Topological Quantum Computing with Majorana Zero Modes and Beyond

Total Page:16

File Type:pdf, Size:1020Kb

Topological Quantum Computing with Majorana Zero Modes and Beyond UC Santa Barbara UC Santa Barbara Electronic Theses and Dissertations Title Topological Quantum Computing with Majorana Zero Modes and Beyond Permalink https://escholarship.org/uc/item/04305656 Author Knapp, Christina Publication Date 2019 Peer reviewed|Thesis/dissertation eScholarship.org Powered by the California Digital Library University of California UNIVERSITY of CALIFORNIA Santa Barbara Topological Quantum Computing with Majorana Zero Modes and Beyond A dissertation submitted in partial satisfaction of the requirements for the degree of Doctor of Philosophy in Physics by Christina Paulsen Knapp Committee in charge: Professor Chetan Nayak, Chair Professor Leon Balents Professor Andrea F. Young June 2019 The dissertation of Christina Paulsen Knapp is approved: Professor Leon Balents Professor Andrea F. Young Professor Chetan Nayak, Chair June 2019 Copyright ⃝c 2019 by Christina Paulsen Knapp iii Of course it is happening in your head, Harry, but why on earth should that mean it is not real? -J.K. Rowling, Harry Potter and the Deathly Hallows To my grandparents, John and Betsy Tower, and Harold and Barbara Knapp, for instilling in me the value of learning. iv Acknowledgements I am immensely grateful to many people for making graduate school a successful and en- joyable experience. First, I would like to thank my advisor Chetan Nayak for introducing me to the field of topological phases and for his patience and guidance throughout my Ph.D. Chetan’s balance of providing direction when necessary and encouraging independence when possible has been essential for my growth as a physicist. His good humor and breadth of expertise has fostered a particularly fun and vibrant group that I feel incredibly fortunate to have joined. Next, I would like to thank Parsa Bonderson, who has in many ways acted as my unofficial co-advisor. In addition to leading me deeper into diagrammatic calculus than I ever anticipated I would dive, Parsa’s meticulous revisions of paper drafts and practice talks have held me to a higher standard than I would have otherwise achieved. I am indebted to him for hours of career advice, scientific guidance, and social commentary. I am extremely grateful to my committee members Leon Balents and Andrea Young for their time and advice. Leon’s group meetings have provided me a glimpse into the greater world of topological physics. Andrea graciously welcomed me onto a project that introduced me to the wizardry of graphene experiments and significantly broadened my research directions. I have been extraordinarily fortunate to work with and learn from numerous collaborators. Roman Lutchyn has advised me on several projects, extensively improved my familiarity with field theory, and been a driving force behind my participation in Majorana-based research. Torsten Karzig has been an MVP coauthor, providing lively discussions and reinvigorating my interest in projects at their dullest moments. Dima Pikulin’s optimistic demeanor and grasp of mesoscopic physics, combined with Michael Beverland’s fault tolerance perspective led to a particularly enjoyable collaboration. My foray into fractional Chern insulator physics would not have been possible without Mike Zaletel’s expertise and enthusiasm; his mentorship let to a fascinating project with many interesting future directions. Discussions with Eric Spanton have sharpened my understanding of “experimental accessibility” and improved my intuition for a new system. Meng Cheng and Dong Liu were extremely helpful, and patient, collaborators on my first project. Kaushal Patel endured my frenzied calculations of anyonic entanglement entropies for years and was a calm check on my descent into diagrammatic madness. I continue to learn and benefit from working with Jukka Vayrynen and Dave Aasen. My graduate school experience has been shaped by the past and present Station Q com- munity. My unofficial office in the seminar room has led to many helpful and interesting discussions with Zhenghan Wang, Bela Bauer, Michael Freedman, Chao-Ming Jian, Maissam Barkeshli, David Clarke, Andrey Antipov, and Anna Keselman. I am particularly grateful for Jen Cano’s mentorship, and to all the Q and UCSB graduate students for helpful discussions and a collaborative environment. Every day in Elings has been brightened by Sean Fraer’s friendly greeting and organizational mastery. Finally, I