A Photonic Quantum Gate Based on Electrically Controlled Strong Cavity Coupling Between a Single Nanocrystal Quantum Dot and an Ultra-High Q Silica Micro-Cavity
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The Future of Quantum Information Processing
SPECIALSECTION INTRODUCTION The Future of Quantum Information Processing IN A WORLD OVERWHELMED BY INCREASING AMOUNTS OF DATA, FINDING NEW WAYS to store and process information has become a necessity. Conventional silicon- based electronics has experienced rapid and steady growth, thanks to the progres- sive miniaturization of its basic component, the transistor, but that trend cannot continue indefi nitely. Quantum In conventional devices, information is stored and manipulated in binary form: The elementary components of these devices—the so-called bits—have Information two states, each of which encodes the binary 0 or 1. To move beyond the binary system, one can exploit the laws of quantum mechanics. A quantum-mechanical Processing object with two energy levels at its disposal can occupy either of those two levels, but also an arbitrary combination (“superposition”) of the two, much like an CONTENTS electron in a two-slit experiment can go through both slits at once. This results in infi nitely many quantum states that a single quantum bit, or “qubit,” can take; together with another strange property of quantum mechanics—entanglement— Reviews it allows for a much more powerful information platform than is possible with 1164 Scaling the Ion Trap Quantum conventional components. Processor Quantum information processing (QIP) uses qubits as its basic information C. Monroe and J. Kim units. QIP has many facets, from quantum simulation, to cryptography, to quantum 1169 Superconducting Circuits for computation, which is expected to solve problems more complex than those within Quantum Information: An Outlook the capabilities of conventional computers. To be useful for QIP, a qubit needs to be M. -
Fault-Tolerant Interface Between Quantum Memories and Quantum Processors
ARTICLE DOI: 10.1038/s41467-017-01418-2 OPEN Fault-tolerant interface between quantum memories and quantum processors Hendrik Poulsen Nautrup 1, Nicolai Friis 1,2 & Hans J. Briegel1 Topological error correction codes are promising candidates to protect quantum computa- tions from the deteriorating effects of noise. While some codes provide high noise thresholds suitable for robust quantum memories, others allow straightforward gate implementation 1234567890 needed for data processing. To exploit the particular advantages of different topological codes for fault-tolerant quantum computation, it is necessary to be able to switch between them. Here we propose a practical solution, subsystem lattice surgery, which requires only two-body nearest-neighbor interactions in a fixed layout in addition to the indispensable error correction. This method can be used for the fault-tolerant transfer of quantum information between arbitrary topological subsystem codes in two dimensions and beyond. In particular, it can be employed to create a simple interface, a quantum bus, between noise resilient surface code memories and flexible color code processors. 1 Institute for Theoretical Physics, University of Innsbruck, Technikerstr. 21a, 6020 Innsbruck, Austria. 2 Institute for Quantum Optics and Quantum Information, Austrian Academy of Sciences, Boltzmanngasse 3, 1090 Vienna, Austria. Correspondence and requests for materials should be addressed to H.P.N. (email: [email protected]) NATURE COMMUNICATIONS | 8: 1321 | DOI: 10.1038/s41467-017-01418-2 | www.nature.com/naturecommunications 1 ARTICLE NATURE COMMUNICATIONS | DOI: 10.1038/s41467-017-01418-2 oise and decoherence can be considered as the major encoding k = n − s qubits. We denote the normalizer of S by Nobstacles for large-scale quantum information processing. -
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. -
Cond-Mat.Supr-Con] 1 Sep 2004 Hnn B Lcutoso H W Ee Ytm Nteoxi the in Systems Level Two 1 the of Fluctuations (B) De Phonon
Decoherence of a Josephson qubit due to coupling to two level systems Li-Chung Ku and C. C. Yu Department of Physics, University of California, Irvine, California 92697, U.S.A. (Dated: October 30, 2018) Abstract Noise and decoherence are major obstacles to the implementation of Josephson junction qubits in quantum computing. Recent experiments suggest that two level systems (TLS) in the oxide tunnel barrier are a source of decoherence. We explore two decoherence mechanisms in which these two level systems lead to the decay of Rabi oscillations that result when Josephson junction qubits are subjected to strong microwave driving. (A) We consider a Josephson qubit coupled resonantly to a two level system, i.e., the qubit and TLS have equal energy splittings. As a result of this resonant interaction, the occupation probability of the excited state of the qubit exhibits beating. Decoherence of the qubit results when the two level system decays from its excited state by emitting a phonon. (B) Fluctuations of the two level systems in the oxide barrier produce fluctuations and 1/f noise in the Josephson junction critical current Io. This in turn leads to fluctuations in the qubit energy splitting that degrades the qubit coherence. We compare our results with experiments on Josephson junction phase qubits. PACS numbers: 03.65.Yz, 03.67.Lx, 85.25.Cp arXiv:cond-mat/0409006v1 [cond-mat.supr-con] 1 Sep 2004 1 I. INTRODUCTION The Josephson junction qubit is a leading candidate as a basic component of a quantum computer. A significant advantage of this approach is scalability, as these qubits may be readily fabricated in large numbers using integrated-circuit technology. -
