Scientific Report for 2011
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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. -
Quantum Quenches: a Probe of Many-Body Quantum Mechanics
Tata Institute of Fundamental Research Hyderabad Colloquium John Cardy University of California, Berkeley Professor John Cardy is well known for his application of quantum field theory and the renormalization group to condensed matter, especially to critical phenomena in both pure and disordered equilibrium and non-equilibrium systems. In the 1980s he helped develop the theory of conformal invariance and its applications to these problems, ideas which also had an impact in string theory and the physics of black holes. In the 1990s he used conformal invariance to derive many exact results in percolation and related probabilistic problems. More recently Professor Cardy has worked on questions of quantum entanglement and non-equilibrium dynamics in many-body systems. He is a Fellow of the Royal Society, a recipient of the 2000 Dirac Medal of the Institute of Physics, of the 2004 Lars Onsager Prize of the American Physical Society, of the 2010 Boltzmann Medal of the International Union of Pure and Applied Physics, and of the 2011 Dirac Medal and Prize of the International Centre for Theoretical Physics. Professor Cardy has a long-standing association with TIFR, and visited our Mumbai campus in 2007-08 as the Homi Bhabha Chair Professor. Quantum Quenches: a probe of many-body quantum mechanics In a quantum quench, a system is prepared in some state (typically the ground state of an initial hamiltonian) and then evolved coherently with a different hamiltonian, e.g. by instantaneously changing a parameter. Such protocols in many-body systems have recently become experimentally achievable with ultracold atoms. I shall discuss some of the theoretical approaches to this problem, and in particular discuss whether, and in what sense, such systems thermalize. -
Scientific Report for 2012
Scientific Report for 2012 Impressum: Eigent¨umer,Verleger, Herausgeber: The Erwin Schr¨odingerInternational Institute for Mathematical Physics - University of Vienna (DVR 0065528), Boltzmanngasse 9, A-1090 Vienna. Redaktion: Joachim Schwermer, Jakob Yngvason. Supported by the Austrian Federal Ministry of Science and Research (BMWF) via the University of Vienna. Contents Preface 3 The Institute and its Mission . 3 Scientific activities in 2012 . 4 The ESI in 2012 . 7 Scientific Reports 9 Main Research Programmes . 9 Automorphic Forms: Arithmetic and Geometry . 9 K-theory and Quantum Fields . 14 The Interaction of Geometry and Representation Theory. Exploring new frontiers. 18 Modern Methods of Time-Frequency Analysis II . 22 Workshops Organized Outside the Main Programmes . 32 Operator Related Function Theory . 32 Higher Spin Gravity . 34 Computational Inverse Problems . 35 Periodic Orbits in Dynamical Systems . 37 EMS-IAMP Summer School on Quantum Chaos . 39 Golod-Shafarevich Groups and Algebras, and the Rank Gradient . 41 Recent Developments in the Mathematical Analysis of Large Systems . 44 9th Vienna Central European Seminar on Particle Physics and Quantum Field Theory: Dark Matter, Dark Energy, Black Holes and Quantum Aspects of the Universe . 46 Dynamics of General Relativity: Black Holes and Asymptotics . 47 Research in Teams . 49 Bruno Nachtergaele et al: Disordered Oscillator Systems . 49 Alexander Fel'shtyn et al: Twisted Conjugacy Classes in Discrete Groups . 50 Erez Lapid et al: Whittaker Periods of Automorphic Forms . 53 Dale Cutkosky et al: Resolution of Surface Singularities in Positive Characteristic . 55 Senior Research Fellows Programme . 57 James Cogdell: L-functions and Functoriality . 57 Detlev Buchholz: Fundamentals and Highlights of Algebraic Quantum Field Theory . -
Generic Transfer from Gsp(4) to GL(4)