have been supported throughout the last six years and my entire life by an amazing network of friends and family. Their love, encouragement, and much-needed distractions have made me a healthier, happier, and better person. v Curriculum Vitæ Christina Paulsen Knapp Education 2019 Ph.D. in Physics (expected), University of California, Santa Barbara Advisor: Chetan Nayak 2016 M.A. in Physics, University of California, Santa Barbara Advisor: Chetan Nayak 2013 B.A. in Physics (highest honors) & Math, Williams College, Williamstown, MA Advisor: William K. Wootters Awards 2016-2018 NSF Graduate Research Fellow 2016-2019 Outstanding Service to the Department, UCSB Physics 2014 Oustanding Teaching Assistant, UCSB Physics 2013 Ferrando-Fithian Award, UCSB Physics 2013 Phi Beta Kappa and Sigma Xi Honor Societies Publications “Fractional Chern insulator edge states and layer-resolved lattice contacts,” Christina Knapp, Eric M. Spanton, Andrea F. Young, Chetan Nayak, and Michael P. Zaletel. Physical Review B 99, 081114 (2019), arXiv:1810.02325. “Modeling noise and error correction for Majorana-based quantum comput- ing,” Christina Knapp, Michael Beverland, Dmitry I. Pikulin, and Torsten Karzig. Quantum 2, 88 (2018), arXiv:1806.01275. “Dephasing of Majorana-based qubits,” Christina Knapp, Torsten Karzig, Roman Lutchyn, and Chetan Nayak. Physical Review B 97, 125404 (2018), arXiv:1711.03968. vi “Anyonic Entanglement and Topological Entanglement Entropy,” Parsa Bon- derson, Christina Knapp, and Kaushal Patel. Annals of Physics 385 (2017), arXiv:1706.09420. “Scalable Designs for Quasiparticle-Poisoning-Protected Topological Quan- tum Computation with Majorana Zero Modes,” Torsten Karzig, Christina Knapp, Roman Lutchyn, Parsa Bonderson, Matthew Hastings, Chetan Nayak, Jason Alicea, Karsten Flensberg, Stephan Plugge, Yuval Oreg, Charles Mar- cus, and Michael Freedman. Physical Review B 95, 235305 (2017), arXiv:1610.05289. “Nature and Correction of Diabatic Errors in Anyon Braiding,” Christina Knapp, Michael P. Zaletel, Dong E. Liu, Meng Cheng, Parsa Bonderson, and Chetan Nayak. Physical Review X 6, 041003 (2016), arXiv:1601.05790. vii Abstract Topological Quantum Computing with Majorana Zero Modes and Beyond by Christina Paulsen Knapp Topological quantum computing seeks to store and manipulate information in a protected manner using topological phases of matter. Information encoded in the degenerate state space of pairs of non-Abelian anyons or defects is robust to local perturbations, reducing its sus- ceptiblity to environmental errors and potentially providing a scalable approach to quantum computing. However, topological quantum computing faces significant challenges, not least of which is identifying an experimentally accessible platform supporting non-Abelian topologi- cal physics. In this thesis, we critically analyze topological quantum computing with Majorana zero modes, non-Abelian defects of a topological superconductor. We identify intrinsic er- ror sources for Majorana-based systems and propose quantum computing architectures that minimize their effects. Additionally, we consider a new approach for realizing and detecting non-Abelian topological defects in fractional Chern insulators. Topological quantum computing is predicated on the idea that braiding non-Abelian anyons adiabatically can implement quantum gates fault tolerantly. However, any braiding experiment will necessarily depart from the strict adiabatic limit. We begin by analyzing the nature of diabatic errors for anyon braiding, paying particular attention to how such errors scale with viii braiding time. We find that diabatic errors are unfavorably large and worryingly sensitive to details of the time evolution. We present a measurement-based correction protocol for such errors, and illustrate its application in a particular Majorana-based qubit design. We next propose designs for Majorana-based qubits operated entirely by a measurement- based protocol, thereby avoiding the diabatic errors discussed above. Our designs can be scaled into large two dimensional arrays amenable to long-term quantum computing goals, whose core components are testable in near-term devices. These qubits are robust to quasiparticle poison- ing, anticipated to be one of the dominant error sources coupling to Majorana zero modes. We demonstrate that our designs support topologically protected Clifford operations and can be augmented to a universal gate set without requiring additional control parameters. While topological protection greatly suppresses errors, residual coupling to noise limits the lifetimes of our proposed Majorana-based qubits. We analyze the dephasing times for our quasiparticle-poisoning-protected qubits by calculating their charge distribution using a particle number-conserving formalism. We find that fluctuations in the electromagnetic en- vironment couple to an exponentially suppressed topological dipole moment. We estimate dephasing times due to 1=f noise, thermal quasiparticle excitations, and phonons for different qubit sizes. The residual errors discussed above will necessarily require error correction for a suffi- ciently long quantum computation. We develop physically
