Quantum Computing 8

Total Page:16

File Type:pdf, Size:1020Kb

Quantum Computing 8 QUANTUM COMPUTING 8. Jozef Gruska Faculty of Informatics Brno Czech Republik October 27, 2020 Quantum computing 8, 2020 8. QUANTUM FINITE AUTOMATA as models of small memory quantum processors Jozef Gruska October 27, 2020 1 Quantum computing 8, 2020 WHY to STUDY QUANTUM PROCESSORS WITH SMALL MEMORY? - I. There are three main reasons why it is of interest and importance to investigate models of quantum processors that use little of quantum resources. and importance. 1. Experiences with classical information processing strongly suggest that investigation of the models of processors with finite memory and working in real-time brings a huge variety of fundamental theoretical results for information processing and, at the same time, provides a variety of methods and tools to design such processors. 2. Two decades of the research in quantum information processing start to make clear that not very powerful, with hundreds of qubits, quantum processors, but processors using only little of quantum resources, are to be seen currently as the goal that could be both feasible and worth to make { because theoretical results have already demonstrated that they can, in some cases, bring significant increase of the information processing power. 3. Processors combining huge classical and small quantum resources should therefore be seen as the next goal in quantum information processing once the current concentration of the research on few qubits storage, few particles entanglement and few unitary operations circuits start to rich fully satisfactory outcomes. Jozef Gruska October 27, 2020 2 Quantum computing 8, 2020 MODELS OF QUANTUM AUTOMATA Models of quantum automata For most of the main classical models of automata there are also their quantum versions. For example for finite automata, Turing machines and quantum cellular automata (QCA). Models of quantum automata are used: • To get an insight into the power of different quantum computing models and modes, using language/automata theoretic methods. • To discover the simplest models of computation at which one can demonstrate large (or huge) difference in the power of quantum versus classical models. • To develop quantum automata (networks, algorithms) design methodologies. • To explore mutual relations between different quantum computation models and modes. • To discover, in a transparent and elegant form, limitations of quantum computations and communications. Jozef Gruska October 27, 2020 3 Quantum computing 8, 2020 WHY to STUDY QUANTUM PROCESSORS WITH SMALL MEMORY? - II. Using such models one can also get deeper insides about: • How much more power, concerning computation, can bring quantum (randomness) resources comparing with classical (randomness) resources? • How much more power can have computation in linear time comparing with with that in real time? • How much more power can bring computation with mixed states comparing that with pure states? • When and how much more power can bring addition of very little of quantum resources? Jozef Gruska October 27, 2020 4 Quantum computing 8, 2020 MAIN MODELS of CLASSICAL PROCESSORS Main classical models of processors are: • Finite automata (deterministic, non-deterministic, probabilistic, ultrametric,...., one-way, two-way,...; one-tape, multi-tape,....) • Turing machines (with one or more tapes, with one or more heads, with one or more dimensional tapes - deterministic, non-deterministic, probabilistic,...) - models of universal processors • Uniform classes of circuits - models of universal processors • Cellular automata (one-, two-, three- and more dimensional){ models of universal processors. Of importance, especially for an understanding of the power and development of methods (of programming) for very powerful real processors are also the following models: • RAM - Random access machines • PRAM - Parallel and shared memory random access machines Jozef Gruska October 27, 2020 5 Quantum computing 8, 2020 MAIN MODELS of QUANTUM AUTOMATA 1. QUANTUM FINITE AUTOMATA (QFA) QFA are considered to be the simplest model of quantum processors, with “finite” quantum memory, that models well the most basic mode of quantum computing | a quantum action is performed on each classical input. 2. QUANTUM (one-tape and many-tape) TURING MACHINES (QTM) QTM are used to explore, at the most general level of sequential computation, the potential and limitations of quantum computing. Using this model the main computational complexity classes are defined. QTM are a main quantum abstraction of human computational processes. 3. QUANTUM CELLULAR AUTOMATA (QCA) QCA are used to model and to explore, on every general and basic level of parallel computation, the potential and limitations of quantum computing. QCA are a very basic quantum abstraction of computation by nature. Main classical modes of computation: deterministic, nondeterministic and randomized. Jozef Gruska October 27, 2020 6 Quantum computing 8, 2020 BASIC MODELS of CLASSICAL FINITE AUTOMATA • Deterministic (one-way) finite automata. • Deterministic two-way finite automata. • Nondeterministic finite automata (one-way or two-way) • Probabilistic (randomized) versions of finite automata ab c x y z # ab c x y z $ σ q control 1FAq control 2FAq control (a) unit (b) unit (c) unit q q 0.5 0.5 q’ q’’ q’ q’’ NFA PFA 0.2 0.80.3 0.7 (d) q1q2 q 3 q 4 q1q2 q 3 q 4 (e) Figure 1: Models of finite automata Jozef Gruska October 27, 2020 7 Quantum computing 8, 2020 FROM MODELS of CLASSICAL AUTOMATA to MODELS of QUANTUM AUTOMATA For the most of the main classical models of automata there are also their quantum versions. Models of quantum automata are used: • To get a deeper insight into the power of different quantum computing models and