Managing Editor: Professor NJ
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Non-Thermal Behavior in Conformal Boundary States
Prepared for submission to JHEP Non-Thermal Behavior in Conformal Boundary States Kevin Kuns and Donald Marolf Department of Physics, University of California, Santa Barbara, CA 93106, U.S.A. E-mail: [email protected], [email protected] Abstract: Cardy has recently observed that certain carefully tuned states of 1+1 CFTs on a timelike strip are periodic with period set by the light-crossing time. The states in question are defined by Euclidean time evolution of conformal boundary states associated with the particular boundary conditions imposed on the edges of the strip. We explain this behavior, and the associated lack of thermalization, by showing that such states are Lorentz-signature conformal transformations of the strip ground state. Taking the long- strip limit implies that states used to model thermalization on the Minkowski plane admit non-thermal conformal extensions beyond future infinity of the Minkowski plane, and thus retain some notion of non-thermal behavior at late times. We also comment on the holo- graphic description of these states. arXiv:1406.4926v2 [cond-mat.stat-mech] 6 Oct 2014 Contents 1 Introduction1 2 Periodicity and Tuned Rectangle States2 2.1 Tuned Rectangle States from Conformal Transformations2 2.2 One-Point Functions5 3 Conformal Transformations to the Thermal Minkowski Plane9 4 Discussion 12 A Holographic Description 13 1 Introduction The rapid change in a quantum system from a Hamiltonian H0 to a Hamiltonian H is known as a quantum quench. Quantum quenches are of experimental interest since they can be studied in laboratory systems involving ultracold atoms. They are also of theoretical interest as examples of out of equilibrium quantum systems whose thermalization, or lack thereof, can be used as a first step towards understanding thermalization in more general quantum systems. -
A First Law of Entanglement Rates from Holography
A First Law of Entanglement Rates from Holography Andy O'Bannon,1, ∗ Jonas Probst,2, y Ronnie Rodgers,1, z and Christoph F. Uhlemann3, 4, x 1STAG Research Centre, Physics and Astronomy, University of Southampton, Highfield, Southampton SO17 1BJ, U. K. 2Rudolf Peierls Centre for Theoretical Physics, University of Oxford, 1 Keble Road, Oxford OX1 3NP, U. K. 3Department of Physics, University of Washington, Seattle, WA 98195-1560, USA 4Mani L. Bhaumik Institute for Theoretical Physics, Department of Physics and Astronomy, University of California, Los Angeles, CA 90095, USA For a perturbation of the state of a Conformal Field Theory (CFT), the response of the entanglement entropy is governed by the so-called “first law" of entanglement entropy, in which the change in entanglement entropy is proportional to the change in energy. Whether such a first law holds for other types of perturbations, such as a change to the CFT La- grangian, remains an open question. We use holography to study the evolution in time t of entanglement entropy for a CFT driven by a t-linear source for a conserved U(1) current or marginal scalar operator. We find that although the usual first law of entanglement entropy may be violated, a first law for the rates of change of entanglement entropy and energy still holds. More generally, we prove that this first law for rates holds in holography for any asymptotically (d + 1)-dimensional Anti-de Sitter metric perturbation whose t dependence first appears at order zd in the Fefferman-Graham expansion about the boundary at z = 0. -
Reading in Fall 2003'S Inside Physics
