Complexity Error Correction
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Simulating Quantum Field Theory with a Quantum Computer
Simulating quantum field theory with a quantum computer John Preskill Lattice 2018 28 July 2018 This talk has two parts (1) Near-term prospects for quantum computing. (2) Opportunities in quantum simulation of quantum field theory. Exascale digital computers will advance our knowledge of QCD, but some challenges will remain, especially concerning real-time evolution and properties of nuclear matter and quark-gluon plasma at nonzero temperature and chemical potential. Digital computers may never be able to address these (and other) problems; quantum computers will solve them eventually, though I’m not sure when. The physics payoff may still be far away, but today’s research can hasten the arrival of a new era in which quantum simulation fuels progress in fundamental physics. Frontiers of Physics short distance long distance complexity Higgs boson Large scale structure “More is different” Neutrino masses Cosmic microwave Many-body entanglement background Supersymmetry Phases of quantum Dark matter matter Quantum gravity Dark energy Quantum computing String theory Gravitational waves Quantum spacetime particle collision molecular chemistry entangled electrons A quantum computer can simulate efficiently any physical process that occurs in Nature. (Maybe. We don’t actually know for sure.) superconductor black hole early universe Two fundamental ideas (1) Quantum complexity Why we think quantum computing is powerful. (2) Quantum error correction Why we think quantum computing is scalable. A complete description of a typical quantum state of just 300 qubits requires more bits than the number of atoms in the visible universe. Why we think quantum computing is powerful We know examples of problems that can be solved efficiently by a quantum computer, where we believe the problems are hard for classical computers. -
The Complexity Zoo
The Complexity Zoo Scott Aaronson www.ScottAaronson.com LATEX Translation by Chris Bourke [email protected] 417 classes and counting 1 Contents 1 About This Document 3 2 Introductory Essay 4 2.1 Recommended Further Reading ......................... 4 2.2 Other Theory Compendia ............................ 5 2.3 Errors? ....................................... 5 3 Pronunciation Guide 6 4 Complexity Classes 10 5 Special Zoo Exhibit: Classes of Quantum States and Probability Distribu- tions 110 6 Acknowledgements 116 7 Bibliography 117 2 1 About This Document What is this? Well its a PDF version of the website www.ComplexityZoo.com typeset in LATEX using the complexity package. Well, what’s that? The original Complexity Zoo is a website created by Scott Aaronson which contains a (more or less) comprehensive list of Complexity Classes studied in the area of theoretical computer science known as Computa- tional Complexity. I took on the (mostly painless, thank god for regular expressions) task of translating the Zoo’s HTML code to LATEX for two reasons. First, as a regular Zoo patron, I thought, “what better way to honor such an endeavor than to spruce up the cages a bit and typeset them all in beautiful LATEX.” Second, I thought it would be a perfect project to develop complexity, a LATEX pack- age I’ve created that defines commands to typeset (almost) all of the complexity classes you’ll find here (along with some handy options that allow you to conveniently change the fonts with a single option parameters). To get the package, visit my own home page at http://www.cse.unl.edu/~cbourke/. -
Arxiv:1506.08857V1 [Quant-Ph] 29 Jun 2015
