Restricted Spin Set Lattice Models A route to Topological Order

Size: px
Start display at page:

Download "Restricted Spin Set Lattice Models A route to Topological Order"

Transcription

1 Restricted Spin Set Lattice Models A route to Topological Order R. Zach Lamberty with Stefanos Papanikolaou and Christopher L. Henley Supported by NSF grant DMR and an NSF GRF APS March Meeting 2012

2 } Our Definition: A state is Topologically Ordered if it possess an entropically degenerate ensemble (in the thermodynamic limit) which cannot be distinguished by local measurements, and cannot be reached by local moves Topological Order Quantum Topological Order } A new knob in the model connects critical models to topologically ordered models Critical Topologically Ordered

3 } Our Definition: A state is Topologically Ordered if it possess an entropically degenerate ensemble (in the thermodynamic limit) which cannot be distinguished by local measurements, and cannot be reached by local moves Topological Order Quantum Topological Order } A new knob in the model connects critical models to topologically ordered models Critical Topologically Ordered

4 } Group } Lattice (Abelian or Non-Abelian) } Periodic Boundary } Directed Spins on edges } Plaquette Constraint } Sectors = loop product } Allowed spin set } Made of conjugacy classes (related by symmetry) Plaquette Product Sector Labels } Non-trivial correlations } Mediated interactions

5 } Group } Lattice (Abelian or Non-Abelian) } Periodic Boundary } Directed Spins on edges } Plaquette Constraint } Sectors = loop product } Allowed spin set } Made of conjugacy classes (related by symmetry) Plaquette Product Sector Labels } Non-trivial correlations } Mediated interactions

6 } Group } Lattice (Abelian or Non-Abelian) } Periodic Boundary } Directed Spins on edges } Plaquette Constraint } Sectors = loop product } Allowed spin set } Made of conjugacy classes (related by symmetry) Plaquette Product Sector Labels } Non-trivial correlations } Mediated interactions

7 } Group } Lattice (Abelian or Non-Abelian) } Periodic Boundary } Directed Spins on edges } Plaquette Constraint } Sectors = loop product } Allowed spin set } Made of conjugacy classes (related by symmetry) Plaquette Product Sector Labels } Non-trivial correlations } Mediated interactions

8 } Group } Lattice (Abelian or Non-Abelian) } Periodic Boundary } Directed Spins on edges } Plaquette Constraint } Sectors = loop product } Allowed spin set } Made of conjugacy classes (related by symmetry) Plaquette Product Sector Labels } Non-trivial correlations } Mediated interactions

9 } Group } Lattice (Abelian or Non-Abelian) } Periodic Boundary } Directed Spins on edges } Plaquette Constraint } Sectors = loop product } Allowed spin set } Made of conjugacy classes (related by symmetry) Plaquette Product Sector Labels } Non-trivial correlations } Mediated interactions

10 Local Local

11 Local Local

12 Global Global

13 Global Global

14 Global Global

15 Global Global

16 Global Global

17 Global Global

18

19

20

21

22 Dimer Model

23 Sector Probabilities Sector Probabilities } Q1: How do we determine a model has Topological Order? } A1: Use sector probabilities as statistical probes } Constrained random walks of defects can change sectors } Sample configurations Sector Sector

24 Sector Probabilities Sector Probabilities } Q1: How do we determine a model has Topological Order? } A1: Use sector probabilities as statistical probes } Constrained random walks of defects can change sectors } Sample configurations Sector Defect Walk Sector

25 Sector Probabilities Sector Probabilities Dimer Model Topologically Ordered Increasing Abelian

26 Sector Probabilities Sector Probabilities Six-Vertex Model Topologically Ordered Increasing Abelian

27 Defect Interactions } Q2: Do we see interactions between defects? Defect Interactions } A2: Restricted spin set non-trivial correlations Distribution of distances from one defect to the other Entropic cost

28 Defect Interactions } Q2: Do we see interactions between defects? Defect Interactions } A2: Restricted spin set non-trivial correlations Distribution of distances from one defect to the other Entropic cost

29 Defect Interactions } The reduced spin set can lead to mediated interactions between defects Critical : TO: Defect Interactions

30 } We have both Abelian and Non-Abelian Classical models with Topological Order } Convergent sector probabilities are a useful diagnostic of Topological Order } Restricting spin degrees of freedom can tune within a family of models from one which is critical to one which is topologically ordered

31 Braiding Features of the Model Bonus Slide Braiding

32 Braiding Features of the Model Bonus Slide Braiding

33 Braiding Features of the Model Bonus Slide Braiding

34 Braiding Features of the Model Bonus Slide Braiding

35 Braiding Features of the Model Bonus Slide Braiding

Non-abelian statistics

Non-abelian statistics Non-abelian statistics Paul Fendley Non-abelian statistics are just plain interesting. They probably occur in the ν = 5/2 FQHE, and people are constructing time-reversal-invariant models which realize

More information

Kitaev honeycomb lattice model: from A to B and beyond

Kitaev honeycomb lattice model: from A to B and beyond Kitaev honeycomb lattice model: from A to B and beyond Jiri Vala Department of Mathematical Physics National University of Ireland at Maynooth Postdoc: PhD students: Collaborators: Graham Kells Ahmet Bolukbasi

More information

Quantum s=1/2 antiferromagnet on the Bethe lattice at percolation I. Low-energy states, DMRG, and diagnostics