FFromrom thethe ChairChair available in the fall of 2001. Visits elcome to the first edition of our by prospective students nearly newsletter, created to keep us in doubled the number for the newsletter, created to keep us in previous year, and 33 new Wclose touch with our alumni and graduate students appeared in the friends. We’d like to hear your reaction: fall of 2001. We were especially friends. We’d like to hear your reaction: pleased that 30% of the entering what’s satisfying, what’s not, what’s class were women. I hope this is missing. Please let us know. no “fluke” and that we continue missing. Please let us know. to increase the participation of women in physics. The applica- tions for the fall of 2002 number Jim Allen over 500 and we look forward to Department Chair enrolling another strong class. OUR FUTURE Three new faculty joined our als. And Walter himself, the EXCITING TIMES ranks: Crystal Martin, an observa- founding director of the Institute “You can dismiss one Nobel Prize tional astrophysicist from Caltech; for Theoretical Physics, received as a statistical fluke,” Walter Kohn David Stuart, a high energy the 1998 prize in chemistry. remarked, “but a spate of three experimental physicist from Fermi signals something important and Lab; and Dik Bouwmeester from exciting happening at UCSB.” ENDOWED CHAIR Oxford, who works on quantum We are delighted that a chair in The three Nobels reflect UCSB’s optics and experimental quantum experimental physics has been longstanding commitment to information science. We continue endowed by Bruce and Susan excellence in science and engi- to search for new faculty in Worster. -
October 2013
LONDONLONDON MATHEMATICALMATHEMATICAL SOCIETYSOCIETY NEWSLETTER No. 429 October 2013 Society MeetingsSociety 2013 ELECTIONS voting the deadline for receipt of Meetings TO COUNCIL AND votes is 7 November 2013. and Events Members may like to note that and Events NOMINATING the LMS Election blog, moderated 2013 by the Scrutineers, can be found at: COMMITTEE http://discussions.lms.ac.uk/ Thursday 31 October The LMS 2013 elections will open on elections2013/. Good Practice Scheme 10th October 2013. LMS members Workshop, London will be contacted directly by the Future elections page 15 Electoral Reform Society (ERS), who Members are invited to make sug- Friday 15 November will send out the election material. gestions for nominees for future LMS Graduate Student In advance of this an email will be elections to Council. These should Meeting, London sent by the Society to all members be addressed to Dr Penny Davies 1 page 4 who are registered for electronic who is the Chair of the Nominat- communication informing them ing Committee (nominations@lms. Friday 15 November that they can expect to shortly re- ac.uk). Members may also make LMS AGM, London ceive some election correspondence direct nominations: details will be page 5 from the ERS. published in the April 2014 News- Monday 16 December Those not registered to receive letter or are available from Duncan SW & South Wales email correspondence will receive Turton at the LMS (duncan.turton@ Regional Meeting, all communications in paper for- lms.ac.uk). Swansea mat, both from the Society and 18-21 December from the ERS. Members should ANNUAL GENERAL LMS Prospects in check their post/email regularly in MEETING Mathematics, Durham October for communications re- page 11 garding the elections. -
The Chiral De Rham Complex of Tori and Orbifolds
The Chiral de Rham Complex of Tori and Orbifolds Dissertation zur Erlangung des Doktorgrades der Fakult¨atf¨urMathematik und Physik der Albert-Ludwigs-Universit¨at Freiburg im Breisgau vorgelegt von Felix Fritz Grimm Juni 2016 Betreuerin: Prof. Dr. Katrin Wendland ii Dekan: Prof. Dr. Gregor Herten Erstgutachterin: Prof. Dr. Katrin Wendland Zweitgutachter: Prof. Dr. Werner Nahm Datum der mundlichen¨ Prufung¨ : 19. Oktober 2016 Contents Introduction 1 1 Conformal Field Theory 4 1.1 Definition . .4 1.2 Toroidal CFT . .8 1.2.1 The free boson compatified on the circle . .8 1.2.2 Toroidal CFT in arbitrary dimension . 12 1.3 Vertex operator algebra . 13 1.3.1 Complex multiplication . 15 2 Superconformal field theory 17 2.1 Definition . 17 2.2 Ising model . 21 2.3 Dirac fermion and bosonization . 23 2.4 Toroidal SCFT . 25 2.5 Elliptic genus . 26 3 Orbifold construction 29 3.1 CFT orbifold construction . 29 3.1.1 Z2-orbifold of toroidal CFT . 32 3.2 SCFT orbifold . 34 3.2.1 Z2-orbifold of toroidal SCFT . 36 3.3 Intersection point of Z2-orbifold and torus models . 38 3.3.1 c = 1...................................... 38 3.3.2 c = 3...................................... 40 4 Chiral de Rham complex 41 4.1 Local chiral de Rham complex on CD ...................... 41 4.2 Chiral de Rham complex sheaf . 44 4.3 Cechˇ cohomology vertex algebra . 49 4.4 Identification with SCFT . 49 4.5 Toric geometry . 50 5 Chiral de Rham complex of tori and orbifold 53 5.1 Dolbeault type resolution . 53 5.2 Torus . -
