Quantum Walks and Ground State Problems
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On the Tightness of the Buhrman-Cleve-Wigderson Simulation
On the tightness of the Buhrman-Cleve-Wigderson simulation Shengyu Zhang Department of Computer Science and Engineering, The Chinese University of Hong Kong. [email protected] Abstract. Buhrman, Cleve and Wigderson gave a general communica- 1 1 n n tion protocol for block-composed functions f(g1(x ; y ); ··· ; gn(x ; y )) by simulating a decision tree computation for f [3]. It is also well-known that this simulation can be very inefficient for some functions f and (g1; ··· ; gn). In this paper we show that the simulation is actually poly- nomially tight up to the choice of (g1; ··· ; gn). This also implies that the classical and quantum communication complexities of certain block- composed functions are polynomially related. 1 Introduction Decision tree complexity [4] and communication complexity [7] are two concrete models for studying computational complexity. In [3], Buhrman, Cleve and Wigderson gave a general method to design communication 1 1 n n protocol for block-composed functions f(g1(x ; y ); ··· ; gn(x ; y )). The basic idea is to simulate the decision tree computation for f, with queries i i of the i-th variable answered by a communication protocol for gi(x ; y ). In the language of complexity measures, this result gives CC(f(g1; ··· ; gn)) = O~(DT(f) · max CC(gi)) (1) i where CC and DT are the communication complexity and the decision tree complexity, respectively. This simulation holds for all the models: deterministic, randomized and quantum1. It is also well known that the communication protocol by the above simulation can be very inefficient. -
Thesis Is Owed to Him, Either Directly Or Indirectly
UvA-DARE (Digital Academic Repository) Quantum Computing and Communication Complexity de Wolf, R.M. Publication date 2001 Document Version Final published version Link to publication Citation for published version (APA): de Wolf, R. M. (2001). Quantum Computing and Communication Complexity. Institute for Logic, Language and Computation. General rights It is not permitted to download or to forward/distribute the text or part of it without the consent of the author(s) and/or copyright holder(s), other than for strictly personal, individual use, unless the work is under an open content license (like Creative Commons). Disclaimer/Complaints regulations If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the Library know, stating your reasons. In case of a legitimate complaint, the Library will make the material inaccessible and/or remove it from the website. Please Ask the Library: https://uba.uva.nl/en/contact, or a letter to: Library of the University of Amsterdam, Secretariat, Singel 425, 1012 WP Amsterdam, The Netherlands. You will be contacted as soon as possible. UvA-DARE is a service provided by the library of the University of Amsterdam (https://dare.uva.nl) Download date:30 Sep 2021 Quantum Computing and Communication Complexity Ronald de Wolf Quantum Computing and Communication Complexity ILLC Dissertation Series 2001-06 For further information about ILLC-publications, please contact Institute for Logic, Language and Computation Universiteit van Amsterdam Plantage Muidergracht 24 1018 TV Amsterdam phone: +31-20-525 6051 fax: +31-20-525 5206 e-mail: [email protected] homepage: http://www.illc.uva.nl/ Quantum Computing and Communication Complexity Academisch Proefschrift ter verkrijging van de graad van doctor aan de Universiteit van Amsterdam op gezag van de Rector Magni¯cus prof.dr. -
Continuous Time Quantum Walks (CTQW)
Continuous Time Quantum Walks (CTQW) Mack Johnson March 2015 1 Introduction Quantum computing became a prominent area of research with publications such as Feynman's 1986 pa- per suggesting a construction for a Hamiltonian that can implement any quantum circuit [1]. Some of the key results in quantum information science such as Shor's algorithm [2] and Grover's algorithm [3] which show speed up over classical algorithms for integer factorisation and database searching have motivated a wealth of research in the field. A particular field of interesting research among these are quantum random walks - the quantum counterpart to classical random walks, used in studies of the fundamentals and applications of diffusion [4{7], modelling of transport for solvents [8], electrons [9], mass, [10], heat [11], radiation, [12], photon motion in isotropic media [13], polymer dynamics [14, 15] among other applications not limited to modelling of stock exchanges in finance, peer to peer networks, astrophysics and the creation of new classical algorithms [16{22]. If the classical random walks are so widely used, then why would one wish to study their quantum counterpart? Grover's algorithm is an example that can be interpreted as a discrete time quantum walk which offers a polynomial speed up over a classical algorithm when searching an unstructured database for a given marked element. Ambainis discovered a quantum algorithm based off of a quantum random walk to solve the element distinctness problem quicker than a classical algorithm [23]. That is, given a set of elements x1; x2:::xn 2 [M] how many times do we have to query to determine if all elements are distinct? This problem is solved by a classical algorithm if we sort Ω(N) times. -
