Quantum Transport in Solid State Devices for Terahertz Frequency Applications
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Quantum Chance Nicolas Gisin
Quantum Chance Nicolas Gisin Quantum Chance Nonlocality, Teleportation and Other Quantum Marvels Nicolas Gisin Department of Physics University of Geneva Geneva Switzerland ISBN 978-3-319-05472-8 ISBN 978-3-319-05473-5 (eBook) DOI 10.1007/978-3-319-05473-5 Springer Cham Heidelberg New York Dordrecht London Library of Congress Control Number: 2014944813 Translated by Stephen Lyle L’impensable Hasard. Non-localité, téléportation et autres merveilles quantiques Original French edition published by © ODILE JACOB, Paris, 2012 © Springer International Publishing Switzerland 2014 This work is subject to copyright. All rights are reserved by the Publisher, whether the whole or part of the material is concerned, specifically the rights of translation, reprinting, reuse of illustrations, recitation, broadcasting, reproduction on microfilms or in any other physical way, and transmission or information storage and retrieval, electronic adaptation, computer software, or by similar or dissimilar methodology now known or hereafter developed. Exempted from this legal reservation are brief excerpts in connection with reviews or scholarly analysis or material supplied specifically for the purpose of being entered and executed on a computer system, for exclusive use by the purchaser of the work. Duplication of this publication or parts thereof is permitted only under the provisions of the Copyright Law of the Publisher’s location, in its current version, and permission for use must always be obtained from Springer. Permissions for use may be obtained through RightsLink at the Copyright Clearance Center. Violations are liable to prosecution under the respective Copyright Law. The use of general descriptive names, registered names, trademarks, service marks, etc. -
Mathematical Languages Shape Our Understanding of Time in Physics Physics Is Formulated in Terms of Timeless, Axiomatic Mathematics
comment Corrected: Publisher Correction Mathematical languages shape our understanding of time in physics Physics is formulated in terms of timeless, axiomatic mathematics. A formulation on the basis of intuitionist mathematics, built on time-evolving processes, would ofer a perspective that is closer to our experience of physical reality. Nicolas Gisin n 1922 Albert Einstein, the physicist, met in Paris Henri Bergson, the philosopher. IThe two giants debated publicly about time and Einstein concluded with his famous statement: “There is no such thing as the time of the philosopher”. Around the same time, and equally dramatically, mathematicians were debating how to describe the continuum (Fig. 1). The famous German mathematician David Hilbert was promoting formalized mathematics, in which every real number with its infinite series of digits is a completed individual object. On the other side the Dutch mathematician, Luitzen Egbertus Jan Brouwer, was defending the view that each point on the line should be represented as a never-ending process that develops in time, a view known as intuitionistic mathematics (Box 1). Although Brouwer was backed-up by a few well-known figures, like Hermann Weyl 1 and Kurt Gödel2, Hilbert and his supporters clearly won that second debate. Hence, time was expulsed from mathematics and mathematical objects Fig. 1 | Debating mathematicians. David Hilbert (left), supporter of axiomatic mathematics. L. E. J. came to be seen as existing in some Brouwer (right), proposer of intuitionist mathematics. Credit: Left: INTERFOTO / Alamy Stock Photo; idealized Platonistic world. right: reprinted with permission from ref. 18, Springer These two debates had a huge impact on physics. -
Quantum Trajectory Theory of Open Cavity-QED Systems with a Time Delayed Coherent Optical Feedback
Quantum trajectory theory of open cavity-QED systems with a time delayed coherent optical feedback by Gavin Crowder A thesis submitted to the Department of Physics, Engineering Physics & Astronomy in conformity with the requirements for the degree of Master of Science Queen's University Kingston, Ontario, Canada May 2020 Copyright © Gavin Crowder, 2020 Abstract The emergence of integrated (or solid state) photonic systems, including quantum dots, waveguides, and cavities, has provided a base to harness quantum optic phenom- ena for use in current and future quantum technologies. These systems also provide opportunities for exploring fundamentally new regimes in quantum optics. In order to fully realize the potential of these systems, many figures of merit need to be improved, for example by increasing the stability and coherent lifetimes of these systems. Fol- lowing the notable improvements using measurement-based feedback, time-delayed coherent optical feedback has been proposed as one such method of stabilizing and improving these systems. Furthermore, modelling coherent feedback itself presents an interesting fundamental problem due to its non-Markovian nature. In this thesis, we use quantum trajectory (QT) theory to derive two models for simulating cavity quantum electrodynamic (cavity-QED) systems with time-delayed coherent feedback. First, an explanation of QT theory is given and the related time discretized waveguide (TDW) model is derived. Next we present a model for feedback using the frequency modes of the waveguide and results are presented in the \one photon in the loop" approximation. We demonstrate how the photon lifetime can be improved in typical cavity-QED with coherent feedback and we explore some nonlinear effects. -
