Space License (CC BY 4.0). http://creativecommons.org/licenses/by/4.0/ Open Access 1. Introduction The unitary group U() plays an essential role in many areas of mathematics and physics, e.g. in representation theory, number theory, topology and in quantum mechanics. In some of the corresponding research articles complicated proofs and constructions have been introduced in order to circumvent the assumed fact that the unitary group is not a topological group when equipped with the strong topology (see Remark 1 below for details).