modes, using language/automata theoretic methods. • To discover the simplest models of computation at which one can clearly demonstrate large (or huge) difference in the power of quantum versus classical models. • To develop quantum automata (networks, algorithms) design methodologies. • To explore mutual relations between different quantum computation models and modes. • To discover, in a transparent and elegant form, limitations of quantum computations and communications. Jozef Gruska October 27, 2020 8 Quantum computing 8, 2020 MAIN MODES of COMPUTATION of FINITE AUTOMATA Basic modes: Deterministic automata (DFA): In each step next configuration is uniquely (deterministically) determined. An input is accepted if it makes the automaton to reach an accepted state. Non-deterministic automata (NFA): In each step one of possible configurations is taken. An input is accepted if it can make the automaton to reach an accepted state. Probabilistic automata (PFA): In each step each possible configuration has a probability assigned. An input is accepted if it makes automaton to reach an accepting state with a certain probability - several modes of that are considered. Ultrametric automata (UFA): In each step each possible transition has a p-adic number assigned. Acceptance of an input is considered as in probabilistic case. Quantum automata (QFA): In each step each possible configuration has a complex number, probability amplitude, assigned and automaton can be at any step in a superposition of configurations. An input is accepted if it makes automaton to reach a configuration of accepting states with a certain probability. Jozef Gruska October 27, 2020 9 Quantum computing 8, 2020 MAIN PROPERTIES of CLASSICAL FINITE AUTOMATA • The concept of classical finite automata is very robust - all main variants of the basic model have the same recognition power. • Informally, classical finite automata can do exactly that what can be done in real-time - in time needed to read input - and with finite (input length independent) memory. • Formally, classical finite automata can recognize exactly the class of regular languages - the class of languages containing finite languages and closed under operations of union, concatenation and iteration. • For each regular language L there is a unique minimal finite deterministic automaton accepting L - minimization problem is therefore well defined. • There is an efficient algorithm to find the minimal deterministic finite automaton with. • All major decision problems for finite classical automata are decidable. • To study various classes of languages accepted by classical finite automata a variety of rich algebraic methods can be used to get deep insights. Jozef Gruska October 27, 2020 10 Quantum computing 8, 2020 MAIN PROBLEMS to EXPLORE for MODELS of QUANTUM FINITE AUTOMATA. • Recognition (processing) power of various models of quantum automata - properties and characterization of the classes of languages accepted by different models of quantum automata. • What kind of acceptance probabilities are achievable? • Succinctness relation to the corresponding models of quantum automata - how much smaller can quantum automata be for doing the same task as classical automata of the similar type. • Decidability of basic decision problems - for example of the equivalence problem. • Decidability of basic decision problems - for example of the equivalence problem. • Development and complexity study of methods to construct minimal quantum automata for the case of various models of quantum automata. Jozef Gruska October 27, 2020 11 Quantum computing 8, 2020 MAIN DIVISIONS of QUANTUM MODELS of FINITE AUTOMATA There are three main ways to divide models of quantum finite automata: 1. According to head moves and power: • all heads have always to read the same symbol and have always move in one direction • all heads can
Recommended publications
  • Quantum Computer: Quantum Model and Reality
    Quantum Computer: Quantum Model and Reality Vasil Penchev, [email protected] Bulgarian Academy of Sciences: Institute of Philosophy and Sociology: Dept. of Logical Systems and Models Abstract. Any computer can create a model of reality. The hypothesis that quantum computer can generate such a model designated as quantum, which coincides with the modeled reality, is discussed. Its reasons are the theorems about the absence of “hidden variables” in quantum mechanics. The quantum modeling requires the axiom of choice. The following conclusions are deduced from the hypothesis. A quantum model unlike a classical model can coincide with reality. Reality can be interpreted as a quantum computer. The physical processes represent computations of the quantum computer. Quantum information is the real fundament of the world. The conception of quantum computer unifies physics and mathematics and thus the material and the ideal world. Quantum computer is a non-Turing machine in principle. Any quantum computing can be interpreted as an infinite classical computational process of a Turing machine. Quantum computer introduces the notion of “actually infinite computational process”. The discussed hypothesis is consistent with all quantum mechanics. The conclusions address a form of neo-Pythagoreanism: Unifying the mathematical and physical, quantum computer is situated in an intermediate domain of their mutual transformations. Key words: model, quantum computer, reality, Turing machine Eight questions: There are a few most essential questions about the philosophical interpretation of quantum computer. They refer to the fundamental problems in ontology and epistemology rather than philosophy of science or that of information and computation only. The contemporary development of quantum mechanics and the theory of quantum information generate them.