Higher AGT Correspondences, W-Algebras, and Higher Quantum
Higher AGT Correspon- dences, W-algebras, and Higher Quantum Geometric Higher AGT Correspondences, W-algebras, Langlands Duality from M-Theory and Higher Quantum Geometric Langlands Meng-Chwan Duality from M-Theory Tan Introduction Review of 4d Meng-Chwan Tan AGT 5d/6d AGT National University of Singapore W-algebras + Higher QGL SUSY gauge August 3, 2016 theory + W-algebras + QGL Higher GL Conclusion Presentation Outline Higher AGT Correspon- dences, Introduction W-algebras, and Higher Quantum Lightning Review: A 4d AGT Correspondence for Compact Geometric Langlands Lie Groups Duality from M-Theory A 5d/6d AGT Correspondence for Compact Lie Groups Meng-Chwan Tan W-algebras and Higher Quantum Geometric Langlands Introduction Duality Review of 4d AGT Supersymmetric Gauge Theory, W-algebras and a 5d/6d AGT Quantum Geometric Langlands Correspondence W-algebras + Higher QGL SUSY gauge Higher Geometric Langlands Correspondences from theory + W-algebras + M-Theory QGL Higher GL Conclusion Conclusion 6d/5d/4d AGT Correspondence in Physics and Mathematics Higher AGT Correspon- Circa 2009, Alday-Gaiotto-Tachikawa [1] | showed that dences, W-algebras, the Nekrasov instanton partition function of a 4d N = 2 and Higher Quantum conformal SU(2) quiver theory is equivalent to a Geometric Langlands conformal block of a 2d CFT with W2-symmetry that is Duality from M-Theory Liouville theory. This was henceforth known as the Meng-Chwan celebrated 4d AGT correspondence. Tan Circa 2009, Wyllard [2] | the 4d AGT correspondence is Introduction Review of 4d proposed and checked (partially) to hold for a 4d N = 2 AGT conformal SU(N) quiver theory whereby the corresponding 5d/6d AGT 2d CFT is an AN−1 conformal Toda field theory which has W-algebras + Higher QGL WN -symmetry. -
Opening Ceremony
Opening ceremony Sir John Ball, President of the International Mathematical Union Your Majesty, Señor Ruiz Gallardón, Señora Cabrera, Señora Aguirre, Professor Manuel de León, Distinguished guests, Ladies and gentlemen, ¡Bienvenidos al ICM dos mil seis! Welcome to ICM 2006, the 25th International Congress of Mathematicians, and the first ICM to be held in Spain. We offer our heartfelt thanks to the Spanish nation, so rich in history and culture, for its invitation to Madrid. We greatly appreciate that His Majesty King Juan Carlos is honouring mathematics by His presence here today. While celebrating this feast of mathematics, with the many talking-points that it will provide, it is worth reflecting on the ways in which our community functions. Mathematics is a profession of high standards and integrity. We freely discuss our work with others without fear of it being stolen, and research is communicated openly prior to formal publication. Editorial procedures are fair and proper, and work gains its reputation through merit and not by how it is promoted. These are the norms operated by the vast majority of mathematicians. The exceptions are rare, and they are noticed. Mathematics has a strong record of service, freely given. We see this in the time and care spent in the refereeing of papers and other forms of peer review. We see it in the running of mathematical societies and journals, in the provision of free mathematical software and teaching resources, and in the various projects world-wide to improve electronic access to the mathematical literature, old and new. We see it in the nurturing of students beyond the call of duty. -
Arxiv:1109.4101V2 [Hep-Th]