Compositio Math. 142 (2006) 541–550 doi:10.1112/S0010437X06001904 Generic transfer from GSp(4) to GL(4) Mahdi Asgari and Freydoon Shahidi Abstract We establish the Langlands functoriality conjecture for the transfer from the generic spec- trum of GSp(4) to GL(4) and give a criterion for the cuspidality of its image. We apply this to prove results toward the generalized Ramanujan conjecture for generic representations of GSp(4). 1. Introduction Let k be a number field and let G denote the group GSp(4, Ak). The (connected component of the) L-group of G is GSp(4, C), which has a natural embedding into GL(4, C). Langlands functoriality predicts that associated to this embedding there should be a transfer of automorphic representations of G to those of GL(4, Ak)(see[Art04]). Langlands’ theory of Eisenstein series reduces the proof of this to unitary cuspidal automorphic representations. We establish functoriality for the generic spectrum of GSp(4, Ak). More precisely (cf. Theorem 2.4), we prove the following. Let π be a unitary cuspidal representation of GSp(4, Ak), which we assume to be globally generic. Then π has a unique transfer to an automorphic representation Π of GL(4, Ak). 2 The transfer is generic (globally and locally) and satisfies ωΠ = ωπ and Π Π⊗ωπ. Here, ωπ and ωΠ denote the central characters of π and Π, respectively. Moreover, we give a cuspidality criterion for Π and prove that, when Π is not cuspidal, it is an isobaric sum of two unitary cuspidal representations of GL(2, Ak)(cf.Proposition2.2). -
Converse Theorem
A strengthening of the GL(2) converse theorem Andrew R. Booker and M. Krishnamurthy dedicated to Ilya Piatetski-Shapiro (1929{2009) Abstract We generalize the method of [Bo03] to prove a version of the converse theorem of Jacquet- Langlands with relaxed conditions on the twists by ramified id`eleclass characters. Contents 1 Introduction 1 1.1 Notation . 3 2 The classical case 5 3 Additive and multiplicative twists 8 3.1 Multiplicative to additive twists . 8 3.2 Additive to multiplicative twists . 9 4 Some generalities of the GL2 theory 12 4.1 New vectors at the finite places . 12 4.2 Archimedean Whittaker functions . 13 4.3 Bounds for the archimedean parameters . 16 4.4 Fourier coefficients and Dirichlet series . 16 5 Proof of Theorem 1.1 19 5.1 Reduction to additively twisted L-functions . 19 5.2 Automorphy relations from unramified twists . 20 5.3 Producing additive twists . 21 5.4 Taylor expansions . 22 5.5 Proof of Lemma 5.2 . 27 Appendix A. Binomial coefficients 38 1. Introduction The \converse theorem" in the theory of automorphic forms has a long history, beginning with the work of Hecke [He36] and a paper of Weil [We67] relating the automorphy relations satisfied by classical holomorphic modular forms f to analytic properties of the twisted L-functions L(s; f × χ) for Dirichlet characters χ. Soon after, the classical theory was recast in the modern setting of automorphic representations by Jacquet and Langlands [JL70], who generalized Weil's result to GL2 representations π over a global field, characterizing them in terms of their twists L(s; π ⊗ !) by id`eleclass characters !. -
Flowing Along in Four Dimensions 15 November 2011, by Tammy Plotner
Flowing along in four dimensions 15 November 2011, by Tammy Plotner His speculation is the a-theorem… a multitude of avenues in which quantum fields can be energetically excited (a) is always greater at high energies than at low energies. If this theory is correct, then it likely will explain physics beyond the current model and shed light on any possible unknown particles yet to be revealed by the Large Hadron Collider (LHC) at CERN, Europe's particle physics lab near Geneva, Switzerland. "I'm pleased if the proof turns out to be correct," says Cardy, a theoretical physicist at the University of Oxford, UK. "I'm quite amazed the conjecture I made in 1988 stood up." According to theorists Zohar Komargodski and Adam Schwimmer of the Weizmann Institute