Quantum s=1/2 antiferromagnet on the Bethe lattice at percolation I. Low-energy states, DMRG, and diagnostics Quantum s=1/2 antiferromagnet on the Bethe lattice at percolation I. Low-energy states, DMRG, and diagnostics Hitesh J. Changlani, Shivam Ghosh, Sumiran Pujari, Christopher L. Henley Laboratory of Atomic

More information

Universal phase transitions in Topological lattice models

Universal phase transitions in Topological lattice models Universal phase transitions in Topological lattice models F. J. Burnell Collaborators: J. Slingerland S. H. Simon September 2, 2010 Overview Matter: classified by orders Symmetry Breaking (Ferromagnet)

More information

Criticality in topologically ordered systems: a case study

Criticality in topologically ordered systems: a case study Criticality in topologically ordered systems: a case study Fiona Burnell Schulz & FJB 16 FJB 17? Phases and phase transitions ~ 194 s: Landau theory (Liquids vs crystals; magnets; etc.) Local order parameter

More information

Topological order from quantum loops and nets

Topological order from quantum loops and nets Topological order from quantum loops and nets Paul Fendley It has proved to be quite tricky to T -invariant spin models whose quasiparticles are non-abelian anyons. 1 Here I ll describe the simplest (so

More information

Realizing non-abelian statistics in quantum loop models

Realizing non-abelian statistics in quantum loop models Realizing non-abelian statistics in quantum loop models Paul Fendley Experimental and theoretical successes have made us take a close look at quantum physics in two spatial dimensions. We have now found

More information

Understanding Topological Order with PEPS. David Pérez-García Autrans Summer School 2016

Understanding Topological Order with PEPS. David Pérez-García Autrans Summer School 2016 Understanding Topological Order with PEPS David Pérez-García Autrans Summer School 2016 Outlook 1. An introduc

More information

Geometry, topology and frustration: the physics of spin ice

Geometry, topology and frustration: the physics of spin ice Geometry, topology and frustration: the physics of spin ice Roderich Moessner CNRS and LPT-ENS 9 March 25, Magdeburg Overview Spin ice: experimental discovery and basic model Spin ice in a field dimensional

More information

Paramagnetic phases of Kagome lattice quantum Ising models p.1/16

Paramagnetic phases of Kagome lattice quantum Ising models p.1/16 Paramagnetic phases of Kagome lattice quantum Ising models Predrag Nikolić In collaboration with T. Senthil Massachusetts Institute of Technology Paramagnetic phases of Kagome lattice quantum Ising models

More information

Topological order of a two-dimensional toric code

Topological order of a two-dimensional toric code University of Ljubljana Faculty of Mathematics and Physics Seminar I a, 1st year, 2nd cycle Topological order of a two-dimensional toric code Author: Lenart Zadnik Advisor: Doc. Dr. Marko Žnidarič June

More information

Ψ({z i }) = i<j(z i z j ) m e P i z i 2 /4, q = ± e m.

Ψ({z i }) = i<j(z i z j ) m e P i z i 2 /4, q = ± e m. Fractionalization of charge and statistics in graphene and related structures M. Franz University of British Columbia franz@physics.ubc.ca January 5, 2008 In collaboration with: C. Weeks, G. Rosenberg,

More information

Shunsuke Furukawa Condensed Matter Theory Lab., RIKEN. Gregoire Misguich Vincent Pasquier Service de Physique Theorique, CEA Saclay, France

Shunsuke Furukawa Condensed Matter Theory Lab., RIKEN. Gregoire Misguich Vincent Pasquier Service de Physique Theorique, CEA Saclay, France Shunsuke Furukawa Condensed Matter Theory Lab., RIKEN in collaboration with Gregoire Misguich Vincent Pasquier Service de Physique Theorique, CEA Saclay, France : ground state of the total system Reduced

More information

Intoduction to topological order and topologial quantum computation. Arnau Riera, Grup QIC, Dept. ECM, UB 16 de maig de 2009

Intoduction to topological order and topologial quantum computation. Arnau Riera, Grup QIC, Dept. ECM, UB 16 de maig de 2009 Intoduction to topological order and topologial quantum computation Arnau Riera, Grup QIC, Dept. ECM, UB 16 de maig de 2009 Outline 1. Introduction: phase transitions and order. 2. The Landau symmetry

More information

Exploring Topological Phases With Quantum Walks

Exploring Topological Phases With Quantum Walks Exploring Topological Phases With Quantum Walks Tk Takuya Kitagawa, Erez Berg, Mark Rudner Eugene Demler Harvard University References: PRA 82:33429 and PRB 82:235114 (2010) Collaboration with A. White

More information

Jiannis K. Pachos. Introduction. Berlin, September 2013

Jiannis K. Pachos. Introduction. Berlin, September 2013 Jiannis K. Pachos Introduction Berlin, September 203 Introduction Quantum Computation is the quest for:» neat quantum evolutions» new quantum algorithms Why? 2D Topological Quantum Systems: How? ) Continuum

More information

Topological Field Theory and Conformal Quantum Critical Points

Topological Field Theory and Conformal Quantum Critical Points Topological Field Theory and Conformal Quantum Critical Points One might expect that the quasiparticles over a Fermi sea have quantum numbers (charge, spin) of an electron. This is not always true! Charge