Absolutely Maximally Entangled states, combinatorial designs and multi-unitary matrices Dardo Goyeneche National Quantum Information Center of Gda´nsk,81-824 Sopot, Poland and Faculty of Applied Physics and Mathematics, Technical University of Gda´nsk,80-233 Gda´nsk,Poland Daniel Alsina Dept. Estructura i Constituents de la Mat`eria,Universitat de Barcelona, Spain. Jos´e I. Latorre Dept. Estructura i Constituents de la Mat`eria,Universitat de Barcelona, Spain. and Center for Theoretical Physics, MIT, USA Arnau Riera ICFO-Institut de Ciencies Fotoniques, Castelldefels (Barcelona), Spain Karol Zyczkowski_ Institute of Physics, Jagiellonian University, Krak´ow,Poland and Center for Theoretical Physics, Polish Academy of Sciences, Warsaw, Poland (Dated: June 29, 2015) Absolutely Maximally Entangled (AME) states are those multipartite quantum states that carry absolute maximum entanglement in all possible partitions. AME states are known to play a relevant role in multipartite teleportation, in quantum secret sharing and they provide the basis novel tensor networks related to holography. We present alternative constructions of AME states and show their link with combinatorial designs. We also analyze a key property of AME, namely their relation to tensors that can be understood as unitary transformations in every of its bi-partitions. We call this property multi-unitarity. I. INTRODUCTION entropy S(ρ) = −Tr(ρ log ρ) ; (1) A complete characterization, classification and it is possible to show [1, 2] that the average entropy quantification of entanglement for quantum states re- of the reduced state σ = TrN=2j ih j to N=2 qubits mains an unfinished long-term goal in Quantum Infor- reads: N mation theory. -
Non-Unitary Quantum Computation in the Ground Space of Local Hamiltonians
Non-Unitary Quantum Computation in the Ground Space of Local Hamiltonians Na¨ıri Usher,1, ∗ Matty J. Hoban,2, 3 and Dan E. Browne1 1Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, United Kingdom. 2University of Oxford, Department of Computer Science, Wolfson Building, Parks Road, Oxford OX1 3QD, United Kingdom. 3School of Informatics, University of Edinburgh, 10 Crichton Street, Edinburgh EH8 9AB, UK A central result in the study of Quantum Hamiltonian Complexity is that the k-local hamilto- nian problem is QMA-complete [1]. In that problem, we must decide if the lowest eigenvalue of a Hamiltonian is bounded below some value, or above another, promised one of these is true. Given the ground state of the Hamiltonian, a quantum computer can determine this question, even if the ground state itself may not be efficiently quantum preparable. Kitaev's proof of QMA-completeness encodes a unitary quantum circuit in QMA into the ground space of a Hamiltonian. However, we now have quantum computing models based on measurement instead of unitary evolution, further- more we can use post-selected measurement as an additional computational tool. In this work, we generalise Kitaev's construction to allow for non-unitary evolution including post-selection. Fur- thermore, we consider a type of post-selection under which the construction is consistent, which we call tame post-selection. We consider the computational complexity consequences of this construc- tion and then consider how the probability of an event upon which we are post-selecting affects the gap between the ground state energy and the energy of the first excited state of its corresponding Hamiltonian. -
CS286.2 Lectures 5-6: Introduction to Hamiltonian Complexity, QMA-Completeness of the Local Hamiltonian Problem
CS286.2 Lectures 5-6: Introduction to Hamiltonian Complexity, QMA-completeness of the Local Hamiltonian problem Scribe: Jenish C. Mehta The Complexity Class BQP The complexity class BQP is the quantum analog of the class BPP. It consists of all languages that can be decided in quantum polynomial time. More formally, Definition 1. A language L 2 BQP if there exists a classical polynomial time algorithm A that ∗ maps inputs x 2 f0, 1g to quantum circuits Cx on n = poly(jxj) qubits, where the circuit is considered a sequence of unitary operators each on 2 qubits, i.e Cx = UTUT−1...U1 where each 2 2 Ui 2 L C ⊗ C , such that: 2 i. Completeness: x 2 L ) Pr(Cx accepts j0ni) ≥ 3 1 ii. Soundness: x 62 L ) Pr(Cx accepts j0ni) ≤ 3 We say that the circuit “Cx accepts jyi” if the first output qubit measured in Cxjyi is 0. More j0i specifically, letting P1 = j0ih0j1 be the projection of the first qubit on state j0i, j0i 2 Pr(Cx accepts jyi) =k (P1 ⊗ In−1)Cxjyi k2 The Complexity Class QMA The complexity class QMA (or BQNP, as Kitaev originally named it) is the quantum analog of the class NP. More formally, Definition 2. A language L 2 QMA if there exists a classical polynomial time algorithm A that ∗ maps inputs x 2 f0, 1g to quantum circuits Cx on n + q = poly(jxj) qubits, such that: 2q i. Completeness: x 2 L ) 9jyi 2 C , kjyik2 = 1, such that Pr(Cx accepts j0ni ⊗ 2 jyi) ≥ 3 2q 1 ii. -