High Energy Physics Quantum Information Science Awards Abstracts
High Energy Physics Quantum Information Science Awards Abstracts Towards Directional Detection of WIMP Dark Matter using Spectroscopy of Quantum Defects in Diamond Ronald Walsworth, David Phillips, and Alexander Sushkov Challenges and Opportunities in Noise‐Aware Implementations of Quantum Field Theories on Near‐Term Quantum Computing Hardware Raphael Pooser, Patrick Dreher, and Lex Kemper Quantum Sensors for Wide Band Axion Dark Matter Detection Peter S Barry, Andrew Sonnenschein, Clarence Chang, Jiansong Gao, Steve Kuhlmann, Noah Kurinsky, and Joel Ullom The Dark Matter Radio‐: A Quantum‐Enhanced Dark Matter Search Kent Irwin and Peter Graham Quantum Sensors for Light-field Dark Matter Searches Kent Irwin, Peter Graham, Alexander Sushkov, Dmitry Budke, and Derek Kimball The Geometry and Flow of Quantum Information: From Quantum Gravity to Quantum Technology Raphael Bousso1, Ehud Altman1, Ning Bao1, Patrick Hayden, Christopher Monroe, Yasunori Nomura1, Xiao‐Liang Qi, Monika Schleier‐Smith, Brian Swingle3, Norman Yao1, and Michael Zaletel Algebraic Approach Towards Quantum Information in Quantum Field Theory and Holography Daniel Harlow, Aram Harrow and Hong Liu Interplay of Quantum Information, Thermodynamics, and Gravity in the Early Universe Nishant Agarwal, Adolfo del Campo, Archana Kamal, and Sarah Shandera Quantum Computing for Neutrino‐nucleus Dynamics Joseph Carlson, Rajan Gupta, Andy C.N. Li, Gabriel Perdue, and Alessandro Roggero Quantum‐Enhanced Metrology with Trapped Ions for Fundamental Physics Salman Habib, Kaifeng Cui1, -
Pulsed Nuclear Magnetic Resonance
Pulsed Nuclear Magnetic Resonance Experiment NMR University of Florida | Department of Physics PHY4803L | Advanced Physics Laboratory References Theory C. P. Schlicter, Principles of Magnetic Res- Recall that the hydrogen nucleus consists of a onance, (Springer, Berlin, 2nd ed. 1978, single proton and no neutrons. The precession 3rd ed. 1990) of a bare proton in a magnetic field is a sim- ple consequence of the proton's intrinsic angu- E. Fukushima, S. B. W. Roeder, Experi- lar momentum and associated magnetic dipole mental Pulse NMR: A nuts and bolts ap- moment. A classical analog would be a gyro- proach, (Perseus Books, 1981) scope having a bar magnet along its rotational M. Sargent, M.O. Scully, W. Lamb, Laser axis. Having a magnetic moment, the proton Physics, (Addison Wesley, 1974). experiences a torque in a static magnetic field. Having angular momentum, it responds to the A. C. Melissinos, Experiments in Modern torque by precessing about the field direction. Physics, This behavior is called Larmor precession. The model of a proton as a spinning positive Introduction charge predicts a proton magnetic dipole mo- ment µ that is aligned with and proportional To observe nuclear magnetic resonance, the to its spin angular momentum s sample nuclei are first aligned in a strong mag- netic field. In this experiment, you will learn µ = γs (1) the techniques used in a pulsed nuclear mag- netic resonance apparatus (a) to perturb the where γ, called the gyromagnetic ratio, would nuclei out of alignment with the field and (b) depend on how the mass and charge is dis- to measure the small return signal as the mis- tributed within the proton. -
Semiclassical Approach to Atomic Decoherence by Gravitational Waves
Semiclassical approach to atomic decoherence by gravitational waves Diego A. Qui˜nones, Benjamin Varcoe August 2, 2018 Abstract A new heuristic model of interaction of an atomic system with a gravitational wave is proposed. In it, the gravitational wave alters the local electromagnetic field of the atomic nucleus, as perceived by the electron, changing the state of the system. The spectral decomposition of the wave function is calculated, from which the energy is obtained. The results suggest a shift in the difference of the atomic energy lev- els, which will induce a small detuning to a resonant transition. The detuning increases with the quantum numbers of the levels, making the effect more prominent for Rydberg states. We performed calcu- lations on the Rabi oscillations of atomic transitions, estimating how they would vary as a result of the proposed effect. 1 Introduction In general relativity, gravity is the curvature of the space-time continuum produced by the mass of objects [41]. Similar to how accelerating electrical charges produce electromagnetic waves, accelerating masses will produce rip- ples in the fabric of space-time [16, 17], which are called gravitational waves (GWs). They are predicted to exist in a very wide range of frequencies, de- pending on the source that generate them [2, 11, 14, 27, 29, 30, 37, 39, 40, 44], but even the most energetic ones (like the ones produced by rotating neutron stars [3]) will only produce a very small distortion of space, making them arXiv:1706.01287v3 [quant-ph] 1 Dec 2017 very hard to detect. Although GWs have been previously observed indirectly [43], it was only re- cently that a direct detection was performed by analyzing the signal of very big interferometers [18–20]. -