of Science in Rehovot, Israel, the proof of Cardy's theories was presented July 2011, and is slowly gaining notoriety among the scientific community as other theoretical physicists take note of his work. The a-theorem could help to explain the theory that describes quarks, fundamental particles seen here in a "I think it's quite likely to be right," says Nathan three-dimensional computer-generated simulation. Seiberg, a theoretical physicist at the Institute of Credit: PASIEKA/SPL Advanced Study in Princeton, New Jersey. The field of quantum theory always stands on shaky ground… it seems that no one can be In 1988, John Cardy asked if there was a c- 100% accurate on their guesses of how particles theorem in four dimensions. At the time, he should behave. -
Arxiv:1412.3500V2 [Math.NT] 29 Oct 2015 Γ En Smrhc(Hn3) Ti Ojcueo Aqe Hti Sh It That Jacquet of Conjecture a Is It Let ([Hen93])
GAMMA FACTORS OF PAIRS AND A LOCAL CONVERSE THEOREM IN FAMILIES GILBERT MOSS Abstract. We prove a GL(n) × GL(n − 1) local converse theorem for ℓ-adic families of smooth representations of GLn(F ) where F is a finite extension of Qp and ℓ =6 p. Along the way, we extend the theory of Rankin-Selberg integrals, first introduced in [JPSS83], to the setting of families, continuing previous work of the author [Mos]. 1. Introduction Let F be a finite extension of Qp. A local converse theorem is a result along the ′ following lines: given V1 and V2 representations of GLn(F ), if γ(V1 × V ,X,ψ) = ′ ′ γ(V2×V ,X,ψ) for all representations V of GLn−1(F ), then V1 and V2 are the same. There exists such a converse theorem for complex representations: if V1, V2, and ′ V are irreducible admissible generic representations of GLn(F ) over C, “the same” means isomorphic ([Hen93]). It is a conjecture of Jacquet that it should suffice to ′ n let V vary over representations of GL n (F ), or in other words a GL(n)×GL(⌊ ⌋) ⌊ 2 ⌋ 2 converse theorem should hold. In this paper we construct γ(V ×V ′,X,ψ) and prove a GL(n)×GL(n−1) local converse theorem in the setting of ℓ-adic families. We deal with admissible generic families that are not typically irreducible, so “the same” will mean that V1 and V2 have the same supercuspidal support. Over families, there arises a new dimension to the local converse problem: determining the smallest coefficient ring over which the twisting representations V ′ can be taken while still having the theorem hold. -
Functorial Products for GL2× GL3 and the Symmetric Cube For
Annals of Mathematics, 155 (2002), 837–893 Functorial products for GL2× GL3 and the symmetric cube for GL2 By Henry H. Kim and Freydoon Shahidi* Dedicated to Robert P. Langlands Introduction In this paper we prove two new cases of Langlands functoriality. The first is a functorial product for cusp forms on GL GL as automorphic forms 2 × 3 on GL6, from which we obtain our second case, the long awaited functorial symmetric cube map for cusp forms on GL2. We prove these by applying a recent version of converse theorems of Cogdell and Piatetski-Shapiro to analytic properties of certain L-functions obtained from the method of Eisenstein series (Langlands-Shahidi method). As a consequence we prove the bound 5/34 for Hecke eigenvalues of Maass forms over any number field and at every place, finite or infinite, breaking the crucial bound 1/6 (see below and Sections 7 and 8) towards Ramanujan-Petersson and Selberg conjectures for GL2. As noted below, many other applications follow. To be precise, let π1 and π2 be two automorphic cuspidal representations of GL2(AF ) and GL3(AF ), respectively, where AF is the ring of ad`eles of a number field F . Write π1 = ⊗vπ1v and π2 = ⊗vπ2v. For each v, finite or otherwise, let π1v ⊠ π2v be the irreducible admissible representation of GL6(Fv), attached to (π1v,π2v) through the local Langlands correspondence by Harris-Taylor [HT], Henniart [He], and Langlands [La4]. We point out that, if ϕiv, i = 1, 2, are the two- and the three-dimensional representations of Deligne-Weil group, arXiv:math/0409607v1 [math.NT] 30 Sep 2004 parametrizing πiv, respectively, then π1v⊠π2v is attached to the six-dimensional representation ϕ ϕ . -