Recommended publications
  • Arxiv:2007.11161V3 [Cond-Mat.Str-El] 13 Mar 2021
    Topological phase transition and single/multi anyon dynamics of /2 spin liquid Zheng Yan,1 Yan-Cheng Wang,2 Nvsen Ma,3 Yang Qi,4, 5, 6, ∗ and Zi Yang Meng1, y 1Department of Physics and HKU-UCAS Joint Institute of Theoretical and Computational Physics, The University of Hong Kong, Pokfulam Road, Hong Kong 2School of Materials Science and Physics, China University of Mining and Technology, Xuzhou 221116, China 3School of Physics, Key Laboratory of Micro-Nano Measurement-Manipulation and Physics, Beihang University, Beijing 100191, China 4State Key Laboratory of Surface Physics, Fudan University, Shanghai 200433, China 5Center for Field Theory and Particle Physics, Department of Physics, Fudan University, Shanghai 200433, China 6Collaborative Innovation Center of Advanced Microstructures, Nanjing 210093, China Among the quantum many-body models that host anyon excitation and topological orders, quantum dimer models (QDM) provide a unique playground for studying the relation between single-anyon and multi-anyon continuum spectra. However, as the prototypical correlated system with local constraints, the generic solution of QDM at different lattice geometry and parameter regimes is still missing due to the lack of controlled methodologies. Here we obtain, via the newly developed sweeping cluster quantum Monte Carlo algorithm, the excitation spectra in different phases of the triangular lattice QDM. Our resultsp revealp the single vison excitations inside the /2 quantum spin liquid (QSL) and its condensation towards the 12 × 12 valence bond solid (VBS), and demonstrate the translational symmetry fractionalization and emergent O(4) symmetry at the QSL-VBS transition. We find the single vison excitations, whose convolution qualitatively reproduces the dimer spectra, are not free but subject to interaction effects throughout the transition.
    [Show full text]
  • Superselection Sectors in Quantum Spin Systems∗
    Superselection sectors in quantum spin systems∗ Pieter Naaijkens Leibniz Universit¨atHannover June 19, 2014 Abstract In certain quantum mechanical systems one can build superpositions of states whose relative phase is not observable. This is related to super- selection sectors: the algebra of observables in such a situation acts as a direct sum of irreducible representations on a Hilbert space. Physically, this implies that there are certain global quantities that one cannot change with local operations, for example the total charge of the system. Here I will discuss how superselection sectors arise in quantum spin systems, and how one can deal with them mathematically. As an example we apply some of these ideas to Kitaev's toric code model, to show how the analysis of the superselection sectors can be used to get a complete un- derstanding of the "excitations" or "charges" in this model. In particular one can show that these excitations are so-called anyons. These notes introduce the concept of superselection sectors of quantum spin systems, and discuss an application to the analysis of charges in Kitaev's toric code. The aim is to communicate the main ideas behind these topics: most proofs will be omitted or only sketched. The interested reader can find the technical details in the references. A basic knowledge of the mathematical theory of quantum spin systems is assumed, such as given in the lectures by Bruno Nachtergaele during this conference. Other references are, among others, [3, 4, 15, 12]. Parts of these lecture notes are largely taken from [12]. 1 Superselection sectors We will say that two representations π and ρ of a C∗-algebra are unitary equiv- alent (or simply equivalent) if there is a unitary operator U : Hπ !Hρ between the corresponding Hilbert spaces and in addition we have that Uπ(A)U ∗ = ρ(A) ∼ ∗ for all A 2 A.
