ZX-Calculus for the Working Quantum Computer Scientist
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Quantum Information
Quantum Information J. A. Jones Michaelmas Term 2010 Contents 1 Dirac Notation 3 1.1 Hilbert Space . 3 1.2 Dirac notation . 4 1.3 Operators . 5 1.4 Vectors and matrices . 6 1.5 Eigenvalues and eigenvectors . 8 1.6 Hermitian operators . 9 1.7 Commutators . 10 1.8 Unitary operators . 11 1.9 Operator exponentials . 11 1.10 Physical systems . 12 1.11 Time-dependent Hamiltonians . 13 1.12 Global phases . 13 2 Quantum bits and quantum gates 15 2.1 The Bloch sphere . 16 2.2 Density matrices . 16 2.3 Propagators and Pauli matrices . 18 2.4 Quantum logic gates . 18 2.5 Gate notation . 21 2.6 Quantum networks . 21 2.7 Initialization and measurement . 23 2.8 Experimental methods . 24 3 An atom in a laser field 25 3.1 Time-dependent systems . 25 3.2 Sudden jumps . 26 3.3 Oscillating fields . 27 3.4 Time-dependent perturbation theory . 29 3.5 Rabi flopping and Fermi's Golden Rule . 30 3.6 Raman transitions . 32 3.7 Rabi flopping as a quantum gate . 32 3.8 Ramsey fringes . 33 3.9 Measurement and initialisation . 34 1 CONTENTS 2 4 Spins in magnetic fields 35 4.1 The nuclear spin Hamiltonian . 35 4.2 The rotating frame . 36 4.3 On-resonance excitation . 38 4.4 Excitation phases . 38 4.5 Off-resonance excitation . 39 4.6 Practicalities . 40 4.7 The vector model . 40 4.8 Spin echoes . 41 4.9 Measurement and initialisation . 42 5 Photon techniques 43 5.1 Spatial encoding . -
Lecture Notes: Qubit Representations and Rotations
Phys 711 Topics in Particles & Fields | Spring 2013 | Lecture 1 | v0.3 Lecture notes: Qubit representations and rotations Jeffrey Yepez Department of Physics and Astronomy University of Hawai`i at Manoa Watanabe Hall, 2505 Correa Road Honolulu, Hawai`i 96822 E-mail: [email protected] www.phys.hawaii.edu/∼yepez (Dated: January 9, 2013) Contents mathematical object (an abstraction of a two-state quan- tum object) with a \one" state and a \zero" state: I. What is a qubit? 1 1 0 II. Time-dependent qubits states 2 jqi = αj0i + βj1i = α + β ; (1) 0 1 III. Qubit representations 2 A. Hilbert space representation 2 where α and β are complex numbers. These complex B. SU(2) and O(3) representations 2 numbers are called amplitudes. The basis states are or- IV. Rotation by similarity transformation 3 thonormal V. Rotation transformation in exponential form 5 h0j0i = h1j1i = 1 (2a) VI. Composition of qubit rotations 7 h0j1i = h1j0i = 0: (2b) A. Special case of equal angles 7 In general, the qubit jqi in (1) is said to be in a superpo- VII. Example composite rotation 7 sition state of the two logical basis states j0i and j1i. If References 9 α and β are complex, it would seem that a qubit should have four free real-valued parameters (two magnitudes and two phases): I. WHAT IS A QUBIT? iθ0 α φ0 e jqi = = iθ1 : (3) Let us begin by introducing some notation: β φ1 e 1 state (called \minus" on the Bloch sphere) Yet, for a qubit to contain only one classical bit of infor- 0 mation, the qubit need only be unimodular (normalized j1i = the alternate symbol is |−i 1 to unity) α∗α + β∗β = 1: (4) 0 state (called \plus" on the Bloch sphere) 1 Hence it lives on the complex unit circle, depicted on the j0i = the alternate symbol is j+i: 0 top of Figure 1. -
Completeness of the ZX-Calculus
Completeness of the ZX-calculus Quanlong Wang Wolfson College University of Oxford A thesis submitted for the degree of Doctor of Philosophy Hilary 2018 Acknowledgements Firstly, I would like to express my sincere gratitude to my supervisor Bob Coecke for all his huge help, encouragement, discussions and comments. I can not imagine what my life would have been like without his great assistance. Great thanks to my colleague, co-auhor and friend Kang Feng Ng, for the valuable cooperation in research and his helpful suggestions in my daily life. My sincere thanks also goes to Amar Hadzihasanovic, who has kindly shared his idea and agreed to cooperate on