Restricted Versions of the Two-Local Hamiltonian Problem
The Pennsylvania State University The Graduate School Eberly College of Science RESTRICTED VERSIONS OF THE TWO-LOCAL HAMILTONIAN PROBLEM A Dissertation in Physics by Sandeep Narayanaswami c 2013 Sandeep Narayanaswami Submitted in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy August 2013 The dissertation of Sandeep Narayanaswami was reviewed and approved* by the following: Sean Hallgren Associate Professor of Computer Science and Engineering Dissertation Adviser, Co-Chair of Committee Nitin Samarth Professor of Physics Head of the Department of Physics Co-Chair of Committee David S Weiss Professor of Physics Jason Morton Assistant Professor of Mathematics *Signatures are on file in the Graduate School. Abstract The Hamiltonian of a physical system is its energy operator and determines its dynamics. Un- derstanding the properties of the ground state is crucial to understanding the system. The Local Hamiltonian problem, being an extension of the classical Satisfiability problem, is thus a very well-motivated and natural problem, from both physics and computer science perspectives. In this dissertation, we seek to understand special cases of the Local Hamiltonian problem in terms of algorithms and computational complexity. iii Contents List of Tables vii List of Tables vii Acknowledgments ix 1 Introduction 1 2 Background 6 2.1 Classical Complexity . .6 2.2 Quantum Computation . .9 2.3 Generalizations of SAT . 11 2.3.1 The Ising model . 13 2.3.2 QMA-complete Local Hamiltonians . 13 2.3.3 Projection Hamiltonians, or Quantum k-SAT . 14 2.3.4 Commuting Local Hamiltonians . 14 2.3.5 Other special cases . 15 2.3.6 Approximation Algorithms and Heuristics . -
Universal Control and Error Correction in Multi-Qubit Spin Registers in Diamond T
LETTERS PUBLISHED ONLINE: 2 FEBRUARY 2014 | DOI: 10.1038/NNANO.2014.2 Universal control and error correction in multi-qubit spin registers in diamond T. H. Taminiau 1,J.Cramer1,T.vanderSar1†,V.V.Dobrovitski2 and R. Hanson1* Quantum registers of nuclear spins coupled to electron spins of including one with an additional strongly coupled 13C spin (see individual solid-state defects are a promising platform for Supplementary Information). To demonstrate the generality of quantum information processing1–13. Pioneering experiments our approach to create multi-qubit registers, we realized the initia- selected defects with favourably located nuclear spins with par- lization, control and readout of three weakly coupled 13C spins for ticularly strong hyperfine couplings4–10. To progress towards each NV centre studied (see Supplementary Information). In the large-scale applications, larger and deterministically available following, we consider one of these NV centres in detail and use nuclear registers are highly desirable. Here, we realize univer- two of its weakly coupled 13C spins to form a three-qubit register sal control over multi-qubit spin registers by harnessing abun- for quantum error correction (Fig. 1a). dant weakly coupled nuclear spins. We use the electron spin of Our control method exploits the dependence of the nuclear spin a nitrogen–vacancy centre in diamond to selectively initialize, quantization axis on the electron spin state as a result of the aniso- control and read out carbon-13 spins in the surrounding spin tropic hyperfine interaction (see Methods for hyperfine par- bath and construct high-fidelity single- and two-qubit gates. ameters), so no radiofrequency driving of the nuclear spins is We exploit these new capabilities to implement a three-qubit required7,23–28. -
Unconditional Quantum Teleportation
