Beyond the Quantum
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Marie Curie and Her Time
Marie Curie and Her Time by Hélène Langevin-Joliot to pass our lives near each other hypnotized by our dreams, your patriotic dream, our humanitarian dream, arie Curie (1867–1934) belongs to that exclu- and our scientific dream.” sive group of women whose worldwide rec- Frederick Soddy wrote about Marie that she was Mognition and fame have endured for a century “the most beautiful discovery of Pierre Curie.” Of or more. She was indeed one of the major agents of course, it might also be said that Pierre Curie was the scientific revolution which allowed experimen- “the most beautiful discovery of Marie Skłodowska.” tal investigation to extend beyond the macroscopic It is difficult to imagine more contrasting personali- world. Her work placed the first stone in the founda- ties than those of Pierre and of Marie. In spite of that, tion of a new discipline: radiochemistry. And Curie’s or because of that, they complemented each other achievements are even more remarkable since they astonishingly well. Pierre was as dreamy as Marie was occurred in the field of science, an intellectual activ- organized. At the same time, they shared similar ideas ity traditionally forbidden to women. However, these about family and society. accomplishments alone don’t seem to fully explain the near mythic status of Marie Curie today. One hundred years ago, she was often considered to be just an assistant to her husband. Perhaps the reason her name still resonates is because of the compelling story of her life and her intriguing personality. The Most Beautiful Discovery of Pierre Curie The story of the young Maria Skłodowska leaving In this iconic photograph of participants at the Fifth her native Poland to pursue upper-level studies in Solvay Conference in 1927, Marie Curie is third from Paris sounds like something out of a novel. -
Quantum Theory at the Crossroads : Reconsidering the 1927 Solvay
QUANTUM THEORY AT THE CROSSROADS Reconsidering the 1927 Solvay Conference GUIDO BACCIAGALUPPI ANTONY VALENTINI 8 CAMBRIDGE ::: UNIVERSITY PRESS Contents List of illustrations page xii Preface xv Abbreviations xxi Typographic conventions xxiii Note on the bibliography and the index xxiii Permissions and copyright notices xxiii Part I Perspectives on the 1927 Solvay conference 1 Historical introduction 3 1.1 Ernest Solvay and the Institute of Physics 3 1.2 War and international relations 6 1.3 Scientific planning and background 8 1.4 Further details of planning 15 1.5 The Solvay meeting 18 1.6 The editing of the proceedings 20 1. 7 Conclusion 21 Archival notes 23 2 De Broglie's pilot-wave theory 27 2.1 Background 27 2.2 A new approach to particle dynamics: 1923-1924 33 2.2.1 First papers on pilot-wave theory (1923) 34 2.2.2 Thesis (1924) 39 2.2.3 Optical interference fringes: November 1924 49 2.3 Towards a complete pilot-wave dynamics: 1925-1927 51 2.3.1 'Structure': Journal de Physique, May 1927 55 2.3.2 Significance of de Broglie's 'Structure' paper 65 vii viii Contents 2.4 1927 Solvay report: the new dynamics of quanta 67 2.5 Significance of de Broglie's work from 1923 to 1927 76 Archival notes 79 3 From matrix mechanics to quantum mechanics 80 3.1 Summary of Born and Heisenberg's report 81 3.2 Writing of the report 84 3.3 Formalism 85 3.3.1 Before matrix mechanics 85 3.3.2 Matrix mechanics 86 3.3.3 Formal extensions of matrix mechanics 90 3.4 Interpretation 92 3.4.1 Matrix mechanics, Born and Wiener 93 3.4.2 Born and Jordan on guiding -
Lecture Notes in Physics
Lecture Notes in Physics Editorial Board R. Beig, Wien, Austria J. Ehlers, Potsdam, Germany U. Frisch, Nice, France K. Hepp, Zurich,¨ Switzerland W. Hillebrandt, Garching, Germany D. Imboden, Zurich,¨ Switzerland R. L. Jaffe, Cambridge, MA, USA R. Kippenhahn, Gottingen,¨ Germany R. Lipowsky, Golm, Germany H. v. Lohneysen,¨ Karlsruhe, Germany I. Ojima, Kyoto, Japan H. A. Weidenmuller,¨ Heidelberg, Germany J. Wess, Munchen,¨ Germany J. Zittartz, Koln,¨ Germany 3 Berlin Heidelberg New York Barcelona Hong Kong London Milan Paris Singapore Tokyo Editorial Policy The series Lecture Notes in Physics (LNP), founded in 1969, reports new developments in physics research and teaching -- quickly, informally but with a high quality. Manuscripts to be considered for publication