More information

Finite Temperature Quantum Memory and Haah s Code

Finite Temperature Quantum Memory and Haah s Code Finite Temperature Quantum Memory and Haah s Code S.M. Kravec 1 1 Department of Physics, University of California at San Diego, La Jolla, CA 92093 This paper addresses the question of whether realizations

More information

5 Topological defects and textures in ordered media

5 Topological defects and textures in ordered media 5 Topological defects and textures in ordered media In this chapter we consider how to classify topological defects and textures in ordered media. We give here only a very short account of the method following

More information

The uses of Instantons for classifying Topological Phases

The uses of Instantons for classifying Topological Phases The uses of Instantons for classifying Topological Phases - anomaly-free and chiral fermions Juven Wang, Xiao-Gang Wen (arxiv:1307.7480, arxiv:140?.????) MIT/Perimeter Inst. 2014 @ APS March A Lattice

More information

Boulder School 2016 Xie Chen 07/28/16-08/02/16

Boulder School 2016 Xie Chen 07/28/16-08/02/16 Boulder School 2016 Xie Chen 07/28/16-08/02/16 Symmetry Fractionalization 1 Introduction This lecture is based on review article Symmetry Fractionalization in Two Dimensional Topological Phases, arxiv:

More information

Think Globally, Act Locally

Think Globally, Act Locally Think Globally, Act Locally Nathan Seiberg Institute for Advanced Study Quantum Fields beyond Perturbation Theory, KITP 2014 Ofer Aharony, NS, Yuji Tachikawa, arxiv:1305.0318 Anton Kapustin, Ryan Thorngren,

More information

Anyons are not energy eigenspaces of quantum double Hamiltonians

Anyons are not energy eigenspaces of quantum double Hamiltonians PHYSICAL REVIEW B 96, 195150 (2017) Anyons are not energy eigenspaces of quantum double Hamiltonians Anna Kómár 1,* and Olivier Landon-Cardinal 2, 1 Institute for Quantum Information and Matter and Walter

More information

Outline for Fundamentals of Statistical Physics Leo P. Kadanoff

Outline for Fundamentals of Statistical Physics Leo P. Kadanoff Outline for Fundamentals of Statistical Physics Leo P. Kadanoff text: Statistical Physics, Statics, Dynamics, Renormalization Leo Kadanoff I also referred often to Wikipedia and found it accurate and helpful.

More information

SU(N) magnets: from a theoretical abstraction to reality

SU(N) magnets: from a theoretical abstraction to reality 1 SU(N) magnets: from a theoretical abstraction to reality Victor Gurarie University of Colorado, Boulder collaboration with M. Hermele, A.M. Rey Aspen, May 2009 In this talk 2 SU(N) spin models are more

More information

Defects in topologically ordered states. Xiao-Liang Qi Stanford University Mag Lab, Tallahassee, 01/09/2014

Defects in topologically ordered states. Xiao-Liang Qi Stanford University Mag Lab, Tallahassee, 01/09/2014 Defects in topologically ordered states Xiao-Liang Qi Stanford University Mag Lab, Tallahassee, 01/09/2014 References Maissam Barkeshli & XLQ, PRX, 2, 031013 (2012) Maissam Barkeshli, Chaoming Jian, XLQ,

More information

SPIN LIQUIDS AND FRUSTRATED MAGNETISM

SPIN LIQUIDS AND FRUSTRATED MAGNETISM SPIN LIQUIDS AND FRUSTRATED MAGNETISM Classical correlations, emergent gauge fields and fractionalised excitations John Chalker Physics Department, Oxford University For written notes see: http://topo-houches.pks.mpg.de/

More information

Time reversal invariant gapped boundaries of the double semion state

Time reversal invariant gapped boundaries of the double semion state PHYSICAL REVIEW B 93, 35161 (016) Time reversal invariant gapped boundaries of the double semion state Fiona Burnell, 1 Xie Chen,,3 Alexei Kitaev, Max Metlitski, 4 and Ashvin Vishwanath 3,5 1 Department

More information

arxiv: v3 [cond-mat.str-el] 23 Sep 2008

arxiv: v3 [cond-mat.str-el] 23 Sep 2008 A Family of Non-Abelian Kitaev Models on a Lattice: Topological Condensation and confinement H. Bombin and M.A. Martin-Delgado Departamento de Física Teórica I, Universidad Complutense, 28040. Madrid,

More information

Quantum Monte Carlo Simulations in the Valence Bond Basis. Anders Sandvik, Boston University

Quantum Monte Carlo Simulations in the Valence Bond Basis. Anders Sandvik, Boston University Quantum Monte Carlo Simulations in the Valence Bond Basis Anders Sandvik, Boston University Outline The valence bond basis for S=1/2 spins Projector QMC in the valence bond basis Heisenberg model with

More information

Quantum Monte Carlo study of a Z 2 gauge theory containing phases with and without a Luttinger volume Fermi surface

Quantum Monte Carlo study of a Z 2 gauge theory containing phases with and without a Luttinger volume Fermi surface Quantum Monte Carlo study of a Z 2 gauge theory containing phases with and without a Luttinger volume Fermi surface V44.00011 APS March Meeting, Los Angeles Fakher Assaad, Snir Gazit, Subir Sachdev, Ashvin

