Ashoke Sen and S-Duality Winner of Fundamental Physics Prize
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3-Fermion Topological Quantum Computation [1]
3-Fermion topological quantum computation [1] Sam Roberts1 and Dominic J. Williamson2 1Centre for Engineered Quantum Systems, School of Physics, The University of Sydney, Sydney, NSW 2006, Australia 2Stanford Institute for Theoretical Physics, Stanford University, Stanford, CA 94305, USA I. INTRODUCTION Topological quantum computation (TQC) is currently the most promising approach to scalable, fault-tolerant quantum computation. In recent years, the focus has been on TQC with Kitaev's toric code [2], due to it's high threshold to noise [3, 4], and amenability to planar architectures with nearest neighbour interactions. To encode and manipulate quantum information in the toric code, a variety of techniques drawn from condensed matter contexts have been utilised. In particular, some of the efficient approaches for TQC with the toric code rely on creating and manipulating gapped-boundaries, symmetry defects and anyons of the underlying topological phase of matter [5{ 10]. Despite great advances, the overheads for universal fault-tolerant quantum computation remain a formidable challenge. It is therefore important to analyse the potential of TQC in a broad range of topological phases of matter, and attempt to find new computational substrates that require fewer quantum resources to execute fault-tolerant quantum computation. In this work we present an approach to TQC for more general anyon theories based on the Walker{Wang mod- els [11]. This provides a rich class of spin-lattice models in three-dimensions whose boundaries can naturally be used to topologically encode quantum information. The two-dimensional boundary phases of Walker{Wang models accommodate a richer set of possibilities than stand-alone two-dimensional topological phases realized by commuting projector codes [12, 13]. -
Arxiv:1705.01740V1 [Cond-Mat.Str-El] 4 May 2017 2
Physics of the Kitaev model: fractionalization, dynamical correlations, and material connections M. Hermanns1, I. Kimchi2, J. Knolle3 1Institute for Theoretical Physics, University of Cologne, 50937 Cologne, Germany 2Department of Physics, Massachusetts Institute of Technology, Cambridge, MA, 02139, USA and 3T.C.M. group, Cavendish Laboratory, J. J. Thomson Avenue, Cambridge, CB3 0HE, United Kingdom Quantum spin liquids have fascinated condensed matter physicists for decades because of their unusual properties such as spin fractionalization and long-range entanglement. Unlike conventional symmetry breaking the topological order underlying quantum spin liquids is hard to detect exper- imentally. Even theoretical models are scarce for which the ground state is established to be a quantum spin liquid. The Kitaev honeycomb model and its generalizations to other tri-coordinated lattices are chief counterexamples | they are exactly solvable, harbor a variety of quantum spin liquid phases, and are also relevant for certain transition metal compounds including the polymorphs of (Na,Li)2IrO3 Iridates and RuCl3. In this review, we give an overview of the rich physics of the Kitaev model, including 2D and 3D fractionalization as well as dynamical correlations and behavior at finite temperatures. We discuss the different materials, and argue how the Kitaev model physics can be relevant even though most materials show magnetic ordering at low temperatures. arXiv:1705.01740v1 [cond-mat.str-el] 4 May 2017 2 CONTENTS I. Introduction 2 II. Kitaev quantum spin liquids 3 A. The Kitaev model 3 B. Classifying Kitaev quantum spin liquids by projective symmetries 4 C. Confinement and finite temperature 5 III. Symmetry and chemistry of the Kitaev exchange 6 IV. -
Inflation, Large Branes, and the Shape of Space