Violations of Locality and Free Choice Are Equivalent Resources in Bell Experiments
For published version see PNAS 118 (17) e2020569118 (2021) Violations of locality and free choice are equivalent resources in Bell experiments Pawel Blasiaka,b,1, Emmanuel M. Pothosb, James M. Yearsleyb, Christoph Gallusc, and Ewa Borsuka aInstitute of Nuclear Physics Polish Academy of Sciences, PL-31342 Krakow, Poland; bCity, University of London, London EC1V 0HB, United Kingdom; cTechnische Hochschule Mittelhessen, D-35390 Gießen, Germany Bell inequalities rest on three fundamental assumptions: realism, lo- Surprisingly, nature violates Bell inequalities (8–15) which cality, and free choice, which lead to nontrivial constraints on cor- means that if the standard causal (or realist) picture is to be relations in very simple experiments. If we retain realism, then vio- maintained at least one of the remaining two assumptions, that lation of the inequalities implies that at least one of the remaining is locality or free choice, has to fail. It turns out that rejecting two assumptions must fail, which can have profound consequences just one of those two assumptions is always enough to explain for the causal explanation of the experiment. We investigate the ex- the observed correlations, while maintaining consistency with tent to which a given assumption needs to be relaxed for the other the causal structure imposed by the other. Either option poses to hold at all costs, based on the observation that a violation need a challenge to deep-rooted intuitions about reality, with a not occur on every experimental trial, even when describing corre- full range of viable positions open to serious philosophical lations violating Bell inequalities. How often this needs to be the dispute (16–18). -
PHYSICS at ARKANSAS Discharge Tubes Were Used
8. Doctoral Program and Graduate Research by Raymond H. Hughes and Paul C. Sharrah second group of programs. These included ani- mal sciences, botany and bacteriology, compara- First Doctoral Programs tive literature, physics, psychology, zoology, and Under the Presidency of Lewis Webster Jones engineering. In the next few years doctoral pro- in 1949 it was determined that it was time to grams were approved also for business adminis- initiate doctoral programs within the graduate tration, agronomy, anatomy, microbiology, school. (Ref. 3, p. 233) instrumental sciences (at the Graduate Institute The newly appointed graduate dean, Dr. Virgil of Technology in Little Rock), and mathematics. W. Adkisson, was instructed to proceed carefully A third significant expansion was authorized but ambitiously in 1970. These programs were history, plant with this program. pathology, and entomology. These last two pro- The departments, grams were implemented after reaccreditation as a starter, were and improved funding had been provided. to offer a better The graduate school enrollment in 1948 had selection of ad- been 272 students (Ref. 2, p. 159) but had risen vanced undergrad- to 1,659 by spring 1971 (Ref. 3, p. 234). By fall uate courses as 1993 there were a total of about 35 clearly deemed appropri- defined doctoral programs on the Fayetteville ate! Physics, for campus and a graduate school enrollment figure example, decided of 2,150 students. (Information courtesy in the early Professor David W. Hart, Associate Dean, 1 9 5 0 ’s, to require Graduate School.) Forty-four years of progress a thesis for the since that day in 1949 when it was decided to M.S. -
Quantum Trajectories of a Superconducting Qubit
Quantum Trajectories of a Superconducting Qubit By Steven Joseph Weber A dissertation submitted in partial satisfaction of the requirements for the degree of Doctor of Philosophy in Physics in the Graduate Division of the University of California, Berkeley Committee in charge: Irfan Siddiqi, Chair John Clarke Sayeef Salahuddin Fall 2014 Quantum Trajectories of a Superconducting Qubit Copyright 2014 by Steven Joseph Weber 1 Abstract Quantum Trajectories of a Superconducting Qubit by Steven Joseph Weber Doctor of Philosophy in Physics University of California, Berkeley Irfan Siddiqi, Chair In quantum mechanics, the process of measurement is intrinsically probabilistic. As a result, continuously monitoring a quantum system will randomly perturb its natural unitary evolution. An accurate measurement record documents this stochastic evolution and can be used to reconstruct the quantum trajectory of the system state in a single experimen- tal iteration. We use weak measurements to track the individual quantum trajectories of a superconducting qubit that evolves under the competing influences of continuous weak measurement and Rabi drive. We analyze large ensembles of such trajectories to examine their characteristics and determine their statistical properties. For example, by considering only the subset of trajectories that evolve between any chosen initial and final states, we can deduce the most probable path through quantum state space. Our investigation reveals the rich interplay between measurement dynamics, typically associated with wavefunction -