More information

Degeneracy Breaking in Some Frustrated Magnets

Degeneracy Breaking in Some Frustrated Magnets Degeneracy Breaking in Some Frustrated Magnets Doron Bergman Greg Fiete Ryuichi Shindou Simon Trebst UCSB Physics KITP UCSB Physics Q Station cond-mat: 0510202 (prl) 0511176 (prb) 0605467 0607210 0608131

More information

Many-body Characterization of Particle-Conserving Topological Superfluids

Many-body Characterization of Particle-Conserving Topological Superfluids Many-body Characterization of Particle-Conserving Topological Superfluids Gerardo Ortiz Department of Physics - Indiana University INT-15-1 - March 2015 Collaborators: Jorge Dukelsky: CSIC - Madrid Emilio

More information

Quantum computation in topological Hilbertspaces. A presentation on topological quantum computing by Deniz Bozyigit and Martin Claassen

Quantum computation in topological Hilbertspaces. A presentation on topological quantum computing by Deniz Bozyigit and Martin Claassen Quantum computation in topological Hilbertspaces A presentation on topological quantum computing by Deniz Bozyigit and Martin Claassen Introduction In two words what is it about? Pushing around fractionally

More information

High-Temperature Criticality in Strongly Constrained Quantum Systems

High-Temperature Criticality in Strongly Constrained Quantum Systems High-Temperature Criticality in Strongly Constrained Quantum Systems Claudio Chamon Collaborators: Claudio Castelnovo - BU Christopher Mudry - PSI, Switzerland Pierre Pujol - ENS Lyon, France PRB 2006

More information

arxiv: v2 [cond-mat.str-el] 20 Apr 2015

arxiv: v2 [cond-mat.str-el] 20 Apr 2015 Gauging time reversal symmetry in tensor network states ie Chen, 2 and Ashvin Vishwanath 2 Department of Physics and Institute for Quantum Information and Matter, California Institute of echnology, Pasadena,

More information

The Kitaev models. The toric code 1. PHYS598PTD A.J.Leggett 2016 Lecture 27 The Kitaev models 1

The Kitaev models. The toric code 1. PHYS598PTD A.J.Leggett 2016 Lecture 27 The Kitaev models 1 PHYS598PTD A.J.Leggett 2016 Lecture 27 The Kitaev models 1 The Kitaev models Since many of the ideas involved in TQC appear rather abstract and perhaps a priori speculative, it is useful to have a concrete

More information

(IN)EQUIVALENCE OF COLOR CODE AND TORIC CODE. Aleksander Kubica, B. Yoshida, F. Pastawski

(IN)EQUIVALENCE OF COLOR CODE AND TORIC CODE. Aleksander Kubica, B. Yoshida, F. Pastawski (IN)EQUIVALENCE OF COLOR CODE AND TORIC CODE Aleksander Kubica, B. Yoshida, F. Pastawski MOTIVATION Topological quantum codes - non-local DOFs, local generators. Toric code: high threshold, experimentally

More information

Parallelization of the Dirac operator. Pushan Majumdar. Indian Association for the Cultivation of Sciences, Jadavpur, Kolkata

Parallelization of the Dirac operator. Pushan Majumdar. Indian Association for the Cultivation of Sciences, Jadavpur, Kolkata Parallelization of the Dirac operator Pushan Majumdar Indian Association for the Cultivation of Sciences, Jadavpur, Kolkata Outline Introduction Algorithms Parallelization Comparison of performances Conclusions

More information

Quantum dots and Majorana Fermions Karsten Flensberg

Quantum dots and Majorana Fermions Karsten Flensberg Quantum dots and Majorana Fermions Karsten Flensberg Center for Quantum Devices University of Copenhagen Collaborator: Martin Leijnse and R. Egger M. Kjærgaard K. Wölms Outline: - Introduction to Majorana

More information

arxiv: v1 [cond-mat.str-el] 11 Sep 2015

arxiv: v1 [cond-mat.str-el] 11 Sep 2015 Gapped boundaries, group cohomology and fault-tolerant logical gates NSF-KITP-15-096 Beni Yoshida Walter Burke Institute for Theoretical Physics, California Institute of Technology, Pasadena, California

More information

After first studying an example of a topological phase and its underlying structures, we study effective field theories for 2D topological phases.

After first studying an example of a topological phase and its underlying structures, we study effective field theories for 2D topological phases. 1 Boulder notes by Victor V Albert I CHETAN NAYAK After first studying an example of a topological phase and its underlying structures, we study effective field theories for D topological phases I1 Example

More information

Dimer model implementations of quantum loop gases. C. Herdman, J. DuBois, J. Korsbakken, K. B. Whaley UC Berkeley

Dimer model implementations of quantum loop gases. C. Herdman, J. DuBois, J. Korsbakken, K. B. Whaley UC Berkeley Dimer model implementations of quantum loop gases C. Herdman, J. DuBois, J. Korsbakken, K. B. Whaley UC Berkeley Outline d-isotopic quantum loop gases and dimer model implementations generalized RK points

More information

been succeeded in 1997 Rb, 23 Na, 7 Li, 1 H, 85 Rb, 41 K, 4 He, 133 Cs, 174 Yb, 52 Cr, 40 Ca, 84 Sr, 164 Dy Laser cooling Trap of atoms 87

been succeeded in 1997 Rb, 23 Na, 7 Li, 1 H, 85 Rb, 41 K, 4 He, 133 Cs, 174 Yb, 52 Cr, 40 Ca, 84 Sr, 164 Dy Laser cooling Trap of atoms 87 Non-Abelian Vortices and Their Non-equilibrium Michikazu Kobayashi a University of Tokyo November 18th, 2011 at Keio University 2 nd Workshop on Quarks and Hadrons under Extreme Conditions - Lattice QCD,