writing a paper based one his results. Many thanks to Simon Perdrix, from whom I have learned a lot and received much help when I worked with him in Nancy, while still benefitting from this experience in Oxford. I would also like to thank Miriam Backens for loads of useful discussions, advertising for my talk in QPL and helping me on latex problems. Special thanks to Dan Marsden for his patience and generousness in answering my questions and giving suggestions. I would like to thank Xiaoning Bian for always being ready to help me solve problems in using latex and other softwares. I also wish to thank all the people who attended the weekly ZX meeting for many interesting discussions. I am also grateful to my college advisor Jonathan Barrett and department ad- visor Jamie Vicary, thank you for chatting with me about my research and my life. I particularly want to thank my examiners, Ross Duncan and Sam Staton, for their very detailed and helpful comments and corrections by which this thesis has been significantly improved. -
Introduction to Quantum Information and Computation
Introduction to Quantum Information and Computation Steven M. Girvin ⃝c 2019, 2020 [Compiled: May 2, 2020] Contents 1 Introduction 1 1.1 Two-Slit Experiment, Interference and Measurements . 2 1.2 Bits and Qubits . 3 1.3 Stern-Gerlach experiment: the first qubit . 8 2 Introduction to Hilbert Space 16 2.1 Linear Operators on Hilbert Space . 18 2.2 Dirac Notation for Operators . 24 2.3 Orthonormal bases for electron spin states . 25 2.4 Rotations in Hilbert Space . 29 2.5 Hilbert Space and Operators for Multiple Spins . 38 3 Two-Qubit Gates and Entanglement 43 3.1 Introduction . 43 3.2 The CNOT Gate . 44 3.3 Bell Inequalities . 51 3.4 Quantum Dense Coding . 55 3.5 No-Cloning Theorem Revisited . 59 3.6 Quantum Teleportation . 60 3.7 YET TO DO: . 61 4 Quantum Error Correction 63 4.1 An advanced topic for the experts . 68 5 Yet To Do 71 i Chapter 1 Introduction By 1895 there seemed to be nothing left to do in physics except fill out a few details. Maxwell had unified electriciy, magnetism and optics with his theory of electromagnetic waves. Thermodynamics was hugely successful well before there was any deep understanding about the properties of atoms (or even certainty about their existence!) could make accurate predictions about the efficiency of the steam engines powering the industrial revolution. By 1895, statistical mechanics was well on its way to providing a microscopic basis in terms of the random motions of atoms to explain the macroscopic predictions of thermodynamics. However over the next decade, a few careful observers (e.g. -
Studies in the Geometry of Quantum Measurements
Irina Dumitru Studies in the Geometry of Quantum Measurements Studies in the Geometry of Quantum Measurements Studies in Irina Dumitru Irina Dumitru is a PhD student at the department of Physics at Stockholm University. She has carried out research in the field of quantum information, focusing on the geometry of Hilbert spaces. ISBN 978-91-7911-218-9 Department of Physics Doctoral Thesis in Theoretical Physics at Stockholm University, Sweden 2020 Studies in the Geometry of Quantum Measurements Irina Dumitru Academic dissertation for the Degree of Doctor of Philosophy in Theoretical Physics at Stockholm University to be publicly defended on Thursday 10 September 2020 at 13.00 in sal C5:1007, AlbaNova universitetscentrum, Roslagstullsbacken 21, and digitally via video conference (Zoom). Public link will be made available at www.fysik.su.se in connection with the nailing of the thesis. Abstract Quantum information studies quantum systems from the perspective of information theory: how much information can be stored in them, how much the information can be compressed, how it can be transmitted. Symmetric informationally- Complete POVMs are measurements that are well-suited for reading out the information in a system; they can be used to reconstruct the state of a quantum system without ambiguity and with minimum redundancy. It is not known whether such measurements can be constructed for systems of any finite dimension. Here, dimension refers to the dimension of the Hilbert space where the state of the system belongs. This thesis introduces the notion of alignment, a relation between a symmetric informationally-complete POVM in dimension d and one in dimension d(d-2), thus contributing towards the search for these measurements. -