    [Show full text]
  • Quantum Algorithms 1
    Quantum Algorithms 1 Computer scientists usually find conventional expositions of quantum computation difficult, since a lot of new concepts have to be learned to- gether to make sense of it all. In this course, we take a different approach, starting from a point where every computer science student is comfortable, and introducing the new concepts one by one into the familiar framework. We hope it will be much easier this way. So let's start with deterministic finite automata! Chapter 1 Finite automata 1.1 Deterministic model You already know the stuff in Sipser's book. Note that the transitions of a DFA can be represented as 0-1 matrices, the states can be traced with vectors, and the execution on an input string boils down to multiplying this vector with the corresponding sequence of those matrices. 1.2 Probabilistic model We define real-time1 probabilistic finite automata (rtPFAs) by generalizing the matrix definition of rtDFAs to column stochastic transition matrices. Consider a transition graph representation for a moment. It is as if compu- tation flows through many arrows (associated with the same input symbol) parallelly in each step. Under this \zero-error" regime (exact computation) rtPFAs are identical to rtDFAs: Since none of these computational paths can arrive at an incorrect response at the end, tracing any single path is suffi- cient for seeing what the machine will do. So we convert each rtPFA matrix (which have to contain at least one nonzero entry in each column) to a rtDFA matrix with a 1 in just the position corresponding to the topmost nonzero entry of the rtPFA in that column.
    [Show full text]
  • 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 .
    [Show full text]
  • STRONGLY UNIVERSAL QUANTUM TURING MACHINES and INVARIANCE of KOLMOGOROV COMPLEXITY (AUGUST 11, 2007) 2 Such That the Aforementioned Halting Conditions Are Satisfied
    STRONGLY UNIVERSAL QUANTUM TURING MACHINES AND INVARIANCE OF KOLMOGOROV COMPLEXITY (AUGUST 11, 2007) 1 Strongly Universal Quantum Turing Machines and Invariance of Kolmogorov Complexity Markus M¨uller Abstract—We show that there exists a universal quantum Tur- For a compact presentation of the results by Bernstein ing machine (UQTM) that can simulate every other QTM until and Vazirani, see the book by Gruska [4]. Additional rele- the other QTM has halted and then halt itself with probability one. vant literature includes Ozawa and Nishimura [5], who gave This extends work by Bernstein and Vazirani who have shown that there is a UQTM that can simulate every other QTM for necessary and sufficient conditions that a QTM’s transition an arbitrary, but preassigned number of time steps. function results in unitary time evolution. Benioff [6] has As a corollary to this result, we give a rigorous proof that worked out a slightly different definition which is based on quantum Kolmogorov complexity as defined by Berthiaume et a local Hamiltonian instead of a local transition amplitude. al. is invariant, i.e. depends on the choice of the UQTM only up to an additive constant. Our proof is based on a new mathematical framework for A. Quantum Turing Machines and their Halting Conditions QTMs, including a thorough analysis of their halting behaviour. Our discussion will rely on the definition by Bernstein and We introduce the notion of mutually orthogonal halting spaces and show that the information encoded in an input qubit string Vazirani. We describe their model in detail in Subsection II-B.