More information

Super Efimov effect. Sergej Moroz University of Washington. together with Yusuke Nishida and Dam Thanh Son. Tuesday, April 1, 14

Super Efimov effect. Sergej Moroz University of Washington. together with Yusuke Nishida and Dam Thanh Son. Tuesday, April 1, 14 Super Efimov effect together with Yusuke Nishida and Dam Thanh Son Sergej Moroz University of Washington Few-body problems They are challenging but useful: Newton gravity Quantum atoms Quantum molecules

More information

VI.D Self Duality in the Two Dimensional Ising Model

VI.D Self Duality in the Two Dimensional Ising Model VI.D Self Duality in the Two Dimensional Ising Model Kramers and Wannier discovered a hidden symmetry that relates the properties of the Ising model on the square lattice at low and high temperatures.

More information

Modern Statistical Mechanics Paul Fendley

Modern Statistical Mechanics Paul Fendley Modern Statistical Mechanics Paul Fendley The point of the book This book, Modern Statistical Mechanics, is an attempt to cover the gap between what is taught in a conventional statistical mechanics class

More information

arxiv: v1 [cond-mat.str-el] 7 Aug 2011

arxiv: v1 [cond-mat.str-el] 7 Aug 2011 Topological Geometric Entanglement of Blocks Román Orús 1, 2 and Tzu-Chieh Wei 3, 4 1 School of Mathematics and Physics, The University of Queensland, QLD 4072, Australia 2 Max-Planck-Institut für Quantenoptik,

More information

Entanglement entropy and gauge fields

Entanglement entropy and gauge fields Entanglement entropy and gauge fields H. C., M.Huerta and A. Rosabal (2012) H. C., M. Huerta (2014) H. C., M. Huerta, in preparation Puzzling results Lattice calculations with extended lattice (Buividovich-Polikarpov,

More information

Degeneracy Breaking in Some Frustrated Magnets. Bangalore Mott Conference, July 2006

Degeneracy Breaking in Some Frustrated Magnets. Bangalore Mott Conference, July 2006 Degeneracy Breaking in Some Frustrated Magnets Doron Bergman Greg Fiete Ryuichi Shindou Simon Trebst UCSB Physics KITP UCSB Physics Q Station Bangalore Mott Conference, July 2006 Outline Motivation: Why

More information

arxiv: v3 [cond-mat.str-el] 4 Aug 2017

arxiv: v3 [cond-mat.str-el] 4 Aug 2017 Symmetry reduction induced by anyon condensation: a tensor network approach José arre-rubio, Sofyan Iblisdir, David Pérez-arcía Departamento de Análisis Matemático, Universidad Complutense de Madrid, 28040

More information

Category theory and topological quantum computing

Category theory and topological quantum computing Categor theor and topological quantum computing Gregor Schaumann Group seminar QOS Freiburg 7..3 Introduction Conformal field theor Invariants of manifolds and knots Topological field theor Tensor categories

More information

H ψ = E ψ. Introduction to Exact Diagonalization. Andreas Läuchli, New states of quantum matter MPI für Physik komplexer Systeme - Dresden

H ψ = E ψ. Introduction to Exact Diagonalization. Andreas Läuchli, New states of quantum matter MPI für Physik komplexer Systeme - Dresden H ψ = E ψ Introduction to Exact Diagonalization Andreas Läuchli, New states of quantum matter MPI für Physik komplexer Systeme - Dresden http://www.pks.mpg.de/~aml laeuchli@comp-phys.org Simulations of

More information

3D topological insulators and half- Heusler compounds

3D topological insulators and half- Heusler compounds 3D topological insulators and half- Heusler compounds Ram Seshadri Materials Department, and Department of Chemistry and Biochemistry Materials Research Laboratory University of California, Santa Barbara

More information

Vertex operator algebras as a new type of symmetry. Beijing International Center for Mathematical Research Peking Universty

Vertex operator algebras as a new type of symmetry. Beijing International Center for Mathematical Research Peking Universty Vertex operator algebras as a new type of symmetry Yi-Zhi Huang Department of Mathematics Rutgers University Beijing International Center for Mathematical Research Peking Universty July 8, 2010 1. What

More information

Applications to simulations: Monte-Carlo

Applications to simulations: Monte-Carlo Applications to simulations: Monte-Carlo A.C. Maggs ESPCI, Paris June 2016 Summary Algorithms Faster/simpler codes Thermodynamics of Electric fields Partition function of electric field Thermal Casimir/Lifshitz

More information

arxiv: v1 [cond-mat.str-el] 6 May 2010

arxiv: v1 [cond-mat.str-el] 6 May 2010 MIT-CTP/4147 Correlated Topological Insulators and the Fractional Magnetoelectric Effect B. Swingle, M. Barkeshli, J. McGreevy, and T. Senthil Department of Physics, Massachusetts Institute of Technology,

More information

arxiv: v2 [cond-mat.str-el] 28 Jul 2010

arxiv: v2 [cond-mat.str-el] 28 Jul 2010 Topological Order with a Twist: Ising Anyons from an Abelian Model H. Bombin Perimeter Institute for Theoretical Physics, 31 Caroline St. N., Waterloo, Ontario N2L 2Y5, Canada Anyon models can be symmetric

More information

Eric Perlmutter, DAMTP, Cambridge

Eric Perlmutter, DAMTP, Cambridge Eric Perlmutter, DAMTP, Cambridge Based on work with: P. Kraus; T. Prochazka, J. Raeymaekers ; E. Hijano, P. Kraus; M. Gaberdiel, K. Jin TAMU Workshop, Holography and its applications, April 10, 2013 1.