are topical volumes consisting of a limited number of contributions, carefully edited and closely related to each other. Each contribution should contain at least partly original and previously unpublished material, be written in a clear, pedagogical style and aimed at a broader readership, especially graduate students and nonspecialist researchers wishing to familiarize themselves with the topic concerned. For this reason, traditional proceedings cannot be considered for this series though volumes to appear in this series are often based on material presented at conferences, workshops and schools (in exceptional cases the original papers and/or those not included in the printed book may be added on an accompanying CD ROM, together with the abstracts of posters and other material suitable for publication, e.g. large tables, colour pictures, program codes, etc.). Acceptance Aprojectcanonlybeacceptedtentativelyforpublication,byboththeeditorialboardandthe publisher, following thorough examination of the material submitted. The book proposal sent to the publisher should consist at least of a preliminary table of contents outlining the structureofthebooktogetherwithabstractsofallcontributionstobeincluded. -
Dynamical Relaxation to Quantum Equilibrium
Dynamical relaxation to quantum equilibrium Or, an account of Mike's attempt to write an entirely new computer code that doesn't do quantum Monte Carlo for the first time in years. ESDG, 10th February 2010 Mike Towler TCM Group, Cavendish Laboratory, University of Cambridge www.tcm.phy.cam.ac.uk/∼mdt26 and www.vallico.net/tti/tti.html [email protected] { Typeset by FoilTEX { 1 What I talked about a month ago (`Exchange, antisymmetry and Pauli repulsion', ESDG Jan 13th 2010) I showed that (1) the assumption that fermions are point particles with a continuous objective existence, and (2) the equations of non-relativistic QM, allow us to deduce: • ..that a mathematically well-defined ‘fifth force', non-local in character, appears to act on the particles and causes their trajectories to differ from the classical ones. • ..that this force appears to have its origin in an objectively-existing `wave field’ mathematically represented by the usual QM wave function. • ..that indistinguishability arguments are invalid under these assumptions; rather antisymmetrization implies the introduction of forces between particles. • ..the nature of spin. • ..that the action of the force prevents two fermions from coming into close proximity when `their spins are the same', and that in general, this mechanism prevents fermions from occupying the same quantum state. This is a readily understandable causal explanation for the Exclusion principle and for its otherwise inexplicable consequences such as `degeneracy pressure' in a white dwarf star. Furthermore, if assume antisymmetry of wave field not fundamental but develops naturally over the course of time, then can see character of reason for fermionic wave functions having symmetry behaviour they do. -
Signal-Locality in Hidden-Variables Theories
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server Signal-Locality in Hidden-Variables Theories Antony Valentini1 Theoretical Physics Group, Blackett Laboratory, Imperial College, Prince Consort Road, London SW7 2BZ, England.2 Center for Gravitational Physics and Geometry, Department of Physics, The Pennsylvania State University, University Park, PA 16802, USA. Augustus College, 14 Augustus Road, London SW19 6LN, England.3 We prove that all deterministic hidden-variables theories, that reproduce quantum theory for an ‘equilibrium’ distribution of hidden variables, give in- stantaneous signals at the statistical level for hypothetical ‘nonequilibrium en- sembles’. This generalises another property of de Broglie-Bohm theory. Assum- ing a certain symmetry, we derive a lower bound on the (equilibrium) fraction of outcomes at one wing of an EPR-experiment that change in response to a shift in the distant angular setting. We argue that the universe is in a special state of statistical equilibrium that hides nonlocality. PACS: 03.65.Ud; 03.65.Ta 1email: [email protected] 2Corresponding address. 3Permanent address. 1 Introduction: Bell’s theorem shows that, with reasonable assumptions, any deterministic hidden-variables theory behind quantum mechanics has to be non- local [1]. Specifically, for pairs of spin-1/2 particles in the singlet state, the outcomes of spin measurements at each wing must depend instantaneously on the axis of measurement at the other, distant wing. In this paper we show that the underlying nonlocality becomes visible at the statistical level for hypothet- ical ensembles whose distribution differs from that of quantum theory. -