The Bloch Equations a Quick Review of Spin- 1 Conventions and Notation
Ph195a lecture notes, 11/21/01 The Bloch Equations 1 A quick review of spin- 2 conventions and notation 1 The quantum state of a spin- 2 particle is represented by a vector in a two-dimensional complex Hilbert space H2. Let | +z 〉 and | −z 〉 be eigenstates of the operator corresponding to component of spin along the z coordinate axis, ℏ S | + 〉 =+ | + 〉, z z 2 z ℏ S | − 〉 = − | − 〉. 1 z z 2 z In this basis, the operators corresponding to spin components projected along the z,y,x coordinate axes may be represented by the following matrices: ℏ ℏ 10 Sz = σz = , 2 2 0 −1 ℏ ℏ 01 Sx = σx = , 2 2 10 ℏ ℏ 0 −i Sy = σy = . 2 2 2 i 0 We commonly use | ±x 〉 to denote eigenstates of Sx, and similarly for Sy. The dimensionless matrices σx,σy,σz are known as the Pauli matrices, and satisfy the following commutation relations: σx,σy = 2iσz, σy,σz = 2iσx, σz,σx = 2iσy. 3 In addition, Trσiσj = 2δij, 4 and 2 2 2 σx = σy = σz = 1. 5 The Pauli matrices are both Hermitian and unitary. 1 An arbitrary state for an isolated spin- 2 particle may be written θ ϕ θ ϕ |Ψ 〉 = cos exp −i | + 〉 + sin exp i | − 〉, 6 2 2 z 2 2 z where θ and ϕ are real parameters that may be chosen in the ranges 0 ≤ θ ≤ π and 0 ≤ ϕ ≤ 2π. Note that there should really be four real degrees of freedom for a vector in a 1 two-dimensional complex Hilbert space, but one is removed by normalization and another because we don’t care about the overall phase of the state of an isolated quantum system. -
Topological Complexity for Quantum Information
Topological Complexity for Quantum Information Zhengwei Liu Tsinghua University Joint with Arthur Jaffe, Xun Gao, Yunxiang Ren and Shengtao Wang Seminar at Dublin IAS, Oct 14, 2020 Z. Liu (Tsinghua University) Topological Complexity for QI Oct 14, 2020 1 / 31 Topological Complexity: The complexity of computing matrix products or contractions of tensors may grows exponentially using the state sum over the basis. Using topological ideas, such as knot-theoretical isotopy, one could compute the tensors in a more efficient way. Fractionalization: We open the \black box" in tensor network and explore \internal pictorial relations" using the 3D quon language, a fractionalization of tensor network. (Euler's formula, Yang-Baxter equation/relation, star-triangle equation, Kramer-Wannier duality, Jordan-Wigner transformation etc.) Applications: We show that two well-known efficiently classically simulable families, Clifford gates and matchgates, correspond to two kinds of topological complexities. Besides the two simulable families, we introduce a new method to design efficiently classically simulable tensor networks and new families of exactly solvable models. Z. Liu (Tsinghua University) Topological Complexity for QI Oct 14, 2020 2 / 31 Qubits and Gates 2 A qubit is a vector state in C . 2 n An n-qubit is a vector state jφi in (C ) . 2 n A n-qubit gate is a unitary on (C ) . Z. Liu (Tsinghua University) Topological Complexity for QI Oct 14, 2020 3 / 31 Quantum Simulation Feynman and Manin both proposed Quantum Simulation in 1980. Simulate a quantum process by local interactions on qubits. Present an n-qubit gate as a composition of 1-qubit gates and adjacent 2-qubits gates. -
Unifying Cps Nqs