More information

Overview of Topological Cluster-State Quantum Computation on 2D Cluster-State

Overview of Topological Cluster-State Quantum Computation on 2D Cluster-State Overview of Topological Cluster-State Quantum Computation on 2D Cluster-State based on High-threshold universal quantum computation on the surface code -Austin G. Fowler, Ashley M. Stephens, and Peter

More information

The path integral for photons

The path integral for photons The path integral for photons based on S-57 We will discuss the path integral for photons and the photon propagator more carefully using the Lorentz gauge: as in the case of scalar field we Fourier-transform

More information

Topology driven quantum phase transitions

Topology driven quantum phase transitions Topology driven quantum phase transitions Dresden July 2009 Simon Trebst Microsoft Station Q UC Santa Barbara Charlotte Gils Alexei Kitaev Andreas Ludwig Matthias Troyer Zhenghan Wang Topological quantum

More information

EDMs from the QCD θ term

EDMs from the QCD θ term ACFI EDM School November 2016 EDMs from the QCD θ term Vincenzo Cirigliano Los Alamos National Laboratory 1 Lecture II outline The QCD θ term Toolbox: chiral symmetries and their breaking Estimate of the

More information

A Superconducting Quantum Simulator for Topological Order and the Toric Code. Michael J. Hartmann Heriot-Watt University, Edinburgh qlightcrete 2016

A Superconducting Quantum Simulator for Topological Order and the Toric Code. Michael J. Hartmann Heriot-Watt University, Edinburgh qlightcrete 2016 A Superconducting Quantum Simulator for Topological Order and the Toric Code Michael J. Hartmann Heriot-Watt University, Edinburgh qlightcrete 2016 Topological Order (in 2D) A 2-dimensional physical system

More information

Surface Defects, Symmetries and Dualities

Surface Defects, Symmetries and Dualities Surface Defects, Symmetries and Dualities Christoph Schweigert Hamburg University, Department of Mathematics and Center for Mathematical Physics joint with Jürgen Fuchs, Jan Priel and Alessandro Valentino

More information

Introduction to Topological Error Correction and Computation. James R. Wootton Universität Basel

Introduction to Topological Error Correction and Computation. James R. Wootton Universität Basel Introduction to Topological Error Correction and Computation James R. Wootton Universität Basel Overview Part 1: Topological Quantum Computation Abelian and non-abelian anyons Quantum gates with Abelian

More information

Electric Dipole Paradox: Question, Answer, and Interpretation

Electric Dipole Paradox: Question, Answer, and Interpretation Electric Dipole Paradox: Question, Answer, and Interpretation Frank Wilczek January 16, 2014 Abstract Non-vanishing electric dipole moments for the electron, neutron, or other entities are classic signals

More information

VI.D Self Duality in the Two Dimensional Ising Model

VI.D Self Duality in the Two Dimensional Ising Model VI.D Self Duality in the Two Dimensional Ising Model Kramers and Wannier discovered a hidden symmetry that relates the properties of the Ising model on the square lattice at low and high temperatures.

More information

Many-Body Fermion Density Matrix: Operator-Based Truncation Scheme

Many-Body Fermion Density Matrix: Operator-Based Truncation Scheme Many-Body Fermion Density Matrix: Operator-Based Truncation Scheme SIEW-ANN CHEONG and C. L. HENLEY, LASSP, Cornell U March 25, 2004 Support: NSF grants DMR-9981744, DMR-0079992 The Big Picture GOAL Ground

More information

arxiv: v3 [cond-mat.str-el] 15 Jan 2015

arxiv: v3 [cond-mat.str-el] 15 Jan 2015 Boundary Degeneracy of Topological Order Juven C. Wang 1, 2, 2, 1, 3, and Xiao-Gang Wen 1 Department of Physics, Massachusetts Institute of Technology, Cambridge, MA 02139, USA 2 Perimeter Institute for

More information

Anyonic Chains, Topological Defects, and Conformal Field Theory

Anyonic Chains, Topological Defects, and Conformal Field Theory QMUL-PH-17-01, EFI-16-29 Anyonic Chains, Topological Defects, and Conformal Field Theory arxiv:1701.02800v2 [hep-th] 20 Feb 2017 Matthew Buican,1 and Andrey Gromov,2 1 CRST and School of Physics and Astronomy

More information

Quantum Symmetry Reduction for Diffeomorphism Invariant Theories of Connections

Quantum Symmetry Reduction for Diffeomorphism Invariant Theories of Connections PITHA 99/23 hep-th/9907042 arxiv:hep-th/9907042v1 7 Jul 1999 Quantum Symmetry Reduction for Diffeomorphism Invariant Theories of Connections M. Bojowald 1 and H.A. Kastrup 2 Institute for Theoretical Physics

More information

August 28, 2016 (Sunday)

August 28, 2016 (Sunday) August 28, 2016 (Sunday) 09:00-10: 30 The Theory of Statistical Comparison with Applications in Quantum Information Science....... 1 Francesco Buscemi (Nagoya University) 10:50-12:20 Introduction to measurement-based

More information

THE ABC OF COLOR CODES

THE ABC OF COLOR CODES THE ABC OF COLOR CODES Aleksander Kubica ariv:1410.0069, 1503.02065 work in progress w/ F. Brandao, K. Svore, N. Delfosse 1 WHY DO WE CARE ABOUT QUANTUM CODES? Goal: store information and perform computation.