    [Show full text]
  • On the Simulation of Quantum Turing Machines
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Theoretical Computer Science 304 (2003) 103–128 www.elsevier.com/locate/tcs On the simulation ofquantum turing machines Marco Carpentieri Universita di Salerno, 84081 Baronissi (SA), Italy Received 20 March 2002; received in revised form 11 December 2002; accepted 12 December 2002 Communicated by G. Ausiello Abstract In this article we shall review several basic deÿnitions and results regarding quantum compu- tation. In particular, after deÿning Quantum Turing Machines and networks the paper contains an exposition on continued fractions and on errors in quantum networks. The topic of simulation ofQuantum Turing Machines by means ofobvious computation is introduced. We give a full discussion ofthe simulation ofmultitape Quantum Turing Machines in a slight generalization of the class introduced by Bernstein and Vazirani. As main result we show that the Fisher-Pippenger technique can be used to give an O(tlogt) simulation ofa multi-tape Quantum Turing Machine by another belonging to the extended Bernstein and Vazirani class. This result, even ifregarding a slightly restricted class ofQuantum Turing Machines improves the simulation results currently known in the literature. c 2003 Published by Elsevier B.V. 1. Introduction Even ifthe present technology does consent realizing only very simple devices based on the principles ofquantum mechanics, many authors considered to be worth it ask- ing whether a theoretical model ofquantum computation could o:er any substantial beneÿts over the correspondent theoretical model based on the assumptions ofclas- sical physics. Recently, this question has received considerable attention because of the growing beliefthat quantum mechanical processes might be able to performcom- putation that traditional computing machines can only perform ine;ciently.
    [Show full text]
  • A Quantum Computer Foundation for the Standard Model and Superstring Theories*
    A Quantum Computer Foundation for the Standard Model and SuperString Theories* By Stephen Blaha** * Excerpted from the book Cosmos and Consciousness by Stephen Blaha (1stBooks Library, Bloomington, IN, 2000) available from amazon.com and bn.com. ** Associate of the Harvard University Physics Department. ABSTRACT 1. SuperString Theory can naturally be based on a Quantum Computer foundation. This provides a totally new view of SuperString Theory. 2. The Standard Model of elementary particles can be viewed as defining a Quantum Computer Grammar and language. 3. A Quantum Computer can be represented in part as a second-quantized Fermi field. 4. A Quantum Computer in a certain limit naturally forms a Superspace upon which Supersymmetry rotations can be defined – a Continuum Quantum Computer. 5. A representation of Quantum Computers exists that is similar to Turing Machines - a Quantum Turing Machine. As part of this development we define various types of Quantum Grammars. 6. High level Quantum Computer languages are described for the first time. New linguistic views of the most fundamental theories of Physics, the Standard Model and SuperString Theory are described. In these new linguistic representations particles become literally symbols or letters, and particle interactions become grammar rules. This view is NOT the same as the often-expressed view that Mathematics is the language of Physics. The linguistic representation is a specific new mathematical construct. We show how to create a SuperString Quantum Computer that naturally provides a framework for SuperStrings in general and heterotic SuperStrings in particular. There are also a number of new developments relating to Quantum Computers and Quantum Turing Machines that are of interest to Computer Science.
    [Show full text]
  • Automata Modeling for Cognitive Interference in Users' Relevance
    Quantum Informatics for Cognitive, Social, and Semantic Processes: Papers from the AAAI Fall Symposium (FS-10-08) Automata Modeling for Cognitive Interference in Users’ Relevance Judgment Peng Zhang1, Dawei Song1, Yuexian Hou1,2, Jun Wang1, Peter Bruza3 1School of Computing, The Robert Gordon University, UK. 2School of Computer Sci. & Tec., Tianjin University, China. 3Queensland University of Technology, Australia Email: [email protected] Abstract This paper is a step further along the direction of inves- tigating the quantum-like interference in a central IR pro- Quantum theory has recently been employed to further ad- cess - user’s relevance judgment, where users are involved vance the theory of information retrieval (IR). A challenging to judge the relevance degree of documents with respect to research topic is to investigate the so called quantum-like in- a given query. In this process, users’ relevance judgment terference in users’ relevance judgment process, where users are involved to judge the relevance degree of each document for the current document is often interfered by the judgment with respect to a given query. In this process, users’ relevance for previously seen documents, as a result of cognitive in- judgment for the current document is often interfered by the terference. A typical scenario is that, after finding a more judgment for previous documents, due to the interference on relevant document, a user may lower the relevance degree users’ cognitive status. Research from cognitive science has of a previously judged document. For example, when a user demonstrated some initial evidence of quantum-like cogni- judges whether a document d0 about “the theory of relativ- tive interference in human decision making, which underpins ity” is relevant to the query “Albert Einstein”, the user might the user’s relevance judgment process.