Citation for published version: Clark, SR 2018, 'Unifying Neural-network Quantum States and Correlator Product States via Tensor Networks', Journal of Physics A: Mathematical and General, vol. 51, no. 13, 135301. https://doi.org/10.1088/1751- 8121/aaaaf2 DOI: 10.1088/1751-8121/aaaaf2 Publication date: 2018 Document Version Peer reviewed version Link to publication This is an author-created, in-copyedited version of an article published in Journal of Physics A: Mathematical and Theoretical. IOP Publishing Ltd is not responsible for any errors or omissions in this version of the manuscript or any version derived from it. The Version of Record is available online at http://iopscience.iop.org/article/10.1088/1751-8121/aaaaf2/meta University of Bath Alternative formats If you require this document in an alternative format, please contact: [email protected] General rights Copyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights. Take down policy If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim. Download date: 04. Oct. 2021 Unifying Neural-network Quantum States and Correlator Product States via Tensor Networks Stephen R Clarkyz yDepartment of Physics, University of Bath, Claverton Down, Bath BA2 7AY, U.K. zMax Planck Institute for the Structure and Dynamics of Matter, University of Hamburg CFEL, Hamburg, Germany E-mail: [email protected] Abstract. -
Remote Preparation of $ W $ States from Imperfect Bipartite Sources
Remote preparation of W states from imperfect bipartite sources M. G. M. Moreno, M´arcio M. Cunha, and Fernando Parisio∗ Departamento de F´ısica, Universidade Federal de Pernambuco, 50670-901,Recife, Pernambuco, Brazil Several proposals to produce tripartite W -type entanglement are probabilistic even if no imperfec- tions are considered in the processes. We provide a deterministic way to remotely create W states out of an EPR source. The proposal is made viable through measurements (which can be demoli- tive) in an appropriate three-qubit basis. The protocol becomes probabilistic only when source flaws are considered. It turns out that, even in this situation, it is robust against imperfections in two senses: (i) It is possible, after postselection, to create a pure ensemble of W states out of an EPR source containing a systematic error; (ii) If no postselection is done, the resulting mixed state has a fidelity, with respect to a pure |W i, which is higher than that of the imperfect source in comparison to an ideal EPR source. This simultaneously amounts to entanglement concentration and lifting. PACS numbers: 03.67.Bg, 03.67.-a arXiv:1509.08438v2 [quant-ph] 25 Aug 2016 ∗ [email protected] 2 I. INTRODUCTION The inventory of potential achievements that quantum entanglement may bring about has steadily grown for decades. It is the concept behind most of the non-trivial, classically prohibitive tasks in information science [1]. However, for entanglement to become a useful resource in general, much work is yet to be done. The efficient creation of entanglement, often involving many degrees of freedom, is one of the first challenges to be coped with, whose simplest instance are the sources of correlated pairs of two-level systems. -
Chapter 2 Quantum Gates
Chapter 2 Quantum Gates “When we get to the very, very small world—say circuits of seven atoms—we have a lot of new things that would happen that represent completely new opportunities for design. Atoms on a small scale behave like nothing on a large scale, for they satisfy the laws of quantum mechanics. So, as we go down and fiddle around with the atoms down there, we are working with different laws, and we can expect to do different things. We can manufacture in different ways. We can use, not just circuits, but some system involving the quantized energy levels, or the interactions of quantized spins.” – Richard P. Feynman1 Currently, the circuit model of a computer is the most useful abstraction of the computing process and is widely used in the computer industry in the design and construction of practical computing hardware. In the circuit model, computer scien- tists regard any computation as being equivalent to the action of a circuit built out of a handful of different types of Boolean logic gates acting on some binary (i.e., bit string) input. Each logic gate transforms its input bits into one or more output bits in some deterministic fashion according to the definition of the gate. By compos- ing the gates in a graph such that the outputs from earlier gates feed into the inputs of later gates, computer scientists can prove that any feasible computation can be performed. In this chapter we will look at the types of logic gates used within circuits and how the notions of logic gates need to be modified in the quantum context. -