Inflation, Large Branes, and the Shape of Space Brett McInnes National University of Singapore email: [email protected] ABSTRACT Linde has recently argued that compact flat or negatively curved spatial sections should, in many circumstances, be considered typical in Inflationary cosmologies. We suggest that the “large brane instability” of Seiberg and Witten eliminates the negative candidates in the context of string theory. That leaves the flat, compact, three-dimensional manifolds — Conway’s platycosms. We show that deep theorems of Schoen, Yau, Gromov and Lawson imply that, even in this case, Seiberg-Witten instability can be avoided only with difficulty. Using a specific cosmological model of the Maldacena-Maoz type, we explain how to do this, and we also show how the list of platycosmic candidates can be reduced to three. This leads to an extension of the basic idea: the conformal compactification of the entire Euclidean spacetime also has the topology of a flat, compact, four-dimensional space. arXiv:hep-th/0410115v2 19 Oct 2004 1. Nearly Flat or Really Flat? Linde has recently argued [1] that, at least in some circumstances, we should regard cosmological models with flat or negatively curved compact spatial sections as the norm from an Inflationary point of view. Here we wish to argue that cosmic holography, in the novel form proposed by Maldacena and Maoz [2], gives a deep new interpretation of this idea, and also sharpens it very considerably to exclude the negative case. This focuses our attention on cosmological models with flat, compact spatial sections. Current observations [3] show that the spatial sections of our Universe [as defined by observers for whom local isotropy obtains] are fairly close to being flat: the total density parameter Ω satisfies Ω = 1.02 0.02 at 95% confidence level, if we allow the imposition ± of a reasonable prior [4] on the Hubble parameter. -
Anomalies, Dualities, and Topology of D = 6 N = 1 Superstring Vacua
RU-96-16 NSF-ITP-96-21 CALT-68-2057 IASSNS-HEP-96/53 hep-th/9605184 Anomalies, Dualities, and Topology of D =6 N =1 Superstring Vacua Micha Berkooz,1 Robert G. Leigh,1 Joseph Polchinski,2 John H. Schwarz,3 Nathan Seiberg,1 and Edward Witten4 1Department of Physics, Rutgers University, Piscataway, NJ 08855-0849 2Institute for Theoretical Physics, University of California, Santa Barbara, CA 93106-4030 3California Institute of Technology, Pasadena, CA 91125 4Institute for Advanced Study, Princeton, NJ 08540 Abstract We consider various aspects of compactifications of the Type I/heterotic Spin(32)/Z2 theory on K3. One family of such compactifications in- cludes the standard embedding of the spin connection in the gauge group, and is on the same moduli space as the compactification of arXiv:hep-th/9605184v1 25 May 1996 the heterotic E8 × E8 theory on K3 with instanton numbers (8,16). Another class, which includes an orbifold of the Type I theory re- cently constructed by Gimon and Polchinski and whose field theory limit involves some topological novelties, is on the moduli space of the heterotic E8 × E8 theory on K3 with instanton numbers (12,12). These connections between Spin(32)/Z2 and E8 × E8 models can be demonstrated by T duality, and permit a better understanding of non- perturbative gauge fields in the (12,12) model. In the transformation between Spin(32)/Z2 and E8 × E8 models, the strong/weak coupling duality of the (12,12) E8 × E8 model is mapped to T duality in the Type I theory. The gauge and gravitational anomalies in the Type I theory are canceled by an extension of the Green-Schwarz mechanism. -
Kitaev Materials
Kitaev Materials Simon Trebst Institute for Theoretical Physics University of Cologne, 50937 Cologne, Germany Contents 1 Spin-orbit entangled Mott insulators 2 1.1 Bond-directional interactions . 4 1.2 Kitaev model . 6 2 Honeycomb Kitaev materials 9 2.1 Na2IrO3 ...................................... 9 2.2 ↵-Li2IrO3 ..................................... 10 2.3 ↵-RuCl3 ...................................... 11 3 Triangular Kitaev materials 15 3.1 Ba3IrxTi3 xO9 ................................... 15 − 3.2 Other materials . 17 4 Three-dimensional Kitaev materials 17 4.1 Conceptual overview . 18 4.2 β-Li2IrO3 and γ-Li2IrO3 ............................. 22 4.3 Other materials . 23 5 Outlook 24 arXiv:1701.07056v1 [cond-mat.str-el] 24 Jan 2017 Lecture Notes of the 48th IFF Spring School “Topological Matter – Topological Insulators, Skyrmions and Majoranas” (Forschungszentrum Julich,¨ 2017). All rights reserved. 