    [Show full text]
  • Quantum Computing : a Gentle Introduction / Eleanor Rieffel and Wolfgang Polak
    QUANTUM COMPUTING A Gentle Introduction Eleanor Rieffel and Wolfgang Polak The MIT Press Cambridge, Massachusetts London, England ©2011 Massachusetts Institute of Technology All rights reserved. No part of this book may be reproduced in any form by any electronic or mechanical means (including photocopying, recording, or information storage and retrieval) without permission in writing from the publisher. For information about special quantity discounts, please email [email protected] This book was set in Syntax and Times Roman by Westchester Book Group. Printed and bound in the United States of America. Library of Congress Cataloging-in-Publication Data Rieffel, Eleanor, 1965– Quantum computing : a gentle introduction / Eleanor Rieffel and Wolfgang Polak. p. cm.—(Scientific and engineering computation) Includes bibliographical references and index. ISBN 978-0-262-01506-6 (hardcover : alk. paper) 1. Quantum computers. 2. Quantum theory. I. Polak, Wolfgang, 1950– II. Title. QA76.889.R54 2011 004.1—dc22 2010022682 10987654321 Contents Preface xi 1 Introduction 1 I QUANTUM BUILDING BLOCKS 7 2 Single-Qubit Quantum Systems 9 2.1 The Quantum Mechanics of Photon Polarization 9 2.1.1 A Simple Experiment 10 2.1.2 A Quantum Explanation 11 2.2 Single Quantum Bits 13 2.3 Single-Qubit Measurement 16 2.4 A Quantum Key Distribution Protocol 18 2.5 The State Space of a Single-Qubit System 21 2.5.1 Relative Phases versus Global Phases 21 2.5.2 Geometric Views of the State Space of a Single Qubit 23 2.5.3 Comments on General Quantum State Spaces
    [Show full text]
  • Computational Power of Observed Quantum Turing Machines
    Computational Power of Observed Quantum Turing Machines Simon Perdrix PPS, Universit´eParis Diderot & LFCS, University of Edinburgh New Worlds of Computation, January 2009 Quantum Computing Basics State space in a classical world of computation: countable A. inaquantumworld: Hilbertspace CA ket map . : A CA | i → s.t. x , x A is an orthonormal basis of CA {| i ∈ } Arbitrary states Φ = αx x | i x A X∈ 2 s.t. x A αx =1 ∈ | | P Quantum Computing Basics bra map . : A L(CA, C) h | → s.t. x, y A, ∀ ∈ 1 if x = y y x = “ Kronecker ” h | | i (0 otherwise v,t A, v t : CA CA: ∀ ∈ | ih | → v if t = x ( v t ) x = v ( t x )= | i “ v t t v ” | ih | | i | i h | | i (0 otherwise | ih |≈ 7→ Evolution of isolated systems: Linear map U L(CA, CA) ∈ U = ux,y y x | ih | x,y A X∈ which is an isometry (U †U = I). Observation Let Φ = αx x | i x A X∈ (Full) measurement in standard basis: 2 The probability to observe a A is αa . ∈ | | If a A is observed, the state becomes Φa = a . ∈ | i Partial measurement in standard basis: Let K = Kλ, λ Λ be a partition of A. { ∈ } 2 The probability to observe λ Λ is pλ = a Kλ αa ∈ ∈ | | If λ Λ is observed, the state becomes P ∈ 1 1 Φλ = PλΦ = αa a √pλ √pλ | i a Kλ X∈ where Pλ = a Kλ a a . ∈ | ih | P Observation Let Φ = αx x | i x A X∈ (Full) measurement in standard basis: 2 The probability to observe a A is αa .