More information

Defects in topological field theory: from categorical tools to applications in physics and representation theory

Defects in topological field theory: from categorical tools to applications in physics and representation theory Defects in topological field theory: from categorical tools to applications in physics and representation theory Christoph Schweigert Mathematics Department Hamburg University based on work with Jürgen

More information

Kai Sun. University of Michigan, Ann Arbor. Collaborators: Krishna Kumar and Eduardo Fradkin (UIUC)

Kai Sun. University of Michigan, Ann Arbor. Collaborators: Krishna Kumar and Eduardo Fradkin (UIUC) Kai Sun University of Michigan, Ann Arbor Collaborators: Krishna Kumar and Eduardo Fradkin (UIUC) Outline How to construct a discretized Chern-Simons gauge theory A necessary and sufficient condition for

More information

arxiv:hep-lat/ v1 30 May 1995

arxiv:hep-lat/ v1 30 May 1995 MONOPOLES IN COMPACT U(1) ANATOMY OF THE PHASE TRANSITION A. Bode Physics Department, Humboldt University D-10115 Berlin, Germany E-mail: achim@eiche.physik.hu-berlin.de arxiv:hep-lat/9505026v1 30 May

More information

Simulations of Quantum Dimer Models

Simulations of Quantum Dimer Models Simulations of Quantum Dimer Models Didier Poilblanc Laboratoire de Physique Théorique CNRS & Université de Toulouse 1 A wide range of applications Disordered frustrated quantum magnets Correlated fermions

More information

Entanglement Entropy In Gauge Theories. Sandip Trivedi Tata Institute of Fundamental Research, Mumbai, India.

Entanglement Entropy In Gauge Theories. Sandip Trivedi Tata Institute of Fundamental Research, Mumbai, India. Entanglement Entropy In Gauge Theories Sandip Trivedi Tata Institute of Fundamental Research, Mumbai, India. On The Entanglement Entropy For Gauge Theories, arxiv: 1501.2593 Sudip Ghosh, Ronak Soni and

More information

Derivation of Electro Weak Unification and Final Form of Standard Model with QCD and Gluons 1 W W W 3

Derivation of Electro Weak Unification and Final Form of Standard Model with QCD and Gluons 1 W W W 3 Derivation of Electro Weak Unification and Final Form of Standard Model with QCD and Gluons 1 W 1 + 2 W 2 + 3 W 3 Substitute B = cos W A + sin W Z 0 Sum over first generation particles. up down Left handed

More information

Symmetry in quantum walks on graphs

Symmetry in quantum walks on graphs NSF Workshop on Quantum Information Processing and Nanoscale Systems, September 2007 Symmetry in quantum walks on graphs Hari Krovi and Todd Brun Communication Sciences Institute Ming Hsieh Department

More information

Large-N Quantum Field Theories and Nonlinear Random Processes

Large-N Quantum Field Theories and Nonlinear Random Processes Large-N Quantum Field Theories and Nonlinear Random Processes Pavel Buividovich (ITEP, Moscow and JINR, Dubna) ITEP Lattice Seminar, 16.09.2010 Motivation Problems for modern Lattice QCD simulations(based

More information

Subfactors and Topological Defects in Conformal Quantum Field Theory

Subfactors and Topological Defects in Conformal Quantum Field Theory Subfactors and Topological Defects in Conformal Quantum Field Theory Marcel Bischoff http://www.math.vanderbilt.edu/~bischom Department of Mathematics Vanderbilt University Nashville, TN San Antonio, TX,

More information

Defects between Gapped Boundaries in (2 + 1)D Topological Phases of Matter

Defects between Gapped Boundaries in (2 + 1)D Topological Phases of Matter Defects between Gapped Boundaries in (2 + 1)D Topological Phases of Matter Iris Cong, Meng Cheng, Zhenghan Wang cong@g.harvard.edu Department of Physics Harvard University, Cambridge, MA January 13th,

More information

Martin Schnabl. Institute of Physics AS CR. Collaborators: T. Kojita, M. Kudrna, C. Maccaferri, T. Masuda and M. Rapčák

Martin Schnabl. Institute of Physics AS CR. Collaborators: T. Kojita, M. Kudrna, C. Maccaferri, T. Masuda and M. Rapčák Martin Schnabl Collaborators: T. Kojita, M. Kudrna, C. Maccaferri, T. Masuda and M. Rapčák Institute of Physics AS CR 36th Winter School Geometry and Physics, Srní, January 22nd, 2016 2d Conformal Field

More information

Anyons and topological quantum computing

Anyons and topological quantum computing Anyons and topological quantum computing Statistical Physics PhD Course Quantum statistical physics and Field theory 05/10/2012 Plan of the seminar Why anyons? Anyons: definitions fusion rules, F and R

More information

Fully symmetric and non-fractionalized Mott insulators at fractional site-filling