    [Show full text]
  • The Conventionality of Parastatistics
    The Conventionality of Parastatistics David John Baker Hans Halvorson Noel Swanson∗ March 6, 2014 Abstract Nature seems to be such that we can describe it accurately with quantum theories of bosons and fermions alone, without resort to parastatistics. This has been seen as a deep mystery: paraparticles make perfect physical sense, so why don't we see them in nature? We consider one potential answer: every paraparticle theory is physically equivalent to some theory of bosons or fermions, making the absence of paraparticles in our theories a matter of convention rather than a mysterious empirical discovery. We argue that this equivalence thesis holds in all physically admissible quantum field theories falling under the domain of the rigorous Doplicher-Haag-Roberts approach to superselection rules. Inadmissible parastatistical theories are ruled out by a locality- inspired principle we call Charge Recombination. Contents 1 Introduction 2 2 Paraparticles in Quantum Theory 6 ∗This work is fully collaborative. Authors are listed in alphabetical order. 1 3 Theoretical Equivalence 11 3.1 Field systems in AQFT . 13 3.2 Equivalence of field systems . 17 4 A Brief History of the Equivalence Thesis 20 4.1 The Green Decomposition . 20 4.2 Klein Transformations . 21 4.3 The Argument of Dr¨uhl,Haag, and Roberts . 24 4.4 The Doplicher-Roberts Reconstruction Theorem . 26 5 Sharpening the Thesis 29 6 Discussion 36 6.1 Interpretations of QM . 44 6.2 Structuralism and Haecceities . 46 6.3 Paraquark Theories . 48 1 Introduction Our most fundamental theories of matter provide a highly accurate description of subatomic particles and their behavior.
    [Show full text]
  • Superselection Structure at Small Scales in Algebraic Quantum Field Theory
    UNIVERSITÀ DEGLI STUDI DI ROMA “LA SAPIENZA” FACOLTÀ DI SCIENZE MATEMATICHE, FISICHE E NATURALI Superselection Structure at Small Scales in Algebraic Quantum Field Theory Gerardo Morsella PH.D. IN MATHEMATICS DOTTORATO DI RICERCA IN MATEMATICA XIV Ciclo – AA. AA. 1998-2002 Supervisor: Ph.D. Coordinator: Prof. Sergio Doplicher Prof. Alessandro Silva Contents Introduction 1 1 Superselection sectors and the reconstruction of fields 5 1.1 Basic assumptions of algebraic quantum field theory . 6 1.2 Superselection theory . 10 1.2.1 Localizable sectors . 11 1.2.2 Topological sectors . 13 1.3 Reconstruction of fields and gauge group . 14 2 Scaling algebras and ultraviolet limit 17 2.1 Scaling algebras as an algebraic version of the renormalization group . 17 2.2 Construction of the scaling limit . 21 2.3 Examples of scaling limit calculation . 24 3 Ultraviolet stability and scaling limit of charges 27 3.1 Scaling limit for field nets . 28 3.2 Ultraviolet stable localizable charges . 36 3.3 Ultraviolet stable topological charges . 43 Conclusions and outlook 55 A Some geometrical results about spacelike cones 57 B An example of ultraviolet stable charge 63 Bibliography 73 i Introduction The phenomenology of elementary particle physics is described on the theoretical side, to a high degree of accuracy, by the perturbative treatment of relativistic quantum field theories. On the mathematical and conceptual side, however, the understanding of these theories is far from being satisfactory, as illustrated, for instance, by the well known difficulties in the very problem of providing them with a mathematically sound definition in d 4 spacetime dimensions.