Quantum Open-Closed Homotopy Algebra and String Field Theory Korbinian M¨unster∗ Arnold Sommerfeld Center for Theoretical Physics, Theresienstrasse 37, D-80333 Munich, Germany Ivo Sachs† Center for the Fundamental Laws of Nature, Harvard University, Cambridge, MA 02138, USA and Arnold Sommerfeld Center for Theoretical Physics, Theresienstrasse 37, D-80333 Munich, Germany (Dated: September 28, 2018) Abstract We reformulate the algebraic structure of Zwiebach’s quantum open-closed string field theory in terms of homotopy algebras. We call it the quantum open-closed homotopy algebra (QOCHA) which is the generalization of the open-closed homo- topy algebra (OCHA) of Kajiura and Stasheff. The homotopy formulation reveals new insights about deformations of open string field theory by closed string back- grounds. In particular, deformations by Maurer Cartan elements of the quantum closed homotopy algebra define consistent quantum open string field theories. arXiv:1109.4101v2 [hep-th] 19 Oct 2011 ∗Electronic address: [email protected] †Electronic address: [email protected] 2 Contents I. Introduction 3 II. Summary 4 III. A∞- and L∞-algebras 7 A. A∞-algebras 7 B. L∞-algebras 10 IV. Homotopy involutive Lie bialgebras 12 A. Higher order coderivations 12 B. IBL∞-algebra 13 C. IBL∞-morphisms and Maurer Cartan elements 15 V. Quantum open-closed homotopy algebra 15 A. Loop homotopy algebra of closed strings 17 B. IBL structure on cyclic Hochschild complex 18 C. Quantum open-closed homotopy algebra 19 VI. Deformations and the quantum open-closed correspondence 23 A. Quantum open string field theory 23 B. Quantum open-closed correspondence 24 VII. -
Mechanics, Control and Lie Algebroids, Geometry Meeting 2009
Mechanics, Control and Lie algebroids Geometry Meeting 2009 Eduardo Martínez University of Zaragoza [email protected] Escola Universitaria Politécnica, Ferrol, October 29–30, 2009 Abstract The most relevant ideas and results about mechanical systems defined on Lie algebroids are presented. This was a program originally proposed by Alan Weinstein (1996) and developed by many authors. 1 Several reasons for formulating Mechanics on Lie algebroids The inclusive nature of the Lie algebroid framework: under the same formalism one can consider standard mechanical systems, systems on Lie algebras, systems on semidirect products, systems with symme- tries. The reduction of a mechanical system on a Lie algebroid is a mechan- ical system on a Lie algebroid, and this reduction procedure is done via morphisms of Lie algebroids. Well adapted: the geometry of the underlying Lie algebroid deter- mines some dynamical properties as well as the geometric structures associated to it (e.g. Symplectic structure). Provides a natural way to use quasi-velocities in Mechanics. 2 Introduction Lagrangian systems Given a Lagrangian L 2 C1(TQ), the Euler-Lagrange equations define a dynamical system q_i = vi d @L @L = : dt @vi @qi Variational Calculus. Symplectic formalism 4 Geodesics of left invariant metrics For instance, if k is a Riemannian metric on a manifold Q , the Euler- 1 Lagrange equations for L(v) = 2 k(v; v) are the equation for the geodesics rvv = 0 If Q = G is a Lie group and k is left invariant, then L defines a function 1 l on the Lie algebra g, by restriction l(ξ) = 2 k(ξ; ξ). -
William M. Goldman June 24, 2021 CURRICULUM VITÆ
William M. Goldman June 24, 2021 CURRICULUM VITÆ Professional Preparation: Princeton Univ. A. B. 1977 Univ. Cal. Berkeley Ph.D. 1980 Univ. Colorado NSF Postdoc. 1980{1981 M.I.T. C.L.E. Moore Inst. 1981{1983 Appointments: I.C.E.R.M. Member Sep. 2019 M.S.R.I. Member Oct.{Dec. 2019 Brown Univ. Distinguished Visiting Prof. Sep.{Dec. 2017 M.S.R.I. Member Jan.{May 2015 Institute for Advanced Study Member Spring 2008 Princeton University Visitor Spring 2008 M.S.R.I. Member Nov.{Dec. 2007 Univ. Maryland Assoc. Chair for Grad. Studies 1995{1998 Univ. Maryland Professor 1990{present Oxford Univ. Visiting Professor Spring 1989 Univ. Maryland Assoc. Professor 1986{1990 M.I.T. Assoc. Professor 1986 M.S.R.I. Member 1983{1984 Univ. Maryland Visiting Asst. Professor Fall 1983 M.I.T. Asst. Professor 1983 { 1986 1 2 W. GOLDMAN Publications (1) (with D. Fried and M. Hirsch) Affine manifolds and solvable groups, Bull. Amer. Math. Soc. 3 (1980), 1045{1047. (2) (with M. Hirsch) Flat bundles with solvable holonomy, Proc. Amer. Math. Soc. 82 (1981), 491{494. (3) (with M. Hirsch) Flat bundles with solvable holonomy II: Ob- struction theory, Proc. Amer. Math. Soc. 83 (1981), 175{178. (4) Two examples of affine manifolds, Pac. J. Math.94 (1981), 327{ 330. (5) (with M. Hirsch) A generalization of Bieberbach's theorem, Inv. Math. , 65 (1981), 1{11. (6) (with D. Fried and M. Hirsch) Affine manifolds with nilpotent holonomy, Comm. Math. Helv. 56 (1981), 487{523. (7) Characteristic classes and representations of discrete subgroups of Lie groups, Bull. -