Fully symmetric and non-fractionalized Mott insulators at fractional site-filling Fully symmetric and non-fractionalized Mott insulators at fractional site-filling Itamar Kimchi University of California, Berkeley EQPCM @ ISSP June 19, 2013 PRL 2013 (kagome), 1207.0498...[PNAS] (honeycomb)

More information

From Majorana Fermions to Topological Order

From Majorana Fermions to Topological Order From Majorana Fermions to Topological Order Arxiv: 1201.3757, to appear in PRL. B.M. Terhal, F. Hassler, D.P. DiVincenzo IQI, RWTH Aachen We are looking for PhD students or postdocs for theoretical research

More information

team Hans Peter Büchler Nicolai Lang Mikhail Lukin Norman Yao Sebastian Huber

team Hans Peter Büchler Nicolai Lang Mikhail Lukin Norman Yao Sebastian Huber title 1 team 2 Hans Peter Büchler Nicolai Lang Mikhail Lukin Norman Yao Sebastian Huber motivation: topological states of matter 3 fermions non-interacting, filled band (single particle physics) topological

More information

condensates and topology fixing action

condensates and topology fixing action condensates and topology fixing action Hidenori Fukaya YITP, Kyoto Univ. hep-lat/0403024 Collaboration with T.Onogi (YITP) 1. Introduction Why topology fixing action? An action proposed by Luscher provide

More information

Non-Abelian Statistics. in the Fractional Quantum Hall States * X. G. Wen. School of Natural Sciences. Institute of Advanced Study

Non-Abelian Statistics. in the Fractional Quantum Hall States * X. G. Wen. School of Natural Sciences. Institute of Advanced Study IASSNS-HEP-90/70 Sep. 1990 Non-Abelian Statistics in the Fractional Quantum Hall States * X. G. Wen School of Natural Sciences Institute of Advanced Study Princeton, NJ 08540 ABSTRACT: The Fractional Quantum

More information

Low energy effec,ve theories for metals. Sung-Sik Lee McMaster University Perimeter Ins,tute

Low energy effec,ve theories for metals. Sung-Sik Lee McMaster University Perimeter Ins,tute Low energy effec,ve theories for metals Sung-Sik Lee McMaster University Perimeter Ins,tute Goal of many-body physics : to extract a small set of useful informa,on out of a large number of degrees of freedom

More information

Topological Quantum Computation. Zhenghan Wang Microsoft Station Q & UC Sana Barbara Texas, March 26, 2015

Topological Quantum Computation. Zhenghan Wang Microsoft Station Q & UC Sana Barbara Texas, March 26, 2015 Topological Quantum Computation Zhenghan Wang Microsoft Station Q & UC Sana Barbara Texas, March 26, 2015 Classical Physics Turing Model Quantum Mechanics Quantum Computing Quantum Field Theory??? String

More information

arxiv:cond-mat/ v1 12 Dec 2006

arxiv:cond-mat/ v1 12 Dec 2006 Universal properties of highly frustrated quantum magnets in strong magnetic fields Oleg Derzhko 1,2,3, Johannes Richter 3,2, Andreas Honecker 4, and Heinz-Jürgen Schmidt 5 1 Institute for Condensed Matter

More information

arxiv: v1 [cond-mat.str-el] 22 Oct 2015

arxiv: v1 [cond-mat.str-el] 22 Oct 2015 arxiv:1510.06627v1 [cond-mat.str-el] 22 Oct 2015 Generating domain walls between topologically ordered phases using quantum double models Miguel Jorge Bernabé Ferreira, a Pramod Padmanabhan, a,b Paulo

More information

Free fields, Quivers and Riemann surfaces

Free fields, Quivers and Riemann surfaces Free fields, Quivers and Riemann surfaces Sanjaye Ramgoolam Queen Mary, University of London 11 September 2013 Quivers as Calculators : Counting, correlators and Riemann surfaces, arxiv:1301.1980, J. Pasukonis,

More information

Zero-temperature phase transitions of an antiferromagnetic Ising model of general spin on a triangular lattice

Zero-temperature phase transitions of an antiferromagnetic Ising model of general spin on a triangular lattice PHYSICAL REVIEW B VOLUME 55, NUMBER 22 1 JUNE 1997-II Zero-temperature phase transitions of an antiferromagnetic Ising model of general spin on a triangular lattice Chen Zeng * Department of Physics, Syracuse

More information

Topological states in quantum antiferromagnets

Topological states in quantum antiferromagnets Pierre Pujol Laboratoire de Physique Théorique Université Paul Sabatier, Toulouse Topological states in quantum antiferromagnets Thanks to I. Makhfudz, S. Takayoshi and A. Tanaka Quantum AF systems : GS

More information

Topological Insulators in 3D and Bosonization

Topological Insulators in 3D and Bosonization Topological Insulators in 3D and Bosonization Andrea Cappelli, INFN Florence (w. E. Randellini, J. Sisti) Outline Topological states of matter: bulk and edge Fermions and bosons on the (1+1)-dimensional

More information

Matrix Product Operators: Algebras and Applications

Matrix Product Operators: Algebras and Applications Matrix Product Operators: Algebras and Applications Frank Verstraete Ghent University and University of Vienna Nick Bultinck, Jutho Haegeman, Michael Marien Burak Sahinoglu, Dominic Williamson Ignacio

More information