Waiting for the Quantum Bus Arxiv:1406.5674V1 [Quant-Ph] 22
Waiting for the Quantum Bus A.J. Bracken ∗ and G.F. Melloy School of of Mathematics and Physics The University of Queensland Brisbane, Australia 4072 Abstract Forty-five years after the discovery of the peculiar quantum effect known as `probability backflow', and twenty years after the greatest possible size of the effect was characterized, an experiment has been proposed recently to observe the effect in a Bose-Einstein condensate. Here the history is described in non-technical terms. arXiv:1406.5674v1 [quant-ph] 22 Jun 2014 ∗Email: [email protected] 1 Einstein's conviction that \God does not play at dice with the universe" is now generally seen as misguided. The quantum world, unlike our everyday classical world, is inherently probabilitistic in nature. But it may yet surprise the reader to learn that even in regard to probability itself, the quantum and classical worlds do not always behave in the same way. Forty-five years ago, British physicist G R Allcock published three papers [1], since widely-cited, on the so-called `arrival-time' problem in quantum me- chanics. This is the problem of determining the probability distribution over times at which a quantum particle may be observed at a given position. It is converse to a problem that quantum mechanics deals with routinely, namely to predict the probability distribution over positions at which a quantum par- ticle may be observed at a given time. The difference between the two looks so subtle as to be insignificant, but the arrival-time problem is by no means as straightforward as its counterpart, and it has led to continuing argument and research over many years [2, 3, 4]. -
Quantum Computing: Progress and Prospects (2018)
THE NATIONAL ACADEMIES PRESS This PDF is available at http://nap.edu/25196 SHARE Quantum Computing: Progress and Prospects (2018) DETAILS 202 pages | 6 x 9 | PAPERBACK ISBN 978-0-309-47969-1 | DOI 10.17226/25196 CONTRIBUTORS GET THIS BOOK Emily Grumbling and Mark Horowitz, Editors; Committee on Technical Assessment of the Feasibility and Implications of Quantum Computing; Computer Science and Telecommunications Board; Intelligence Community Studies Board; Division on FIND RELATED TITLES Engineering and Physical Sciences; National Academies of Sciences, Engineering, and Medicine SUGGESTED CITATION National Academies of Sciences, Engineering, and Medicine 2018. Quantum Computing: Progress and Prospects. Washington, DC: The National Academies Press. https://doi.org/10.17226/25196. Visit the National Academies Press at NAP.edu and login or register to get: – Access to free PDF downloads of thousands of scientific reports – 10% off the price of print titles – Email or social media notifications of new titles related to your interests – Special offers and discounts Distribution, posting, or copying of this PDF is strictly prohibited without written permission of the National Academies Press. (Request Permission) Unless otherwise indicated, all materials in this PDF are copyrighted by the National Academy of Sciences. Copyright © National Academy of Sciences. All rights reserved. Quantum Computing: Progress and Prospects PREPUBLICATION COPY – SUBJECT TO FURTHER EDITORIAL CORRECTION Quantum Computing: Progress and Prospects Emily Grumbling and Mark Horowitz, Editors Committee on Technical Assessment of the Feasibility and Implications of Quantum Computing Computer Science and Telecommunications Board Intelligence Community Studies Board Division on Engineering and Physical Sciences A Consensus Study Report of PREPUBLICATION COPY – SUBJECT TO FURTHER EDITORIAL CORRECTION Copyright National Academy of Sciences. -
Synthesis of Quantum-Logic Circuits Vivek V