Quant-Ph/0512168V1 20 Dec 2005 Uly M Fcus,Ntwiigfrenti,Btfor Ac- Sub- the Well, but Somewhat of Einstein, (Necessarily [2])
Can relativity be considered complete ? From Newtonian nonlocality to quantum nonlocality and beyond Nicolas Gisin Group of Applied Physics, University of Geneva, 1211 Geneva 4, Switzerland (Dated: October 31, 2018) We review the long history of nonlocality in physics with special emphasis on the conceptual breakthroughs over the last few years. For the first time it is possible to study ”nonlocality without signaling” from the outside, that is without all the quantum physics Hilbert space artillery. We emphasize that physics has always given a nonlocal description of Nature, except during a short 10 years gap. We note that the very concept of ”nonlocality without signaling” is totally foreign to the spirit of relativity, the only strictly local theory. PACS numbers: I. INTRODUCTION in his rejection of nonlocality! However, most physicists didn’t pay much attention to this aspect of Newtonian 100 years after Einstein miraculous year and 70 years physics. By lack of alternative, physics remained nonlo- after the EPR paper [1], I like to think that Einstein cal until about 1915 when Einstein introduced the world would have appreciated the somewhat provocative title to General Relativity. But let’s start ten years earlier, in of this contribution. However, Einstein would probably 1905. not have liked its conclusion. But who can doubt that relativity is incomplete? and likewise that quantum me- chanics is incomplete! Indeed, these are two scientific III. EINSTEIN, THE GREATEST theories and Science is nowhere near its end (as a matter MECHANICAL ENGINEER of fact, I do believe that there is no end [2]). Well, ac- tually, I am, of course, not writing for Einstein, but for In 1905 Einstein introduced three radically new the- those readers interested in a (necessarily somewhat sub- ories or models in physics. -
Quantum Cryptography: Where Do We Stand?
Quantum Cryptography: where do we stand? Nicolas Gisin Group of Applied Physics University of Geneva - Switzerland In the last few years the world in which Quantum Cryptography evolves has deeply changed. On the one side the revelations of Snowden, though he said nothing really new, made the world more aware of the importance to protect sensitive data from all kinds of adversaries, including sometimes “friends”. On the other side, breakthroughs in quantum computation, in particular in superconducting qubits and surface-codes, made it possible that in 15 to 25 years there might be a quantum machine able to break today’s codes. This implies that in order to protect today’s data over a few decades, one has to act now and use some quantum-safe cryptography. Such a perspective is taken very seriously by the cryptography community who is looking for a quantum-safe alternative to today’s systems. Quantum-safe cryptography covers all cryptography systems that resist to quantum attacks. As in today’s cryptography, this covers both complexity-based protocols and provably secure systems. The first ones consists in merely replacing the problem on which RSA rests (i.e. factoring) by another problem claimed to be intractable both for classical and for quantum computers, as factoring was claimed to be intractable. This approach has the great advantage of being flexible, cost-effective and relatively similar to today’s approach, hence security experts don’t need to change much. But it has the great drawback that one is again betting on the unknown to secure our information-based society. -
Prizes 2012 Editor’S Note Inside Ian T
The Quantum Volume 7, Number 1 Times Second Half, 2012 Newsletter of the Topical Group s・p・e・c・i・a・l i・s・s・u・e on Quantum Information American Physical Society Prizes 2012 Editor’s Note Inside Ian T. Durham In what could be viewed as a watershed moment for p. 2 Nobel laureate profiles quantum information, foundations, and computation, this year’s Nobel Prize has been p. 5 FQXi large grant, “Physics of awarded to two of our field’s experimental pioneers: Serge Haroche of Collège de France and École Information” initial inquiry Normale Supérieure, both in Paris, and David (deadline January 16, 2013) Wineland of the National Institute of Standards and Technology (NIST) in Boulder, Colorado. In honor of both Serge and Dave, we have commissioned p. 6 FQXi honorees in quantum profiles on each from people who know them well, information both on a professional and a personal level. There were several other recent awards and recognitions given to members of the quantum p. 7 Letter from Incoming Chair information community including the addition of Daniel Lidar four APS fellows under the GQI banner and Rob Spekkens’ First Prize in the FQXi Essay Contest. We highlight those on subsequent pages and include p. 8 New APS GQI Fellows the latest FQXi Large Grant RFP which is specifically aimed at the physics of information. On a more practical note, this issue also p. 8 GQI Elections (deadline includes information on the current GQI election. January 17, 2013) Biographies and candidate statements for the Vice Chair and Member-at-Large positions begin on p. -
Non-Locality of Experimental Qutrit Pairs 2