R ESEARCH A RTICLES our experiment achieves Fexp 5 0.58 6 0.02 for the field emerging from Bob’s station, thus Unconditional Quantum demonstrating the nonclassical character of this experimental implementation. Teleportation To describe the infinite-dimensional states of optical fields, it is convenient to introduce a A. Furusawa, J. L. Sørensen, S. L. Braunstein, C. A. Fuchs, pair (x, p) of continuous variables of the electric H. J. Kimble,* E. S. Polzik field, called the quadrature-phase amplitudes (QAs), that are analogous to the canonically Quantum teleportation of optical coherent states was demonstrated experi- conjugate variables of position and momentum mentally using squeezed-state entanglement. The quantum nature of the of a massive particle (15). In terms of this achieved teleportation was verified by the experimentally determined fidelity analogy, the entangled beams shared by Alice Fexp 5 0.58 6 0.02, which describes the match between input and output states. and Bob have nonlocal correlations similar to A fidelity greater than 0.5 is not possible for coherent states without the use those first described by Einstein et al.(16). The of entanglement. This is the first realization of unconditional quantum tele- requisite EPR state is efficiently generated via portation where every state entering the device is actually teleported. the nonlinear optical process of parametric down-conversion previously demonstrated in Quantum teleportation is the disembodied subsystems of infinite-dimensional systems (17). The resulting state corresponds to a transport of an unknown quantum state from where the above advantages can be put to use. squeezed two-mode optical field. -
Quantum Error Modelling and Correction in Long Distance Teleportation Using Singlet States by Joe Aung
Quantum Error Modelling and Correction in Long Distance Teleportation using Singlet States by Joe Aung Submitted to the Department of Electrical Engineering and Computer Science in partial fulfillment of the requirements for the degree of Master of Science in Electrical Engineering and Computer Science at the MASSACHUSETTS INSTITUTE OF TECHNOLOGY May 2002 @ Massachusetts Institute of Technology 2002. All rights reserved. Author ................... " Department of Electrical Engineering and Computer Science May 21, 2002 72-1 14 Certified by.................. .V. ..... ..'P . .. ........ Jeffrey H. Shapiro Ju us . tn Professor of Electrical Engineering Director, Research Laboratory for Electronics Thesis Supervisor Accepted by................I................... ................... Arthur C. Smith Chairman, Department Committee on Graduate Students BARKER MASSACHUSE1TS INSTITUTE OF TECHNOLOGY JUL 3 1 2002 LIBRARIES 2 Quantum Error Modelling and Correction in Long Distance Teleportation using Singlet States by Joe Aung Submitted to the Department of Electrical Engineering and Computer Science on May 21, 2002, in partial fulfillment of the requirements for the degree of Master of Science in Electrical Engineering and Computer Science Abstract Under a multidisciplinary university research initiative (MURI) program, researchers at the Massachusetts Institute of Technology (MIT) and Northwestern University (NU) are devel- oping a long-distance, high-fidelity quantum teleportation system. This system uses a novel ultrabright source of entangled photon pairs and trapped-atom quantum memories. This thesis will investigate the potential teleportation errors involved in the MIT/NU system. A single-photon, Bell-diagonal error model is developed that allows us to restrict possible errors to just four distinct events. The effects of these errors on teleportation, as well as their probabilities of occurrence, are determined. -
6.845 Quantum Complexity Theory, Lecture 16
6.896 Quantum Complexity Theory Oct. 28, 2008 Lecture 16 Lecturer: Scott Aaronson 1 Recap Last time we introduced the complexity class QMA (quantum Merlin-Arthur), which is a quantum version for NP. In particular, we have seen Watrous’s Group Non-Membership (GNM) protocol which enables a quantum Merlin to prove to a quantum Arthur that some element x of a group G is not a member of H, a subgroup of G. Notice that this is a problem that people do not know how to solve in classical world. To understand the limit of QMA, we have proved that QMA ⊆ P P (and also QMA ⊆ P SP ACE). We have also talked about QMA-complete problems, which are the quantum version of NP complete problem. In particular we have introduced the Local Hamiltonians problem, which is the quantum version of the SAT problem. We also have a quantum version of the Cook-Levin theorem, due to Kitaev, saying that the Local Hamiltonians problem is QMA complete. We will prove Kitaev’s theorem in this lecture. 