The Age of Chance Reserved for the Winning Side of the Struggle
BOOKS & ARTS NATURE|Vol 446|22 March 2007 unfortunately, that Lindley’s perceptive and sympathetic treatment of ideas and figures is The age of chance reserved for the winning side of the struggle. He marginalizes Einstein’s concerns by pre- Uncertainty: Einstein, Heisenberg, Bohr, posal for a radically non-newtonian dynamic senting him as a young revolutionary turned and the Struggle for the Soul of Science theory in which particles followed trajectories old reactionary. Lindley keeps returning to by David Lindley determined by an associated wave. De Bro- Einstein’s desire for causality, while down- Doubleday: 2007. 272 pp. $26 glie showed how this could account for basic playing Einstein’s equally strong insistence that interference phenomena (as waves) as well as physics, causal or not, should deal with nature Arthur Fine quantized energy (as particles). That drew it to itself, not just our observations. The author In Uncertainty, David Lindley tells the intrigu- the attention of Einstein and Schrödinger, who also overlooks Einstein’s radical critique of the ing tale of how Albert Einstein, Werner found the ideas promising, and to Heisenberg, classical, physical concepts used in quantum Heisenberg and Niels Bohr (among others) Pauli and Bohr, who felt threatened by them. theory, as well as his programme for develop- struggled to create and understand the new But de Broglie lacked a general treatment of ing new concepts, and his eventual openness quantum physics. Lindley organizes his tale the waves that guided his particles, and that is to an algebraic, rather than a spatiotemporal, around the issue of indeterminism, which Max where wave mechanics comes in. -
Quantum Computing in the De Broglie-Bohm Pilot-Wave Picture
Quantum Computing in the de Broglie-Bohm Pilot-Wave Picture Philipp Roser September 2010 Blackett Laboratory Imperial College London Submitted in partial fulfilment of the requirements for the degree of Master of Science of Imperial College London Supervisor: Dr. Antony Valentini Internal Supervisor: Prof. Jonathan Halliwell Abstract Much attention has been drawn to quantum computing and the expo- nential speed-up in computation the technology would be able to provide. Various claims have been made about what aspect of quantum mechan- ics causes this speed-up. Formulations of quantum computing have tradi- tionally been made in orthodox (Copenhagen) and sometimes many-worlds quantum mechanics. We will aim to understand quantum computing in terms of de Broglie-Bohm Pilot-Wave Theory by considering different sim- ple systems that may function as a basic quantum computer. We will provide a careful discussion of Pilot-Wave Theory and evaluate criticisms of the theory. We will assess claims regarding what causes the exponential speed-up in the light of our analysis and the fact that Pilot-Wave The- ory is perfectly able to account for the phenomena involved in quantum computing. I, Philipp Roser, hereby confirm that this dissertation is entirely my own work. Where other sources have been used, these have been clearly referenced. 1 Contents 1 Introduction 3 2 De Broglie-Bohm Pilot-Wave Theory 8 2.1 Motivation . 8 2.2 Two theories of pilot-waves . 9 2.3 The ensemble distribution and probability . 18 2.4 Measurement . 22 2.5 Spin . 26 2.6 Objections and open questions . 33 2.7 Pilot-Wave Theory, Many-Worlds and Many-Worlds in denial . -
The Spirit and the Intellect: Lessons in Humility