1000 IEEE TRANSACTIONS ON COMPUTER-AIDED DESIGN OF INTEGRATED CIRCUITS AND SYSTEMS, VOL. 25, NO. 6, 2006 Synthesis of Quantum-Logic Circuits Vivek V. Shende, Stephen S. Bullock, and Igor L. Markov, Senior Member, IEEE Abstract—The pressure of fundamental limits on classical com- I. INTRODUCTION putation and the promise of exponential speedups from quantum effects have recently brought quantum circuits (Proc. R. Soc. S THE ever-shrinking transistor approaches atomic pro- Lond. A, Math. Phys. Sci., vol. 425, p. 73, 1989) to the atten- A portions, Moore’s law must confront the small-scale tion of the electronic design automation community (Proc. 40th granularity of the world: We cannot build wires thinner than ACM/IEEE Design Automation Conf., 2003), (Phys.Rev.A,At.Mol. atoms. Worse still, at atomic dimensions, we must contend with Opt. Phy., vol. 68, p. 012318, 2003), (Proc. 41st Design Automation Conf., 2004), (Proc. 39th Design Automation Conf., 2002), (Proc. the laws of quantum mechanics. For example, suppose 1 bit Design, Automation, and Test Eur., 2004), (Phys. Rev. A, At. Mol. is encoded as the presence or the absence of an electron in a Opt. Phy., vol. 69, p. 062321, 2004), (IEEE Trans. Comput.-Aided small region.1 Since we know very precisely where the electron Des. Integr. Circuits Syst., vol. 22, p. 710, 2003). Efficient quantum– is located, the Heisenberg uncertainty principle dictates that logic circuits that perform two tasks are discussed: 1) implement- we cannot know its momentum with high accuracy. Without ing generic quantum computations, and 2) initializing quantum registers. In contrast to conventional computing, the latter task a reasonable upper bound on the electron’s momentum, there is nontrivial because the state space of an n-qubit register is not is no alternative but to use a large potential to keep it in place, finite and contains exponential superpositions of classical bit- and expend significant energy during logic switching. -
Arxiv:2010.08699V1 [Quant-Ph] 17 Oct 2020 Tum Computation Systems
Bosonic quantum error correction codes in superconducting quantum circuits 1, 1, 1, 2,† 1,‡ W. Cai, ∗ Y. Ma, ∗ W. Wang, ∗ C.-L. Zou, and L. Sun 1Center for Quantum Information, Institute for Interdisciplinary Information Sciences, Tsinghua University, Beijing 100084, China 2Key Laboratory of Quantum Information, CAS, University of Science and Technology of China, Hefei, Anhui 230026, P. R. China Quantum information is vulnerable to environmental noise and experimental imperfections, hindering the reliability of practical quantum information processors. Therefore, quantum error correction (QEC) that can protect quantum information against noise is vital for universal and scalable quantum compu- tation. Among many different experimental platforms, superconducting quantum circuits and bosonic encodings in superconducting microwave modes are appealing for their unprecedented potential in QEC. During the last few years, bosonic QEC is demonstrated to reach the break-even point, i.e. the lifetime of a logical qubit is enhanced to exceed that of any individual components composing the experimen- tal system. Beyond that, universal gate sets and fault-tolerant operations on the bosonic codes are also realized, pushing quantum information processing towards the QEC era. In this article, we review the recent progress of the bosonic codes, including the Gottesman-Kitaev-Preskill codes, cat codes, and bino- mial codes, and discuss the opportunities of bosonic codes in various quantum applications, ranging from fault-tolerant quantum computation to quantum metrology. We also summarize the challenges associated with the bosonic codes and provide an outlook for the potential research directions in the long terms. I. INTRODUCTION grees of freedom, e.g. spatial, temporal, frequency, polar- ization, or their combinations, and thus are scalable. -
Spin Chain Systems for Quantum Computing and Quantum Information Applications
Spin Chain Systems for Quantum Computing and Quantum Information Applications MARTA P. ESTARELLAS PHD UNIVERSITY OF YORK Physics April, 2018 3 University of York Abstract York Center for Quantum Technologies Department of Physics Doctor of Philosophy Spin Chain Systems for Quantum Computing and Quantum Information Applications by Marta P. ESTARELLAS One of the most essential processes in classical computation is that related to the information manipulation; each component or register of a computer needs to com- municate to others by exchanging information encoded in bits and transforming it through logical operations. Hence the theoretical study of methods for informa- tion transfer and processing in classical information theory is of fundamental impor- tance for telecommunications and computer science, along with study of errors and robustness of such proposals. When adding the quantum ingredient, there arises a whole new set of paradigms and devices, based on manipulations of qubits, the quantum analogues of conventional data bits. Such systems can show enormous advantage against their classical analogues, but at the same time present a whole new set of technical and conceptual challenges to overcome. The full and detailed understanding of quantum processes and studies of theoretical models and devices therefore provide the first logical steps to the future technological exploitation of these new machines. In this line, this thesis focuses on spin chains as such theoreti- cal models, formed by series of coupled qubits that can be applied to a wide range of physical systems, and its several potential applications as quantum devices. In this work spin chains are presented as reliable devices for quantum communication with high transfer fidelities, entanglement generation and distribution over distant par- ties and protected storage of quantum information.