Automorphic Forms and L-Functions
Program of the Israel Science Foundation Workshop on Automorphic Forms and L-functions May 15-19, 2006, Rehovot and Tel-Aviv MONDAY, May 15 (Weizmann Institute, Schmidt Lecture Hall) 09:00 – 10:00 Registration of participants 10:00 – 12:30 Morning session on the trace formula James Arthur (University of Toronto) 12:30 LUNCH 14:30 – 15:30 Marie-France Vigneras (Institut Mathematiques de Jussieu) Irreducibility and cuspidality of the Steinberg representation modulo p 16:00 – 17:00 Prof. Chaim Leib Pekeris Memorial Lecture by Peter Sarnak (Princeton University) Equidistribution and Primes (Dolfi and Lola Ebner Auditorium) TUESDAY, May 16 (Tel-Aviv University, Melamed Auditorium) 08:30 – 9:30 Bus from San-Martin to Tel-Aviv University 10:00 – 12:30 Morning session on L-functions Daniel Bump (Stanford University) James Cogdell (Ohio State University) 12:30 LUNCH 14:00 – 15:00 Akshay Venkatesh (Courant Institute) A spherical simple trace formula, and Weyl’s law for cusp forms 15:30 – 16:30 Wee Teck Gan (University of California, San Diego) The regularized Siegel-Weil formula for exceptional groups 17:00 – 18:00 Jiu-Kang Yu (Purdue University) Construction of tame types WEDNESDAY, May 17 (Weizmann Institute, Schmidt Lecture Hall) 10:00 – 12:30 Morning session on theta correspondence Roger Howe (Yale University) Stephen Kudla (University of Maryland) 13:00 – 22:00 A tour and dinner in Jerusalem (bus leaves from San-Martin) THURSDAY, May 18 (Weizmann Institute, Schmidt Lecture Hall) 10:00 – 11:00 Birgit Speh (Cornell University) The restriction -
The Michigan Center for Theoretical Physics∗
Michigan Center for Theoretical Physics THE MICHIGAN CENTER FOR THEORETICAL PHYSICS∗ PAST, PRESENT, AND FUTURE Written by: M. Duff, Director Emeritus G. Kane, Interim Director L. Sander, Associate Director for Research J. Liu, Associate Director for Budget/Executive Committee K. Freese, Associate Director for Outreach A. Bloch, Executive Committee G. Evrard, Executive Committee F. Nori, Executive Committee A. Milliken, Research Secretary ∗ http://www.umich.edu/~mctp/ 1 Michigan Center for Theoretical Physics SUMMARY The missions of The Michigan Center for Theoretical Physics (MCTP) are to carry out quality research, to educate, and to perform service. It is meant to focus particularly on promoting interdisciplinary explorations in theoretical physics and related mathematical sciences through a program of individual and collaborative research, seminars, workshops, and conferences. In the time since its inception in 2001 the MCTP has already gained a strong international reputation for its intellectual and organizational activities, and it is now poised to have an even larger impact as the world of theoretical and mathematical sciences increasingly takes advantage of the MCTP infrastructure to focus national and international activities at the MCTP. External fund raising began in fall 2004 and is showing signs of success. This report documents the structure and achievements of MCTP, and its goals for the future. Basically, within certain guidelines, the MCTP functions by responding to proposals from full members (perhaps with internal or external colleagues) for Workshops, Conferences, Visitors, and students support. Typically two postdocs have also been hired, and support provided for graduate and undergraduate students. This report documents the past activities of MCTP, and forms the foundation for urging the Department of Physics, the College of LS&A, and the University of Michigan to renew their support for an extended period in such a way that total resources are at least as large as they have been.