Efficient Quantum Algorithms for Simulating Lindblad Evolution
Efficient Quantum Algorithms for Simulating Lindblad Evolution∗ Richard Cleveyzx Chunhao Wangyz Abstract We consider the natural generalization of the Schr¨odingerequation to Markovian open system dynamics: the so-called the Lindblad equation. We give a quantum algorithm for simulating the evolution of an n-qubit system for time t within precision . If the Lindbladian consists of poly(n) operators that can each be expressed as a linear combination of poly(n) tensor products of Pauli operators then the gate cost of our algorithm is O(t polylog(t/)poly(n)). We also obtain similar bounds for the cases where the Lindbladian consists of local operators, and where the Lindbladian consists of sparse operators. This is remarkable in light of evidence that we provide indicating that the above efficiency is impossible to attain by first expressing Lindblad evolution as Schr¨odingerevolution on a larger system and tracing out the ancillary system: the cost of such a reduction incurs an efficiency overhead of O(t2/) even before the Hamiltonian evolution simulation begins. Instead, the approach of our algorithm is to use a novel variation of the \linear combinations of unitaries" construction that pertains to channels. 1 Introduction The problem of simulating the evolution of closed systems (captured by the Schr¨odingerequation) was proposed by Feynman [11] in 1982 as a motivation for building quantum computers. Since then, several quantum algorithms have appeared for this problem (see subsection 1.1 for references to these algorithms). However, many quantum systems of interest are not closed but are well-captured by the Lindblad Master equation [20, 12]. -
Arxiv:1611.07995V1 [Quant-Ph] 23 Nov 2016
Factoring using 2n + 2 qubits with Toffoli based modular multiplication Thomas H¨aner∗ Station Q Quantum Architectures and Computation Group, Microsoft Research, Redmond, WA 98052, USA and Institute for Theoretical Physics, ETH Zurich, 8093 Zurich, Switzerland Martin Roettelery and Krysta M. Svorez Station Q Quantum Architectures and Computation Group, Microsoft Research, Redmond, WA 98052, USA We describe an implementation of Shor's quantum algorithm to factor n-bit integers using only 2n+2 qubits. In contrast to previous space-optimized implementations, ours features a purely Toffoli based modular multiplication circuit. The circuit depth and the overall gate count are in (n3) and (n3 log n), respectively. We thus achieve the same space and time costs as TakahashiO et al. [1], Owhile using a purely classical modular multiplication circuit. As a consequence, our approach evades most of the cost overheads originating from rotation synthesis and enables testing and localization of faults in both, the logical level circuit and an actual quantum hardware implementation. Our new (in-place) constant-adder, which is used to construct the modular multiplication circuit, uses only dirty ancilla qubits and features a circuit size and depth in (n log n) and (n), respectively. O O I. INTRODUCTION Cuccaro [5] Takahashi [6] Draper [4] Our adder Size Θ(n) Θ(n) Θ(n2) Θ(n log n) Quantum computers offer an exponential speedup over Depth Θ(n) Θ(n) Θ(n) Θ(n) their classical counterparts for solving certain problems, n the most famous of which is Shor's algorithm [2] for fac- Ancillas n+1 (clean) n (clean) 0 2 (dirty) toring a large number N | an algorithm that enables the breaking of many popular encryption schemes including Table I. -
Durham E-Theses
Durham E-Theses Quantum search at low temperature in the single avoided crossing model PATEL, PARTH,ASHVINKUMAR How to cite: PATEL, PARTH,ASHVINKUMAR (2019) Quantum search at low temperature in the single avoided crossing model, Durham theses, Durham University. Available at Durham E-Theses Online: http://etheses.dur.ac.uk/13285/ Use policy The full-text may be used and/or reproduced, and given to third parties in any format or medium, without prior permission or charge, for personal research or study, educational, or not-for-prot purposes provided that: • a full bibliographic reference is made to the original source • a link is made to the metadata record in Durham E-Theses • the full-text is not changed in any way The full-text must not be sold in any format or medium without the formal permission of the copyright holders. Please consult the full Durham E-Theses policy for further details. Academic Support Oce, Durham University, University Oce, Old Elvet, Durham DH1 3HP e-mail: [email protected] Tel: +44 0191 334 6107 http://etheses.dur.ac.uk 2 Quantum search at low temperature in the single avoided crossing model Parth Ashvinkumar Patel A Thesis presented for the degree of Master of Science by Research Dr. Vivien Kendon Department of Physics University of Durham England August 2019 Dedicated to My parents for supporting me throughout my studies. Quantum search at low temperature in the single avoided crossing model Parth Ashvinkumar Patel Submitted for the degree of Master of Science by Research August 2019 Abstract We begin with an n-qubit quantum search algorithm and formulate it in terms of quantum walk and adiabatic quantum computation. -