    [Show full text]
  • Observing Spinons and Holons in 1D Antiferromagnets Using Resonant
    Summary on “Observing spinons and holons in 1D antiferromagnets using resonant inelastic x-ray scattering.” Umesh Kumar1,2 1 Department of Physics and Astronomy, The University of Tennessee, Knoxville, TN 37996, USA 2 Joint Institute for Advanced Materials, The University of Tennessee, Knoxville, TN 37996, USA (Dated Jan 30, 2018) We propose a method to observe spinon and anti-holon excitations at the oxygen K-edge of Sr2CuO3 using resonant inelastic x-ray scattering (RIXS). The evaluated RIXS spectra are rich, containing distinct two- and four-spinon excitations, dispersive antiholon excitations, and combinations thereof. Our results further highlight how RIXS complements inelastic neutron scattering experiments by accessing charge and spin components of fractionalized quasiparticles Introduction:- One-dimensional (1D) magnetic systems are an important playground to study the effects of quasiparticle fractionalization [1], defined below. Hamiltonians of 1D models can be solved with high accuracy using analytical and numerical techniques, which is a good starting point to study strongly correlated systems. The fractionalization in 1D is an exotic phenomenon, in which electronic quasiparticle excitation breaks into charge (“(anti)holon”), spin (“spinon”) and orbit (“orbiton”) degree of freedom, and are observed at different characteristic energy scales. Spin-charge and spin-orbit separation have been observed using angle-resolved photoemission spectroscopy (ARPES) [2] and resonant inelastic x-ray spectroscopy (RIXS) [1], respectively. RIXS is a spectroscopy technique that couples to spin, orbit and charge degree of freedom of the materials under study. Unlike spin-orbit, spin-charge separation has not been observed using RIXS to date. In our work, we propose a RIXS experiment that can observe spin-charge separation at the oxygen K-edge of doped Sr2CuO3, a prototype 1D material.
    [Show full text]
  • Topological Quantum Compiling Layla Hormozi
    Florida State University Libraries Electronic Theses, Treatises and Dissertations The Graduate School 2007 Topological Quantum Compiling Layla Hormozi Follow this and additional works at the FSU Digital Library. For more information, please contact [email protected] THE FLORIDA STATE UNIVERSITY COLLEGE OF ARTS AND SCIENCES TOPOLOGICAL QUANTUM COMPILING By LAYLA HORMOZI A Dissertation submitted to the Department of Physics in partial fulfillment of the requirements for the degree of Doctor of Philosophy Degree Awarded: Fall Semester, 2007 The members of the Committee approve the Dissertation of Layla Hormozi defended on September 20, 2007. Nicholas E. Bonesteel Professor Directing Dissertation Philip L. Bowers Outside Committee Member Jorge Piekarewicz Committee Member Peng Xiong Committee Member Kun Yang Committee Member Approved: Mark A. Riley , Chair Department of Physics Joseph Travis , Dean, College of Arts and Sciences The Office of Graduate Studies has verified and approved the above named committee members. ii ACKNOWLEDGEMENTS To my advisor, Nick Bonesteel, I am indebted at many levels. I should first thank him for introducing me to the idea of topological quantum computing, for providing me with the opportunity to work on the problems that are addressed in this thesis, and for spending an infinite amount of time helping me toddle along, every step of the process, from the very beginning up until the completion of this thesis. I should also thank him for his uniquely caring attitude, for his generous support throughout the years, and for his patience and understanding for an often-recalcitrant graduate student. Thank you Nick — I truly appreciate all that you have done for me.
    [Show full text]
  • Physics of Resonating Valence Bond Spin Liquids Julia Saskia Wildeboer Washington University in St
    Washington University in St. Louis Washington University Open Scholarship All Theses and Dissertations (ETDs) Summer 8-13-2013 Physics of Resonating Valence Bond Spin Liquids Julia Saskia Wildeboer Washington University in St. Louis Follow this and additional works at: https://openscholarship.wustl.edu/etd Recommended Citation Wildeboer, Julia Saskia, "Physics of Resonating Valence Bond Spin Liquids" (2013). All Theses and Dissertations (ETDs). 1163. https://openscholarship.wustl.edu/etd/1163 This Dissertation is brought to you for free and open access by Washington University Open Scholarship. It has been accepted for inclusion in All Theses and Dissertations (ETDs) by an authorized administrator of Washington University Open Scholarship. For more information, please contact [email protected]. WASHINGTON UNIVERSITY IN ST. LOUIS Department of Physics Dissertation Examination Committee: Alexander Seidel, Chair Zohar Nussinov Michael C. Ogilvie Jung-Tsung Shen Xiang Tang Li Yang Physics of Resonating Valence Bond Spin Liquids by Julia Saskia Wildeboer A dissertation presented to the Graduate School of Arts and Sciences of Washington University in partial fulfillment of the requirements for the degree of Doctor of Philosophy August 2013 St. Louis, Missouri TABLE OF CONTENTS Page LIST OF FIGURES ................................ v ACKNOWLEDGMENTS ............................. ix DEDICATION ................................... ix ABSTRACT .................................... xi 1 Introduction .................................. 1 1.1 Landau’s principle of symmetry breaking and topological order .... 2 1.2 From quantum dimer models to spin models .............. 5 1.2.1 The Rokhsar-Kivelson (RK) point ................ 12 1.3 QDM phase diagrams ........................... 14 1.4 Z2 quantum spin liquid and other topological phases .......... 15 1.4.1 Z2 RVB liquid ........................... 16 1.4.2 U(1) critical RVB liquid ....................