2 Simon Trebst 1 Spin-orbit entangled Mott insulators Transition-metal oxides with partially filled 4d and 5d shells exhibit an intricate interplay of electronic, spin, and orbital degrees of freedom arising from a largely accidental balance of electronic correlations, spin-orbit entanglement, and crystal-field effects [1]. With different ma- terials exhibiting slight tilts towards one of the three effects, a remarkably broad variety of novel forms of quantum matter can be explored. On the theoretical side, topology is found to play a crucial role in these systems – an observation which, in the weakly correlated regime, has lead to the discovery of the topological band insulator [2, 3] and subsequently its metallic cousin, the Weyl semi-metal [4, 5]. Upon increasing electronic correlations, Mott insulators with unusual local moments such as spin-orbit entangled degrees of freedom can form and whose collective behavior gives rise to unconventional types of magnetism including the formation of quadrupo- lar correlations or the emergence of so-called spin liquid states. -
Introduction to Conformal Field Theory and String
SLAC-PUB-5149 December 1989 m INTRODUCTION TO CONFORMAL FIELD THEORY AND STRING THEORY* Lance J. Dixon Stanford Linear Accelerator Center Stanford University Stanford, CA 94309 ABSTRACT I give an elementary introduction to conformal field theory and its applications to string theory. I. INTRODUCTION: These lectures are meant to provide a brief introduction to conformal field -theory (CFT) and string theory for those with no prior exposure to the subjects. There are many excellent reviews already available (or almost available), and most of these go in to much more detail than I will be able to here. Those reviews con- centrating on the CFT side of the subject include refs. 1,2,3,4; those emphasizing string theory include refs. 5,6,7,8,9,10,11,12,13 I will start with a little pre-history of string theory to help motivate the sub- ject. In the 1960’s it was noticed that certain properties of the hadronic spectrum - squared masses for resonances that rose linearly with the angular momentum - resembled the excitations of a massless, relativistic string.14 Such a string is char- *Work supported in by the Department of Energy, contract DE-AC03-76SF00515. Lectures presented at the Theoretical Advanced Study Institute In Elementary Particle Physics, Boulder, Colorado, June 4-30,1989 acterized by just one energy (or length) scale,* namely the square root of the string tension T, which is the energy per unit length of a static, stretched string. For strings to describe the strong interactions fi should be of order 1 GeV. Although strings provided a qualitative understanding of much hadronic physics (and are still useful today for describing hadronic spectra 15 and fragmentation16), some features were hard to reconcile. -
Nominations for Different “Academy Awards/Lectures/ Medals”
The National Academy of Sciences, India (NASI) 5, Lajpatrai Road, Prayagraj – 211002 Prof. Paramjit Khurana Ph.D., FNA, FASc, FNAAS, FTWAS, FNASc Prof. Satya Deo Ph.D. (Arkansas, USA), F.N.A.Sc. General Secretaries June 15, 2021 Subject : Nominations for different “Academy Awards/Lectures/Medals” Dear Fellows, I request you to kindly send nominations for the following “Academy Awards/Lectures/Medals”– 1. Prof. Meghnad Saha Memorial Lecture Award (2021) 2. Prof. N.R. Dhar Memorial Lecture Award (2021) 3. Prof. Archana Sharma Memorial Lecture Award (2021) 4. Prof. M.G.K. Menon Lecture Award (2021) 5. Prof. M.G.K. Menon Memorial Award (2021) 6. Prof. V. P. Sharma Memorial Lecture Award (2021) 7. Prof. A.K. Sharma Memorial Lecture Award (2021) 8. Prof. Prafulla Chandra Ray Memorial Lecture Award (2021) 9. Prof. S.K. Joshi Memorial Lecture Award (2021) 10. Prof. A.C. Banerji Memorial Lecture Award (2021) 11. Dr. B.P. Pal Memorial Lecture Award (2021) 12. Dr. P. Sheel Memorial (Young Women Scientist) Lecture Award (2021) 13. Prof. B.K. Bachhawat Memorial Lecture Award (2021) 14. Prof. U.S. Srivastava Memorial Lecture Award (2021) 15. Lecture Award in the field of Biodiversity (2021) 16. NASI-Buti Foundation Lecture Award (2021) The nomination papers duly completed in all respect should be emailed to NASI on [email protected] latest by July 15, 2021. No hard copy is required for this year; kindly send the nomination on aforesaid email only (not on any other email id of NASI). The copy of Regulations regarding these Academy Awards/Lectures/Medals and the names of past recipients are enclosed. -
Some Comments on Physical Mathematics
