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Optimizing and Characterizing Measurement-Only Topological Quantum Computing with Majorana Zero Mode Based Qubits

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Optimizing and Characterizing Measurement-Only Topological Quantum Computing with Majorana Zero Mode Based Qubits University of California Santa Barbara Optimizing and Characterizing Measurement-Only Topological Quantum Computing with Majorana Zero Mode Based Qubits A dissertation submitted in partial satisfaction of the requirements for the degree Doctor of Philosophy in Physics by Alan D Tran Committee in charge: Dr. Parsa Bonderson, Co-Chair Professor Chetan Nayak, Co-Chair Professor Andrea Young September 2020 The Dissertation of Alan D Tran is approved. Professor Andrea Young Professor Chetan Nayak, Committee Co-Chair Dr. Parsa Bonderson, Committee Co-Chair August 2020 Optimizing and Characterizing Measurement-Only Topological Quantum Computing with Majorana Zero Mode Based Qubits Copyright c 2020 by Alan D Tran iii For my brother and sister, my parents, and my grandparents iv Acknowledgements I would like to acknowledge and thank everyone who has made this dissertation and Ph.D. possible. I am beyond grateful to my advisor, Parsa Bonderson, for all his patience and guidance throughout my time here. He has been a pillar of support and encouragement and I count myself exceedingly fortunate to have him as a mentor. I would like to thank all the collaborators I have had the pleasure of working with: Alex Bocharov, Bela Bauer, César Galindo, Colleen Delaney, Eric Rowell, Marcus P. da Silva, Meng Cheng, Roger Mong, Steven Flammia, and Zhenghan Wang. In addition, I want to thank the physics and math community at UCSB who has shaped my experience here. I am lucky to have been able to discuss with and learn from all the students, post-docs, researchers, visitors, and professors at UCSB, KITP, Microsoft, and HRL. Special thanks goes especially to my committee members Chetan Nayak and Andrea Young, and to Sean Fraer who has made every trip to Q all the more enriching. Finally, I am deeply thankful to my friends and family who have supported me always and brightened each day. v Curriculum Vitæ Alan D Tran Education 2020 Ph.D. in Physics (Expected), University of California, Santa Barbara. 2017 M.Sc. in Physics, University of California, Santa Barbara. 2014 B.Sc. in Physics, University of California, Los Angeles. Publications • A. Tran, B. Bauer, P. Bonderson, S. Flammia, and M. P. da Silva, Randomized bench- marking of measurement-only Majorana zero mode qubits, [In preparation] • A. Tran, A. Bocharov, B. Bauer, and P. Bonderson, Optimizing Clifford gate genera- tion for measurement-only topological quantum computation with Majorana zero modes, [SciPost Phys. 8, 91 (2020)] • C. Delaney and A. Tran, A systematic search of knot and link invariants beyond modular data, [arXiv:1806:02843] • P. Bonderson, C. Delaney, C. Galindo, E. Rowell, A. Tran, Z. Wang, On invariants of modular categories beyond modular data, [Journal of Pure and Applied Algebra 223(9) (2019)] vi Abstract Optimizing and Characterizing Measurement-Only Topological Quantum Computing with Majorana Zero Mode Based Qubits by Alan D Tran Quantum computing is a revolutionizing technology on many fronts. Topological quan- tum computing is an especially attractive platform for this due to its innate robustness to local sources of noise and scalability. As the advent of quantum computing technologies nears, it becomes increasingly important to both optimize as much as possible the basic operations and to characterize them. In this thesis we study measurement-only topological quantum comput- ing with Majorana zero mode (MZM) based qubits, particularly on their incarnation as the boudnary defects of 1d topological superconducting nanowires. The specific qubit device we consider are comprised of collections of such wires connected together on a single island such that 4 or 6 MZMs are hosted (tetron and hexon qubits respectively). This thesis focuses on optimizing and characterizing the basic operations needed for quan- tum computing with such MZM qubits, concentrating on hexons which are the smallest MZM qubit allowing measurement-only gates on a single island. We begin by optimizing the Clifford gates for a single hexon qubit and for the controlled-Pauli, W, and SWAP gates on two hexon qubits. A brute-force searched is performed with respect to a physically motivated example cost function. Tools and techniques are developed to aid in the compiling and optimization vii of measurement sequences. Utilizing the developed tools, we apply it towards the optimiza- tion of the stabilizer measurements for the surface code, an especially useful quantum error correcting code for the present MZM setting. Finally, we discuss adapting the technique of randomized benchmarking to the hexon setting, addressing simplifications and extensions that a hexon qubit can offer. viii Contents Curriculum Vitae vi Abstract vii 1 Introduction 1 2 Majoana Zero Modes in nanowires 6 2.1 Toy model . .7 2.2 Realizing MZMs . 