    [Show full text]
  • Probabilistic and Quantum Finite Automata with Postselection
    Probabilistic and quantum finite automata with ⋆ ⋆⋆ postselection ’ Abuzer Yakaryılmaz and A. C. Cem Say Bo˘gazi¸ci University, Department of Computer Engineering, Bebek 34342 Istanbul,˙ Turkey abuzer,[email protected] June 26, 2018 Abstract. We prove that endowing a real-time probabilistic or quantum computer with the ability of postselection increases its computational power. For this purpose, we provide a new model of finite automata with postselection, and compare it with the model of L¯ace et al. We examine the related language classes, and also establish separations between the classical and quantum versions, and between the zero-error vs. bounded- error modes of recognition in this model. 1 Introduction The notion of postselection as a mode of computation was introduced by Aaronson [1]. Postselection is the (unrealistic) capability of discarding all branches of a computation in which a specific event does not occur, and focusing on the surviving branches for the final decision about the membership of the input string in the recognized language. Aaronson examined PostBQP, the class of languages recognized with bounded error by polynomial-time quantum computers with postselection, and showed it to be identical to the well-known classical complexity class PP. It is, arXiv:1102.0666v1 [cs.CC] 3 Feb 2011 however, still an open question whether postselection adds anything to the power of polynomial-time computation, since we do not even know whether P, the class of languages recognized by classical computers with zero error in polynomial time, equals PP or not. In this paper, we prove that postselection is useful for real-time computers with a constant space bound, that is, finite automata.
    [Show full text]
  • Quantum Finite Automata and Their Simulations
    Quantum Finite Automata and Their Simulations Gustaw Lippa Krzysztof Makie la Marcin Kuta [email protected] Department of Computer Science, AGH University of Science and Technology, Krak´ow, Poland Krak´owQuantum Informatics Seminar (KQIS) 13 October 2020 Outline Motivation Quantum finite automata Library for simulating quantum finite automata Existing libraries Java Formal Languages and Automata Package (JFLAP) Quirk Quantum++ Q# Qiskit ProjectQ Probabilistic automata Probabilistic Finite Automaton (PFA) Quantum automata Measure-Once Quantum Finite Automaton (MO-QFA) Measure-Many Quantum Finite Automaton (MM-QFA) General Quantum Finite Automaton (GQFA) Types of Finite Automata Classical automata Deterministic Finite Automaton (DFA) Nondeterministic Finite Automaton (NFA) Alternating Finite Automaton (AFA) Quantum automata Measure-Once Quantum Finite Automaton (MO-QFA) Measure-Many Quantum Finite Automaton (MM-QFA) General Quantum Finite Automaton (GQFA) Types of Finite Automata Classical automata Deterministic Finite Automaton (DFA) Nondeterministic Finite Automaton (NFA) Alternating Finite Automaton (AFA) Probabilistic automata Probabilistic Finite Automaton (PFA) Types of Finite Automata Classical automata Deterministic Finite Automaton (DFA) Nondeterministic Finite Automaton (NFA) Alternating Finite Automaton (AFA) Probabilistic automata Probabilistic Finite Automaton (PFA) Quantum automata Measure-Once Quantum Finite Automaton (MO-QFA) Measure-Many Quantum Finite Automaton (MM-QFA) General Quantum Finite Automaton (GQFA) Deterministic
    [Show full text]
  • Quantum Computational Complexity Theory Is to Un- Derstand the Implications of Quantum Physics to Computational Complexity Theory
    Quantum Computational Complexity John Watrous Institute for Quantum Computing and School of Computer Science University of Waterloo, Waterloo, Ontario, Canada. Article outline I. Definition of the subject and its importance II. Introduction III. The quantum circuit model IV. Polynomial-time quantum computations V. Quantum proofs VI. Quantum interactive proof systems VII. Other selected notions in quantum complexity VIII. Future directions IX. References Glossary Quantum circuit. A quantum circuit is an acyclic network of quantum gates connected by wires: the gates represent quantum operations and the wires represent the qubits on which these operations are performed. The quantum circuit model is the most commonly studied model of quantum computation. Quantum complexity class. A quantum complexity class is a collection of computational problems that are solvable by a cho- sen quantum computational model that obeys certain resource constraints. For example, BQP is the quantum complexity class of all decision problems that can be solved in polynomial time by a arXiv:0804.3401v1 [quant-ph] 21 Apr 2008 quantum computer. Quantum proof. A quantum proof is a quantum state that plays the role of a witness or certificate to a quan- tum computer that runs a verification procedure. The quantum complexity class QMA is defined by this notion: it includes all decision problems whose yes-instances are efficiently verifiable by means of quantum proofs. Quantum interactive proof system. A quantum interactive proof system is an interaction between a verifier and one or more provers, involving the processing and exchange of quantum information, whereby the provers attempt to convince the verifier of the answer to some computational problem.
    [Show full text]