Preprint typeset in JHEP style - HYPER VERSION Some Comments on Physical Mathematics Gregory W. Moore Abstract: These are some thoughts that accompany a talk delivered at the APS Savannah meeting, April 5, 2014. I have serious doubts about whether I deserve to be awarded the 2014 Heineman Prize. Nevertheless, I thank the APS and the selection committee for their recognition of the work I have been involved in, as well as the Heineman Foundation for its continued support of Mathematical Physics. Above all, I thank my many excellent collaborators and teachers for making possible my participation in some very rewarding scientific research. 1 I have been asked to give a talk in this prize session, and so I will use the occasion to say a few words about Mathematical Physics, and its relation to the sub-discipline of Physical Mathematics. I will also comment on how some of the work mentioned in the citation illuminates this emergent field. I will begin by framing the remarks in a much broader historical and philosophical context. I hasten to add that I am neither a historian nor a philosopher of science, as will become immediately obvious to any expert, but my impression is that if we look back to the modern era of science then major figures such as Galileo, Kepler, Leibniz, and New- ton were neither physicists nor mathematicans. Rather they were Natural Philosophers. Even around the turn of the 19th century the same could still be said of Bernoulli, Euler, Lagrange, and Hamilton. But a real divide between Mathematics and Physics began to open up in the 19th century. -
2005 March Meeting Gears up for Showtime in the City of Angels
NEWS See Pullout Insert Inside March 2005 Volume 14, No. 3 A Publication of The American Physical Society http://www.aps.org/apsnews 2005 March Meeting Gears Up for Reborn Nicholson Medal Showtime in the City of Angels Stresses Mentorship Established in memory of Dwight The latest research relevance to the design R. Nicholson of the University of results on the spin Hall and creation of next- Iowa, who died tragically in 1991, effect, new chemistry generation nano-electro- and first given in 1994, the APS with superatoms, and mechanical systems Nicholson Medal has been reborn several sessions cel- (NEMS). Moses Chan this year as an award for human ebrating all things (Pennsylvania State Uni- outreach. According to the infor- Einstein are among the versity) will talk about mation contained on the Medal’s expected highlights at evidence of Bose-Einstein web site (http://www.aps.org/praw/ the 2005 APS March condensation in solid he- nicholso/index.cfm), the Nicholson meeting, to be held later lium, while Stanford Medal for Human Outreach shall Photo Credit: Courtesy of the Los Angeles Convention Center this month in Los University’s Zhixun Shen be awarded to a physicist who ei- Angeles, California. The will discuss how photo- ther through teaching, research, or Photo from Iowa University Relations. conference is the largest physics Boltzmann, and Ehrenfest, but also emission spectroscopy has science-related activities, Dwight R. Nicholson. meeting of the year, featuring some Emmy Noether, one of the rare emerged as a leading tool to push -
Quantum Information Science Activities at NSF
Quantum Information Science Activities at NSF Some History, Current Programs, and Future Directions Presentation for HEPAP 11/29/2018 Alex Cronin, Program Director National Science Foundation Physics Division QIS @ NSF goes back a long time Wootters & Zurek (1982) “A single quantum cannot be cloned”. Nature, 299, 802 acknowledged NSF Award 7826592 [PI: John A. Wheeler, UT Austin] C. Caves (1981) “Quantum Mechanical noise in an interferometer” PRD, 23,1693 acknowledged NSF Award 7922012 [PI: Kip Thorne, Caltech] “Information Mechanics (Computer and Information Science)” NSF Award 8618002; PI: Tommaso Toffoli, MIT; Start: 1987 led to one of the “basic building blocks for quantum computation” - Blatt, PRL, 102, 040501 (2009), “Realization of the Quantum Toffoli Gate with Trapped Ions” “Research on Randomized Algorithms, Complexity Theory, and Quantum Computers” NSF Award 9310214; PI: Umesh Vazirani, UC-Berkeley; Start: 1993 led to a quantum Fourier transform algorithm, later used by Shor QIS @ NSF goes back a long time Quantum Statistics of Nonclassical, Pulsed Light Fields Award: 9224779; PI: Michael Raymer, U. Oregon - Eugene; NSF Org:PHY Complexity Studies in Communications and Quantum