Non-Locality of Experimental Qutrit Pairs C Bernhard†, B Bessire†, A Montina∗, M Pfaffhauser∗, A Stefanov†, S Wolf∗ † Institute of Applied Physics, University of Bern, Bern, Switzerland. ∗ Faculty of Informatics, USI Lugano, Switzerland. Abstract. The insight due to John Bell that the joint behavior of individually measured entangled quantum systems cannot be explained by shared information remains a mystery to this day. We describe an experiment, and its analysis, displaying non-locality of entangled qutrit pairs. The non-locality of such systems, as compared to qubit pairs, is of particular interest since it potentially opens the door for tests of bipartite non-local behavior independent of probabilistic Bell inequalities, but of deterministic nature. 1. Non-Locality in Theory ... The discovery of John Bell that nature was non-local and quantum physics cannot be embedded into a local realistic theory in which the outcomes of experiments are completely determined by values located where the experiment actually takes place, and no far-away variables, is profound. It probably poses more questions than it has solved: If shared classical information [4] as well as hidden communication [3] both fall short of explaining non-local correlations, what “mechanism” could possibly be behind this strange effect? What can we learn from Bell’s insight — and from the series of experiments carried out in the aftermath [18, 2, 28, 30] — about the nature of space and time? What can we conclude about free choices (randomness) and, more generally, the role of information in physics and in our understanding of natural laws? In fact, Bell’s theorem is an information-theoretic statement: It characterizes what kind of joint input-output behavior P (ab xy) | arXiv:1402.5026v1 [quant-ph] 20 Feb 2014 can in principle be explained by shared (classical) information R, i.e., is of the form r r PR(r)P (a x)P (b y) , r | | X and which cannot. -
Experiments with Entangled Photons
Experiments with Entangled Photons Bell Inequalities, Non-local Games and Bound Entanglement Muhammad Sadiq Thesis for the degree of Doctor of Philosophy in Physics Department of Physics Stockholm University Sweden. c Muhammad Sadiq, Stockholm 2016 c American Physical Society. (papers) c Macmillan Publishers Limited. (papers) ISBN 978-91-7649-358-8 Printed in Sweden by Holmbergs, Malmö 2016. Distributor: Department of Physics, Stockholm University. Abstract Quantum mechanics is undoubtedly a weird field of science, which violates many deep conceptual tenets of classical physics, requiring reconsideration of the concepts on which classical physics is based. For instance, it permits per- sistent correlations between classically separated systems, that are termed as entanglement. To circumvent these problems and explain entanglement, hid- den variables theories–based on undiscovered parameters–have been devised. However, John S. Bell and others invented inequalities that can distinguish be- tween the predictions of local hidden variable (LHV) theories and quantum mechanics. The CHSH-inequality (formulated by J. Clauser, M. Horne, A. Shimony and R. A. Holt), is one of the most famous among these inequalities. In the present work, we found that this inequality actually contains an even simpler logical structure, which can itself be described by an inequality and will be violated by quantum mechanics. We found 3 simpler inequalities and were able to violate them experimentally. Furthermore, the CHSH inequality can be used to devise games that can outperform classical strategies. We explore CHSH-games for biased and un- biased cases and present their experimental realizations. We also found a re- markable application of CHSH-games in real life, namely in the card game of duplicate Bridge. -
Quantum Communication Jubilee of Teleportation
Quantum Communication Quantum • Rotem Liss and Tal Mor Liss • Rotem and Tal Quantum Communication Celebrating the Silver Jubilee of Teleportation Edited by Rotem Liss and Tal Mor Printed Edition of the Special Issue Published in Entropy www.mdpi.com/journal/entropy Quantum Communication—Celebrating the Silver Jubilee of Teleportation Quantum Communication—Celebrating the Silver Jubilee of Teleportation Editors Rotem Liss Tal Mor MDPI • Basel • Beijing • Wuhan • Barcelona • Belgrade • Manchester • Tokyo • Cluj • Tianjin Editors Rotem Liss Tal Mor Technion–Israel Institute of Technology Technion–Israel Institute of Technology Israel Israel Editorial Office MDPI St. Alban-Anlage 66 4052 Basel, Switzerland This is a reprint of articles from the Special Issue published online in the open access journal Entropy (ISSN 1099-4300) (available at: https://www.mdpi.com/journal/entropy/special issues/Quantum Communication). For citation purposes, cite each article independently as indicated on the article page online and as indicated below: LastName, A.A.; LastName, B.B.; LastName, C.C. Article Title. Journal Name Year, Article Number, Page Range. ISBN 978-3-03943-026-0 (Hbk) ISBN 978-3-03943-027-7 (PDF) c 2020 by the authors. Articles in this book are Open Access and distributed under the Creative Commons Attribution (CC BY) license, which allows users to download, copy and build upon published articles, as long as the author and publisher are properly credited, which ensures maximum dissemination and a wider impact of our publications. The book as a whole is distributed by MDPI under the terms and conditions of the Creative Commons license CC BY-NC-ND. Contents About the Editors .............................................