2 Local Hamiltonians is QMA-complete De¯nition 1 (Local Hamiltonians Problem) Given m measurements E1; : : : ; Em each of which acts on at most k (out of n) qubits where k is a constant, the Local Hamiltonians problem is to decide which of the following two statements is true, promised that one is true: Pm 1. 9 an n-qubit state j'i such that i=1 Pr[Ei accepts j'i] ¸ b; or Pm 2. 8 n-qubit state j'i, i=1 Pr[Ei accepts j'i] · a. -
Arxiv:Quant-Ph/0612113V1 14 Dec 2006 † ∗ Nalo Hs Rosi Euto Ewe Unu Icisadtim and Circuits Quantum C Between Reduction QMA a Is Is Hamiltonian Complete
A new construction for a QMA complete 3-local Hamiltonian. 1, , Daniel Nagaj ∗ and Shay Mozes † 1Center for Theoretical Physics, MIT, Cambridge, MA 02139 (Dated: December 12, 2006) We present a new way of encoding a quantum computation into a 3-local Hamiltonian. Our construction is novel in that it does not include any terms that induce legal-illegal clock transitions. Therefore, the weights of the terms in the Hamiltonian do not scale with the size of the problem as in previous constructions. This improves the construction by Kempe and Regev [2], who were the first to prove that 3-local Hamiltonian is complete for the complexity class QMA, the quantum analogue of NP. Quantum k-SAT, a restricted version of the local Hamiltonian problem using only projector terms, was introduced by Bravyi [1] as an analogue of the classical k-SAT problem. Bravyi proved that quantum 4-SAT is complete for the class QMA with one-sided error (QMA1) and that quantum 2-SAT is in P. We give an encoding of a quantum circuit into a quantum 4-SAT Hamiltonian using only 3-local terms. As an intermediate step to this 3-local construction, we show that quantum 3-SAT for particles with dimensions 3 × 2 × 2 (a qutrit and two qubits) is QMA1 complete. The complexity of quantum 3-SAT with qubits remains an open question. I. INTRODUCTION In recent years, quantum complexity classes have been defined and studied in an attempt to understand the capacity and limitations of quantum computers and quantum algorithms and their relation to classical complexity classes. -
Adiabatic Quantum Computation Is Equivalent To
SIAM REVIEW c 2008 Society for Industrial and Applied Mathematics Vol. 50, No. 4, pp. 755–787 Adiabatic Quantum Computation Is Equivalent to ∗ Standard Quantum Computation Dorit Aharonov† Wim van Dam‡ Julia Kempe§ Zeph Landau¶ Seth Lloyd Oded Regev§ Abstract. The model of adiabatic quantum computation is a relatively recent model of quantum com- putation that has attracted attention in the physics and computer science communities. We describe an efficient adiabatic simulation of any given quantum circuit. This implies that the adiabatic computation model and the standard circuit-based quantum compu- tation model are polynomially equivalent. Our result can be extended to the physically realistic setting of particles arranged on a two-dimensional grid with nearest neighbor inter- actions. The equivalence between the models allows one to state the main open problems in quantum computation using well-studied mathematical objects such as eigenvectors and spectral gaps of Hamiltonians. Key words. quantum computation,adiabatic computation,nearest neighbor interactions AMS subject classifications. 81P68,68Q05 DOI. 10.1137/080734479 1. Introduction. The model of quantum computation has been thoroughly in- vestigated in the last two decades and is by now a well-established one [47]. In this ∗ Published electronically November 5,2008. This paper originally appeared in SIAM Journal on Computing,Volume 37,Number 1,2007,pages 166–194. This work was performed by an em- ployee of the U.S. Government or under U.S. Government contract. The U.S. Government retains a nonexclusive,royalty-free license to publish or reproduce the published form of this contribution, or allow others to do so,for U.S.