Algebraic Topology - Wikipedia, the Free Encyclopedia Page 1 of 5
Algebraic topology - Wikipedia, the free encyclopedia Page 1 of 5 Algebraic topology From Wikipedia, the free encyclopedia Algebraic topology is a branch of mathematics which uses tools from abstract algebra to study topological spaces. The basic goal is to find algebraic invariants that classify topological spaces up to homeomorphism, though usually most classify up to homotopy equivalence. Although algebraic topology primarily uses algebra to study topological problems, using topology to solve algebraic problems is sometimes also possible. Algebraic topology, for example, allows for a convenient proof that any subgroup of a free group is again a free group. Contents 1 The method of algebraic invariants 2 Setting in category theory 3 Results on homology 4 Applications of algebraic topology 5 Notable algebraic topologists 6 Important theorems in algebraic topology 7 See also 8 Notes 9 References 10 Further reading The method of algebraic invariants An older name for the subject was combinatorial topology , implying an emphasis on how a space X was constructed from simpler ones (the modern standard tool for such construction is the CW-complex ). The basic method now applied in algebraic topology is to investigate spaces via algebraic invariants by mapping them, for example, to groups which have a great deal of manageable structure in a way that respects the relation of homeomorphism (or more general homotopy) of spaces. This allows one to recast statements about topological spaces into statements about groups, which are often easier to prove. Two major ways in which this can be done are through fundamental groups, or more generally homotopy theory, and through homology and cohomology groups. -
Iterated Loop Modules and a Filtration for Vertex Representation of Toroidal Lie Algebras
Pacific Journal of Mathematics ITERATED LOOP MODULES AND A FILTRATION FOR VERTEX REPRESENTATION OF TOROIDAL LIE ALGEBRAS S. ESWARA RAO Volume 171 No. 2 December 1995 PACIFIC JOURNAL OF MATHEMATICS Vol. 171, No. 2, 1995 ITERATED LOOP MODULES AND A FILTERATION FOR VERTEX REPRESENTATION OF TOROIDAL LIE ALGEBRAS S. ESWARA RAO The purpose of this paper is two fold. The first one is to construct a continuous new family of irreducible (some of them are unitarizable) modules for Toroidal algebras. The second one is to describe the sub-quotients of the (integrable) modules constructed through the use of Vertex operators. Introduction. Toroidal algebras r[d] are defined for every d > 1 and when d — 1 they are precisely the untwisted affine Lie-algebras. Such an affine algebra Q can be realized as the universal central extension of the loop algebra Q ®C[t, t"1] where Q is simple finite dimensional Lie-algebra over C. It is well known that Q is a one dimensional central extension of Q ®C[ί, ί"1]. The Toroidal algebras ηd] are the universal central extensions of the iterated loop algebra Q ®C[tfλ, tJ1] which, for d > 2, turnout to be infinite central extension. These algebras are interesting because they are related to the Lie-algebra of Map (X, G), the infinite dimensional group of polynomial maps of X to the complex algebraic group G where X is a d-dimensional torus. For additional material on recent developments in the theory of Toroidal algebras one may consult [BC], [FM] and [MS]. In [MEY] and [EM] a countable family of modules (also integrable see [EMY]) are constructed for Toroidal algebras on Fock space through the use of Vertex Operators (Theorem 3.4, [EM]).