    [Show full text]
  • Charge and Spin Fractionalization in Strongly Correlated Topological Insulators
    Charge and spin fractionalization in strongly correlated topological insulators Predrag Nikolić George Mason University October 26, 2011 Acknowledgments Zlatko Tešanović Michael Levin Tanja Duric IQM @ Johns Hopkins University of Maryland Max Planck Institute, Dresden • Affiliations and sponsors The Center for Quantum Science Charge and spin fractionalization in strongly correlated topological insulators 2/33 Overview • TIs with time-reversal symmetry – Introduction to topological band-insulators – Introduction to interacting TIs • Experimental realization of strongly correlated TIs – Cooper pair TI by proximity effect – Exciton TI • Theory of strongly correlated TIs – Topological Landau-Ginzburg theory – Charge and spin fractionalization Charge and spin fractionalization in strongly correlated topological insulators 3/33 Topological vs. Conventional • Conventional states of matter – Characterized by local properties (LDOS, order parameter...) • Topological states of matter – Characterized by non-local properties (entanglement, edge modes, torus spectra...) • Examples of topological quantum states – Quantum Hall states & “topological insulators” – Spin liquids, string-net condensates... Charge and spin fractionalization in strongly correlated topological insulators 4/33 The Appeal of Topological • Macroscopic quantum entanglement – What makes quantum mechanics fascinating... – Still uncharted class of quantum states • Non-local properties are hard to perturb – Standard for measurements of resistivity – Topological quantum computation •
    [Show full text]
  • Quantum Computing Methods for Supervised Learning Arxiv
    Quantum Computing Methods for Supervised Learning Viraj Kulkarni1, Milind Kulkarni1, Aniruddha Pant2 1 Vishwakarma University 2 DeepTek Inc June 23, 2020 Abstract The last two decades have seen an explosive growth in the theory and practice of both quantum computing and machine learning. Modern machine learning systems process huge volumes of data and demand massive computational power. As silicon semiconductor miniaturization approaches its physics limits, quantum computing is increasingly being considered to cater to these computational needs in the future. Small-scale quantum computers and quantum annealers have been built and are already being sold commercially. Quantum computers can benefit machine learning research and application across all science and engineering domains. However, owing to its roots in quantum mechanics, research in this field has so far been confined within the purview of the physics community, and most work is not easily accessible to researchers from other disciplines. In this paper, we provide a background and summarize key results of quantum computing before exploring its application to supervised machine learning problems. By eschewing results from physics that have little bearing on quantum computation, we hope to make this introduction accessible to data scientists, machine learning practitioners, and researchers from across disciplines. 1 Introduction Supervised learning is the most commonly applied form of machine learning. It works in two arXiv:2006.12025v1 [quant-ph] 22 Jun 2020 stages. During the training stage, the algorithm extracts patterns from the training dataset that contains pairs of samples and labels and converts these patterns into a mathematical representation called a model. During the inference stage, this model is used to make predictions about unseen samples.