BYU Studies Quarterly Volume 50 Issue 4 Article 6 12-1-2011 The Spirit and the Intellect: Lessons in Humility Duane Boyce Follow this and additional works at: https://scholarsarchive.byu.edu/byusq Recommended Citation Boyce, Duane (2011) "The Spirit and the Intellect: Lessons in Humility," BYU Studies Quarterly: Vol. 50 : Iss. 4 , Article 6. Available at: https://scholarsarchive.byu.edu/byusq/vol50/iss4/6 This Article is brought to you for free and open access by the Journals at BYU ScholarsArchive. It has been accepted for inclusion in BYU Studies Quarterly by an authorized editor of BYU ScholarsArchive. For more information, please contact [email protected], [email protected]. Boyce: The Spirit and the Intellect: Lessons in Humility The Spirit and the Intellect Lessons in Humility Duane Boyce “The only wisdom we can hope to acquire is the wisdom of humility: humility is endless.” —T. S. Eliot1 Whence Such Confidence? I have friends who see themselves as having intellectual problems with the gospel—with some spiritual matter or other. Interestingly, these friends all share the same twofold characteristic: they are confident they know a lot about spiritual topics, and they are confident they know a lot about various intellectual matters. This always interests me, because my experience is very different. I am quite struck by how much I don’t know about spiritual things and by how much I don’t know about anything else. The overwhelming feeling I get, both from thoroughly examining a scriptural subject (say, faith2) and from carefully studying an academic topic (for example, John Bell’s inequality theorem in physics), is the same—a profound recognition of how little I really know, and how significantly, on many topics, scholars who are more knowledgeable than I am disagree among themselves: in other words, I am surprised by how little they really know, too. -
Solvay Conference - Wikipedia, the Free Encyclopedia Page 1
Solvay Conference - Wikipedia, the free encyclopedia Page 1 Solvay Conference From Wikipedia, the free encyclopedia The International Solvay Institutes for Physics and Chemistry, located in Brussels, were founded by the Belgian industrialist Ernest Solvay in 1912, following the historic invitation-only 1911 Conseil Solvay , considered a turning point in the world of physics. The Institutes coordinate conferences, workshops, seminars, and colloquia.[1] Following the initial success of 1911, the Solvay Conferences (Conseils Solvay ) have been devoted to outstanding preeminent open problems in both physics and chemistry. The usual schedule is every three years, but there have been larger gaps. Photograph of the first conference in 1911 Contents at the Hotel Metropole. Seated (L-R): W. Nernst, M. Brillouin, E. Solvay, H. 1 Notable Solvay Conferences Lorentz, E. Warburg, J. Perrin, W. Wien, 1.1 First Conference M. Skłodowska-Curie, and H. Poincaré. 1.2 Third Conference Standing (L-R): R. Goldschmidt, M. 1.3 Fifth Conference Planck, H. Rubens, A. Sommerfeld, F. 2 Solvay Conferences on Physics Lindemann, M. de Broglie, M. Knudsen, 2.1 Conferences on Physics gallery F. Hasenöhrl, G. Hostelet, E. Herzen, J.H. 3 Solvay Conferences on Chemistry 3.1 Conferences on Chemistry Jeans, E. Rutherford, H. Kamerlingh gallery Onnes, A. Einstein and P. Langevin. 4 References 5 Further reading 6 External links Notable Solvay Conferences First Conference Hendrik A. Lorentz was chairman of the first Solvay Conference held in Brussels in the autumn of 1911. The subject was Radiation and the Quanta . This conference looked at the problems of having two approaches, namely the classical physics and quantum theory. -
Extreme Quantum Nonequilibrium, Nodes, Vorticity, Drift, and Relaxation Retarding States
Extreme quantum nonequilibrium, nodes, vorticity, drift, and relaxation retarding states Nicolas G Underwood1;2 1Perimeter Institute for Theoretical Physics, 31 Caroline Street North, Waterloo, Ontario, Canada, N2L 2Y5 2Kinard Laboratory, Clemson University, Clemson, South Carolina, USA, 29634 E-mail: [email protected] Abstract. Consideration is given to the behaviour of de Broglie trajectories that are separated from the bulk of the Born distribution with a view to describing the quantum relaxation properties of more `extreme' forms of quantum nonequilibrium. For the 2-dimensional isotropic harmonic oscillator, through the construction of what is termed the `drift field’, a description is given of a general mechanism that causes the relaxation of `extreme' quantum nonequilibrium. Quantum states are found which do not feature this mechanism, so that relaxation may be severely delayed or possibly may not take place at all. A method by which these states may be identified, classified and calculated is given in terms of the properties of the