12 2.2.1 Theoretical proposals . 13 2.2.2 Experimetnal progress . 15 2.3 MZM nanowires as qubits . 16 3 Optimal Clifford gate synthesis for MZM hexon qubits 22 3.1 Introduction . 23 3.2 Majorana Hexon Architecture . 27 3.2.1 Single-hexon state space and operators . 32 3.2.2 Single-qubit gates through measurements . 37 3.2.3 Multi-hexon operations . 40 3.2.4 Not all measurements are created equal . 48 3.2.5 Relabeling Majorana zero modes . 52 3.3 Forced-Measurement Methods . 55 3.3.1 Forced-measurement protocols for 2-MZM measurements . 56 3.3.2 Forced-measurement protocols involving 2N-MZM measurements . 61 3.3.3 Procrastination methods . 63 3.3.4 Adaptive methods . 68 3.4 Majorana-Pauli Tracking . 69 3.4.1 Proof of Majorana-Pauli tracking . 71 3.5 Brute-force Optimization of Measurement-Only Generation of Gates . 75 3.5.1 Optimization . 75 3.5.1.1 Majorana-Pauli tracking methods . 77 ix 3.5.1.2 Forced-measurement methods . 79 3.5.2 Gate search . 80 3.5.3 Demonstration of Methods . 84 3.5.4 Comparative Analysis . 87 3.6 Final Remarks . 89 4 Optimal stabilizer measurements for measurement-only MZM based surface code 91 4.1 Overview and motivation . 92 4.2 Measurement circuit and example compilation . 95 4.3 Circuit optimization . 102 4.4 Boundary circuits . 105 4.5 Interleaving . 106 5 Measurement-Only Randomized Benchmarking for MZM Hexon Qubits 113 5.1 Introduction . 114 5.2 Review . 115 5.2.1 Notation . 115 5.2.2 Randomized benchmarking . 116 5.3 Randomized benchmarking on a hexon . 120 5.4 Simulations . 131 5.5 Discussion . 134 A Optimal compilation tools and details 135 A.1 Example of Adaptive Forced-Measurement Protocol . 135 A.2 Sequence Morphology . 137 A.2.1 Some general formulas . 137 A.2.2 Sequence Morphology . 140 A.2.2.1 Space-time reflections . 141 A.2.2.2 Paulimorphism . 143 A.2.2.3 Sequence reduction . 147 A.3 Demonstration Details . 151 A.3.1 Two-Sided Hexon with Configuration h3; 4; 1; 2; 6; 5i .......... 151 A.3.2 One-Sided Hexon with Configuration h1; 2; 6; 3; 4; 5i .......... 157 A.3.3 One-Sided Hexon with Configuration h3; 4; 1; 2; 6; 5i .......... 164 B Optimal surface code details 172 B.1 Measurement sequences for an all-hexon surface code . 172 B.2 Optimal stabilizer measurement sequence . 174 Bibliography 190 x Chapter 1 Introduction Quantum computing is a paradigm for understanding and manipulating information at a more fundamental, quantum mechanical level [6, 29, 30, 67, 75] and has the potential to be a dis- ruptive, revolutionizing technology. Already, it has birthed new fields of study and connected previously disparate ones. It promises applications in efficient simulation of quantum sys- tems [42], cryptography [82], and general optimization tasks to name a few. These can for example aid in the design of novel drugs [91] or to the engineering of more efficient industrial processes, for instance in nitrogen fixation which accounts for on the order of 2% of world energy consumption [79]. In addition many quantum algorithms have been developed that are lower in complexity than any rival classical algorithm [7, 28, 82]. Efficient prime factor- ization is one such algorithm and it furthermore breaks many modern encryption schemes. This has necessitated the development of cryptographic channels secure even against quantum computers [8–10]. In addition, such quantum algorithms have also spurred the development 1 Introduction Chapter 1 of quantum inspired classical algorithms that perform exponentially better than previous it- erations [4, 85]. Notwithstanding, there are hopefully many yet unforseen possibilities and synergies to be discovered as was the case with the introduction of classical computing. As a result, quantum information and computing has grown significantly in recent years and has attracted interest and investments from almost all sectors, from academic institutions to star- tups and venture capital firms to established corporations and from governments all around the world. Quantum information is stored in quantum mechanical systems, the simplest of which are two-level systems known as qubits (quantum bits). Qubits are processed via quantum gates which are unitary operations acting on their Hilbert space. Output can be extracted from mea- suring qubits which give a binary, classical result. A system of N qubits has a 2N dimensional Hilbert space which requires 2N complex numbers to represent. Therefore, the resources re- quired to simulate a quantum mechanical system scales polynomially in the number of qubits versus exponentially in the number of bits. It is this key feature which naturally gives quan- tum computers an edge in simulating quantum systems. The computational power of quantum computers also leads to them being more error prone as well. In contrast to classical bits which are discrete, qubits can continuously interpolate between two basis states. Schematically, a classical bit is pinned to point from the center towards either the north or south pole of a globe while a qubit can point to any position 1.
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