Hamiltonian Simulation with Nearly Optimal Dependence on All Parameters
Hamiltonian simulation with nearly optimal dependence on all parameters Dominic W. Berry∗ Andrew M. Childsy Robin Kothariz We present an algorithm for sparse Hamiltonian simulation that has optimal dependence on all pa- rameters of interest (up to log factors). Previous algorithms had optimal or near-optimal scaling in some parameters at the cost of poor scaling in others. Hamiltonian simulation via quantum walk has optimal dependence on the sparsity d at the expense of poor scaling in the allowed error . In contrast, an ap- proach based on fractional-query simulation provides optimal scaling in at the expense of poor scaling in d. Here we combine the two approaches, achieving the best features of both. By implementing a linear combination of quantum walk steps with coefficients given by Bessel functions, our algorithm achieves near-linear scaling in τ := dkHkmaxt and sublogarithmic scaling in 1/. Our dependence on is optimal, and we prove a new lower bound ruling out sublinear dependence on τ. The problem of simulating the dynamics of quantum systems was the original motivation for quantum com- puters [14] and remains one of their major potential applications. The first explicit quantum simulation algorithm [16] gave a method for simulating Hamiltonians that are sums of local interaction terms. Aharonov and Ta-Shma gave an efficient simulation algorithm for the more general class of sparse Hamiltonians [2], and much subsequent work has given improved simulations [4,5,6,7,8, 12, 17, 18]. Sparse Hamiltonians include most physically realistic Hamiltonians as a special case. In addition, sparse Hamiltonian simulation can also be used to design other quantum algorithms [9, 10, 15]. -
Quantum Computing: Lecture Notes
Quantum Computing: Lecture Notes Ronald de Wolf Preface These lecture notes were formed in small chunks during my “Quantum computing” course at the University of Amsterdam, Feb-May 2011, and compiled into one text thereafter. Each chapter was covered in a lecture of 2 45 minutes, with an additional 45-minute lecture for exercises and × homework. The first half of the course (Chapters 1–7) covers quantum algorithms, the second half covers quantum complexity (Chapters 8–9), stuff involving Alice and Bob (Chapters 10–13), and error-correction (Chapter 14). A 15th lecture about physical implementations and general outlook was more sketchy, and I didn’t write lecture notes for it. These chapters may also be read as a general introduction to the area of quantum computation and information from the perspective of a theoretical computer scientist. While I made an effort to make the text self-contained and consistent, it may still be somewhat rough around the edges; I hope to continue polishing and adding to it. Comments & constructive criticism are very welcome, and can be sent to [email protected] Attribution and acknowledgements Most of the material in Chapters 1–6 comes from the first chapter of my PhD thesis [71], with a number of additions: the lower bound for Simon, the Fourier transform, the geometric explanation of Grover. Chapter 7 is newly written for these notes, inspired by Santha’s survey [62]. Chapters 8 and 9 are largely new as well. Section 3 of Chapter 8, and most of Chapter 10 are taken (with many changes) from my “quantum proofs” survey paper with Andy Drucker [28]. -
Quantum Information Theory by Michael Aaron Nielsen
Quantum Information Theory By Michael Aaron Nielsen B.Sc., University of Queensland, 1993 B.Sc. (First Class Honours), Mathematics, University of Queensland, 1994 M.Sc., Physics, University of Queensland, 1998 DISSERTATION Submitted in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy Physics The University of New Mexico Albuquerque, New Mexico, USA December 1998 c 1998, Michael Aaron Nielsen ii Dedicated to the memory of Michael Gerard Kennedy 24 January 1951 – 3 June 1998 iii Acknowledgments It is a great pleasure to thank the many people who have contributed to this Dissertation. My deepest thanks goes to my friends and family, especially my parents, Howard and Wendy, for their support and encouragement. Warm thanks also to the many other people who have con- tributed to this Dissertation, especially Carl Caves, who has been a terrific mentor, colleague, and friend; to Gerard Milburn, who got me started in physics, in research, and in quantum in- formation; and to Ben Schumacher, whose boundless enthusiasm and encouragement has provided so much inspiration for my research. Throughout my graduate career I have had the pleasure of many enjoyable and helpful discussions with Howard Barnum, Ike Chuang, Chris Fuchs, Ray- mond Laflamme, Manny Knill, Mark Tracy, and Wojtek Zurek. In particular, Howard Barnum, Carl Caves, Chris Fuchs, Manny Knill, and Ben Schumacher helped me learn much of what I know about quantum operations, entropy, and distance measures for quantum information. The material reviewed in chapters 3 through 5 I learnt in no small measure from these people. Many other friends and colleagues have contributed to this Dissertation. -
Andrew Childs University of Maryland Arxiv:1711.10980