The SIC Question: History and State of Play
axioms Review The SIC Question: History and State of Play Christopher A. Fuchs 1,*, Michael C. Hoang 2 and Blake C. Stacey 1 1 Physics Department, University of Massachusetts Boston, Boston, MA 02125, USA; [email protected] 2 Computer Science Department, University of Massachusetts Boston, Boston, MA 02125, USA; [email protected] * Correspondence: [email protected] or [email protected]; Tel.: +1-617-287-3317 Academic Editor: Palle Jorgensen Received: 30 June 2017 ; Accepted: 15 July 2017; Published: 18 July 2017 Abstract: Recent years have seen significant advances in the study of symmetric informationally complete (SIC) quantum measurements, also known as maximal sets of complex equiangular lines. Previously, the published record contained solutions up to dimension 67, and was with high confidence complete up through dimension 50. Computer calculations have now furnished solutions in all dimensions up to 151, and in several cases beyond that, as large as dimension 844. These new solutions exhibit an additional type of symmetry beyond the basic definition of a SIC, and so verify a conjecture of Zauner in many new cases. The solutions in dimensions 68 through 121 were obtained by Andrew Scott, and his catalogue of distinct solutions is, with high confidence, complete up to dimension 90. Additional results in dimensions 122 through 151 were calculated by the authors using Scott’s code. We recap the history of the problem, outline how the numerical searches were done, and pose some conjectures on how the search technique could be improved. In order to facilitate communication across disciplinary boundaries, we also present a comprehensive bibliography of SIC research. -
Categorical Tensor Network States
Categorical Tensor Network States Jacob D. Biamonte,1,2,3,a Stephen R. Clark2,4 and Dieter Jaksch5,4,2 1Oxford University Computing Laboratory, Parks Road Oxford, OX1 3QD, United Kingdom 2Centre for Quantum Technologies, National University of Singapore, 3 Science Drive 2, Singapore 117543, Singapore 3ISI Foundation, Torino Italy 4Keble College, Parks Road, University of Oxford, Oxford OX1 3PG, United Kingdom 5Clarendon Laboratory, Department of Physics, University of Oxford, Oxford OX1 3PU, United Kingdom We examine the use of string diagrams and the mathematics of category theory in the description of quantum states by tensor networks. This approach lead to a unifi- cation of several ideas, as well as several results and methods that have not previously appeared in either side of the literature. Our approach enabled the development of a tensor network framework allowing a solution to the quantum decomposition prob- lem which has several appealing features. Specifically, given an n-body quantum state |ψi, we present a new and general method to factor |ψi into a tensor network of clearly defined building blocks. We use the solution to expose a previously un- known and large class of quantum states which we prove can be sampled efficiently and exactly. This general framework of categorical tensor network states, where a combination of generic and algebraically defined tensors appear, enhances the theory of tensor network states. PACS numbers: 03.65.Fd, 03.65.Ca, 03.65.Aa arXiv:1012.0531v2 [quant-ph] 17 Dec 2011 a [email protected] 2 I. INTRODUCTION Tensor network states have recently emerged from Quantum Information Science as a gen- eral method to simulate quantum systems using classical computers.