    [Show full text]
  • Spin Liquids with Topological Order
    Spin Liquids with Topological Order 2d Mott Insulators with one electron per unit cell Quantum s=1/2 magnets Will show that topologically ordered spin liquids have: • an emergent “gauge structure” • Quantum number fractionalization • Ground state degeneracy on a torus Focus on Spin liquids with: • Z2 Topological order • Fully gapped with bosonic “spinons” and “visons” • 2d square lattice and Kagome lattice Resonating Valence Bond “Picture” 2d square lattice s=1/2 AFM = Singlet or a Valence Bond - Gains exchange energy J Valence Bond Solid Plaquette Resonance Resonating Valence Bond “Spin liquid” Plaquette Resonance Resonating Valence Bond “Spin liquid” Plaquette Resonance Resonating Valence Bond “Spin liquid” Gapped Spin Excitations “Break” a Valence Bond - costs energy of order J Create s=1 excitation Try to separate two s=1/2 “spinons” Valence Bond Solid Energy cost is linear in separation Spinons are “Confined” in VBS RVB State: Exhibits Fractionalization! Energy cost stays finite when spinons are separated Spinons are “deconfined” in the RVB state Spinon carries the electrons spin, but not its charge ! The electron is “fractionalized”. Gauge Theory Formulation of RVB Spin liquid Focus on the Valence bonds and their quantum dynamics - “A Quantum Dimer model” Place a “spin” on each link i j of the lattice vector of Pauli matrices no bond on link ij Define: Plaquette “Flux” bond on link ij 1 -1 -1 1 Hamiltonian: Need a Constraint: One valence bond coming out of each site Z2 Gauge Theory: Qi = -1 implies one or three bonds out of each
    [Show full text]
  • Identity, Superselection Theory and the Statistical Properties of Quantum Fields
    Identity, Superselection Theory and the Statistical Properties of Quantum Fields David John Baker Department of Philosophy, University of Michigan [email protected] October 9, 2012 Abstract The permutation symmetry of quantum mechanics is widely thought to imply a sort of metaphysical underdetermination about the identity of particles. Despite claims to the contrary, this implication does not hold in the more fundamental quantum field theory, where an ontology of particles is not generally available. Although permuta- tions are often defined as acting on particles, a more general account of permutation symmetry can be formulated using superselection theory. As a result, permutation symmetry applies even in field theories with no particle interpretation. The quantum mechanical account of permutations acting on particles is recovered as a special case. 1 Introduction The permutation symmetry of quantum theory has inspired a long debate about the meta- physics of identity and such related principles as haecceitism and the identity of indis- cernibles. Since permutations are normally defined as acting on particles, this debate has largely proceeded by interpreting quantum physics as a theory of particles. As a result, there is presently no clear connection between this work and the latest foundational studies of quantum field theory (QFT), many of which have argued against particle ontologies. It is not quite right to say that the debate concerning the metaphysics of statistics has ignored QFT. Rather, parties to this debate have engaged with QFT in a set of idealized special cases: Fock space QFTs on Minkowski spacetime, which can be treated as particle 1 theories (albeit with the number of particles sometimes indeterminate).
    [Show full text]
  • Topological Quantum Computation Zhenghan Wang
    Topological Quantum Computation Zhenghan Wang Microsoft Research Station Q, CNSI Bldg Rm 2237, University of California, Santa Barbara, CA 93106-6105, U.S.A. E-mail address: [email protected] 2010 Mathematics Subject Classification. Primary 57-02, 18-02; Secondary 68-02, 81-02 Key words and phrases. Temperley-Lieb category, Jones polynomial, quantum circuit model, modular tensor category, topological quantum field theory, fractional quantum Hall effect, anyonic system, topological phases of matter To my parents, who gave me life. To my teachers, who changed my life. To my family and Station Q, where I belong. Contents Preface xi Acknowledgments xv Chapter 1. Temperley-Lieb-Jones Theories 1 1.1. Generic Temperley-Lieb-Jones algebroids 1 1.2. Jones algebroids 13 1.3. Yang-Lee theory 16 1.4. Unitarity 17 1.5. Ising and Fibonacci theory 19 1.6. Yamada and chromatic polynomials 22 1.7. Yang-Baxter equation 22 Chapter 2. Quantum Circuit Model 25 2.1. Quantum framework 26 2.2. Qubits 27 2.3. n-qubits and computing problems 29 2.4. Universal gate set 29 2.5. Quantum circuit model 31 2.6. Simulating quantum physics 32 Chapter 3. Approximation of the Jones Polynomial 35 3.1. Jones evaluation as a computing problem 35 3.2. FP#P-completeness of Jones evaluation 36 3.3. Quantum approximation 37 3.4. Distribution of Jones evaluations 39 Chapter 4. Ribbon Fusion Categories 41 4.1. Fusion rules and fusion categories 41 4.2. Graphical calculus of RFCs 44 4.3. Unitary fusion categories 48 4.4. Link and 3-manifold invariants 49 4.5.
    [Show full text]