Computations Award: 9627819; PI: Andrew Yao, Princeton; NSF Org:CCF Quantum Logic, Quantum Information and Quantum Computation Award: 9601997; PI: David MacCallum, Carleton College; NSF Org:SES Physics of Quantum Computing Award: 9802413; PI:Julio Gea-Banacloche, U Arkansas; NSF Org:PHY Quantum Foundations and Information Theory Using Consistent Histories Award: 9900755; PI: Robert Griffiths, Carnegie-Mellon U; NSF Org:PHY QIS @ NSF goes back a long time ITR: Institute for Quantum Information Award: 0086038; PI: John Preskill; Co-PI:John Doyle, Leonard Schulman, Axel Scherer, Alexei Kitaev, CalTech; NSF Org: CCF Start: 09/01/2000; Award Amount:$5,012,000. -
From 2D Droplets to 2D Yang-Mills Arxiv:2010.11923V1 [Hep-Th]
Prepared for submission to JHEP From 2d Droplets to 2d Yang-Mills Arghya Chattopadhyaya, Suvankar Duttab, Debangshu Mukherjeeb;c, Neetub aInstitute of Mathematical Sciences, Homi Bhaba National Institute (HBNI) IV Cross Road, Taramani, Chennai 600113, Tamil Nadu, India bIndian Institute of Science Education and Research Bhopal Bhopal Bypass, Bhopal 462066, India cIndian Institute of Science Education and Research Thiruvananthapuram Vithura 695551, Kerala, India E-mail: [email protected], [email protected], [email protected], [email protected] Abstract: We establish a connection between time evolution of free Fermi droplets and partition function of generalised q-deformed Yang-Mills theories on Riemann surfaces. Classical phases of (0 + 1) dimensional unitary matrix models can be characterised by free Fermi droplets in two dimensions. We quantise these droplets and find that the modes satisfy an abelian Kac-Moody algebra. The Hilbert spaces H+ and H− associated with the upper and lower free Fermi surfaces of a droplet admit a Young diagram basis in which the phase space Hamiltonian is diagonal with eigenvalue, in the large N limit, equal to the quadratic Casimir of u(N). We establish an exact mapping between states in H± and geometries of droplets. In particular, coherent states in H± correspond to classical deformation of upper and lower Fermi surfaces. We prove that correlation between two coherent states in H± is equal to the chiral and anti-chiral partition function of 2d Yang-Mills theory on a cylinder. Using the fact that the full Hilbert space H+ ⊗ H− admits a composite basis, we show that correlation between two classical droplet geometries is equal to the full U(N) Yang-Mills partition function on cylinder. -
Achievements, Progress and Open Questions in String Field Theory Strings 2021 ICTP-SAIFR, S˜Ao Paulo June 22, 2021
Achievements, Progress and Open Questions in String Field Theory Strings 2021 ICTP-SAIFR, S˜ao Paulo June 22, 2021 Yuji Okawa and Barton Zwiebach 1 Achievements We consider here instances where string field theory provided the answer to physical open questions. • Tachyon condensation, tachyon vacuum, tachyon conjectures The tachyon conjectures (Sen, 1999) posited that: (a) The tachyon potential has a locally stable minimum, whose energy density measured with respect to that of the unstable critical point, equals minus the tension of the D25-brane (b) Lower-dimensional D-branes are solitonic solutions of the string theory on the back- ground of a D25-brane. (c) The locally stable vacuum of the system is the closed string vac- uum; it has no open string excitations exist. Work in SFT established these conjectures by finding the tachyon vac- uum, first numerically, and then analytically (Schnabl, 2005). These are non-perturbative results. 2 • String field theory is the first complete definition of string pertur- bation theory. The first-quantized world-sheet formulation of string theory does not define string perturbation theory completely: – No systematic way of dealing with IR divergences. – No systematic way of dealing with S-matrix elements for states that undergo mass renormalization. Work of A. Sen and collaborators demonstrating this: (a) One loop-mass renormalization of unstable particles in critical string theories. (b) Fixing ambiguities in two-dimensional string theory: For the one- instanton contribution to N-point scattering amplitudes there are four undetermined constants (Balthazar, Rodriguez, Yin, 2019). Two of them have been fixed with SFT (Sen 2020) (c) Fixing the normalization of Type IIB D-instanton amplitudes (Sen, 2021).