nodes of the state. Properties of the nodes that enable this classification are described for the first time. 1. Introduction De Broglie-Bohm theory [1,2,3,4] is the archetypal member of a class [5,6,7,8] of interpretations of quantum mechanics that feature a mechanism by which quantum probabilities arise dynamically [5,9, 10, 11, 12, 13, 14] from standard ignorance-type probabilities. This mechanism, called `quantum relaxation', occurs spontaneously through a process that is directly analogous to the classical relaxation (from statistical nonequilibrium to statistical equilibrium) of a simple isolated mechanical system as described by the second thermodynamical law. -
Pilot Wave Theory, Bohmian Metaphysics, and the Foundations of Quantum Mechanics Lecture 7 Not Even Wrong
Pilot wave theory, Bohmian metaphysics, and the foundations of quantum mechanics Lecture 7 Not even wrong. Why does nobody like pilot-wave theory? Mike Towler TCM Group, Cavendish Laboratory, University of Cambridge www.tcm.phy.cam.ac.uk/∼mdt26 and www.vallico.net/tti/tti.html [email protected] – Typeset by FoilTEX – 1 Acknowledgements The material in this lecture is to a large extent a summary of publications by Peter Holland, Antony Valentini, Guido Bacciagaluppi, David Peat, David Bohm, Basil Hiley, Oliver Passon, James Cushing, David Peat, Christopher Norris, H. Nikolic, David Deutsch and the Daily Telegraph. Bacciagaluppi and Valentini’s book on the history of the Solvay conference was a particularly vauable resource. Other sources used and many other interesting papers are listed on the course web page: www.tcm.phy.cam.ac.uk/∼mdt26/pilot waves.html MDT – Typeset by FoilTEX – 2 Life on Mars Today we are apt to forget that - not so very long ago - disagreeing with Bohr on quantum foundational issues, or indeed just writing about the subject in general, was professionally equivalent to having a cuckoo surgically attached to the centre of one’s forehead via a small spring. Here, for example, we encounter the RMP Editor feeling the need to add a remark on editorial policy before publishing Prof. Ballentine’s (hardly very controversial) paper on the statistical interpretation, concluding with what seems very like a threat. One need hardly be surprised at Bohm’s reception seventeen years earlier.. – Typeset by FoilTEX – 3 An intimidating atmosphere.. “The idea of an objective real world whose smallest parts exist objectively in the same sense as stones or trees exist, independently of whether or not we observe them.. -
Foundations of Statistical Mechanics and the Status of the Born Rule in De Broglie-Bohm Pilot-Wave Theory
Foundations of statistical mechanics and the status of the Born rule in de Broglie-Bohm pilot-wave theory Antony Valentini Augustus College, 14 Augustus Road, London SW19 6LN, UK. Department of Physics and Astronomy, Clemson University, Kinard Laboratory, Clemson, SC 29634-0978, USA. We compare and contrast two distinct approaches to understanding the Born rule in de Broglie-Bohm pilot-wave theory, one based on dynamical relaxation over time (advocated by this author and collaborators) and the other based on typicality of initial conditions (advocated by the `Bohmian mechanics' school). It is argued that the latter approach is inherently circular and physically mis- guided. The typicality approach has engendered a deep-seated confusion be- tween contingent and law-like features, leading to misleading claims not only about the Born rule but also about the nature of the wave function. By arti- ficially restricting the theory to equilibrium, the typicality approach has led to further misunderstandings concerning the status of the uncertainty principle, the role of quantum measurement theory, and the kinematics of the theory (in- cluding the status of Galilean and Lorentz invariance). The restriction to equi- librium has also made an erroneously-constructed stochastic model of particle creation appear more plausible than it actually is. To avoid needless controversy, we advocate a modest `empirical approach' to the foundations of statistical me- chanics. We argue that the existence or otherwise of quantum nonequilibrium in our world is an empirical question to be settled by experiment. To appear in: Statistical Mechanics and Scientific Explanation: Determin- ism, Indeterminism and Laws of Nature, ed.