Toward the first quantum simulation with quantum speedup Andrew Childs University of Maryland Dmitri Maslov Yunseong Nam Neil Julien Ross Yuan Su arXiv:1711.10980 Simulating Hamiltonian dynamics on a small quantum computer Andrew Childs Department of Combinatorics & Optimization and Institute for Quantum Computing University of Waterloo based in part on joint work with Dominic Berry, Richard Cleve, Robin Kothari, and Rolando Somma Workshop on What do we do with a small quantum computer? IBM Watson, 9 December 2013 Toward practical quantum speedup IBM Google/UCSB Delft Maryland Important early goal: demonstrate quantum computational advantage … but can we find a practical application of near-term devices? Challenges • Improve experimental systems • Improve algorithms and their implementation, making the best use of available hardware Our goal: Produce concrete resource estimates for the simplest possible practical application of quantum computers Quantum simulation “… nature isn’t classical, dammit, A classical computer cannot even represent and if you want to make a the state efficiently. simulation of nature, you’d better make it quantum mechanical, and by golly it’s a wonderful problem, A quantum computer cannot produce a because it doesn’t look so easy.” complete description of the state. Richard Feynman (1981) Simulating physics with computers But given succinct descriptions of • the initial state (suitable for a quantum computer to prepare it efficiently) and Quantum simulation problem: Given a • a final measurement (say, measurements description of the Hamiltonian H, an of the individual qubits in some basis), evolution time t, and an initial state (0) , a quantum computer can efficiently answer produce the final state ( t ) (to within| i questions that (apparently) a classical one some error tolerance ²|) i cannot. -
On the Equivalence Between Quantum and Random Walks on Finite Graphs
On the equivalence between quantum and random walks on finite graphs Matheus G. Andrade Franklin Marquezino Daniel R. Figueiredo Department of Computer and System Engineering COPPE Federal University of Rio de Janeiro (UFRJ), Brazil fguedesm, franklin, [email protected] February 7, 2020 Abstract Quantum walks on graphs are ubiquitous in quantum computing finding a myriad of ap- plications. Likewise, random walks on graphs are a fundamental building block for a large number of algorithms with diverse applications. While the relationship between quantum and random walks has been recently discussed in specific scenarios, this work establishes a formal equivalence between the processes on arbitrary finite graphs and general conditions for shift and coin operators. It requires empowering random walks with time heterogeneity, where the transition probability of the walker is non-uniform and time dependent. The equivalence is obtained by equating the probability of measuring the quantum walk on a given node of the graph and the probability that the random walk is at that same node, for all nodes and time steps. The result is given by the construction procedure of a matrix sequence for the random walk that yields the exact same vertex probability distribution sequence of any given quantum walk, including the scenario with multiple interfering walkers. Interestingly, these matrices allows for a different simulation approach for quantum walks where node samples respect neighbor locality and convergence is guaranteed by the law of large numbers, enabling efficient (polynomial) sampling of quantum graph trajectories (paths). Furthermore, the complexity of constructing this sequence of matrices is discussed in the general case. -
Exponential Improvement in Precision for Simulating Sparse Hamiltonians
Exponential improvement in precision for simulating sparse Hamiltonians , , Dominic W. Berry∗ Andrew M. Childs† ‡ Richard Cleve§ ‡ Robin Kothari§ Rolando D. Somma¶ Abstract We provide a quantum algorithm for simulating the dynamics of sparse Hamiltonians with complexity sublogarithmic in the inverse error, an exponential improvement over previous meth- ods. Specifically, we show that a d-sparse Hamiltonian H acting on n qubits can be simulated 2 log(τ/ǫ) log (τ/ǫ) for time t with precision ǫ using O τ log log(τ/ǫ) queries and O τ log log(τ/ǫ) n additional 2-qubit 2 gates, where τ = d H maxt. Unlike previous approaches based on product formulas, the query complexity is independentk k of the number of qubits acted on, and for time-varying Hamiltonians, the gate complexity is logarithmic in the norm of the derivative of the Hamiltonian. Our al- gorithm is based on a significantly improved simulation of the continuous- and fractional-query models using discrete quantum queries, showing that the former models are not much more powerful than the discrete model even for very small error. We also simplify the analysis of this conversion, avoiding the need for a complex fault correction procedure. Our simplification relies on a new form of “oblivious amplitude amplification” that can be applied even though the reflection about the input state is unavailable. Finally, we prove new lower bounds showing that our algorithms are optimal as a function of the error. 1 Introduction Simulation of quantum mechanical systems is a major potential application of quantum computers. Indeed, the problem of simulating Hamiltonian dynamics was the original motivation for the idea of quantum computation [21].