Timelessness Strictly Inside the Quantum Realm
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Yes, More Decoherence: a Reply to Critics
Yes, More Decoherence: A Reply to Critics Elise M. Crull∗ Submitted 11 July 2017; revised 24 August 2017 1 Introduction A few years ago I published an article in this journal titled \Less interpretation and more decoherence in quantum gravity and inflationary cosmology" (Crull, 2015) that generated replies from three pairs of authors: Vassallo and Esfeld (2015), Okon and Sudarsky (2016) and Fortin and Lombardi (2017). As a philosopher of physics it is my chief aim to engage physicists and philosophers alike in deeper conversation regarding scientific theories and their implications. In as much as my earlier paper provoked a suite of responses and thereby brought into sharper relief numerous misconceptions regarding decoherence, I welcome the occasion provided by the editors of this journal to continue the discussion. In what follows, I respond to my critics in some detail (wherein the devil is often found). I must be clear at the outset, however, that due to the nature of these criticisms, much of what I say below can be categorized as one or both of the following: (a) a repetition of points made in the original paper, and (b) a reiteration of formal and dynamical aspects of quantum decoherence considered uncontroversial by experts working on theoretical and experimental applications of this process.1 I begin with a few paragraphs describing what my 2015 paper both was, and was not, about. I then briefly address Vassallo's and Esfeld's (hereafter VE) relatively short response to me, dedicating the bulk of my reply to the lengthy critique of Okon and Sudarsky (hereafter OS). -
Arxiv:Quant-Ph/0105127V3 19 Jun 2003
DECOHERENCE, EINSELECTION, AND THE QUANTUM ORIGINS OF THE CLASSICAL Wojciech Hubert Zurek Theory Division, LANL, Mail Stop B288 Los Alamos, New Mexico 87545 Decoherence is caused by the interaction with the en- A. The problem: Hilbert space is big 2 vironment which in effect monitors certain observables 1. Copenhagen Interpretation 2 of the system, destroying coherence between the pointer 2. Many Worlds Interpretation 3 B. Decoherence and einselection 3 states corresponding to their eigenvalues. This leads C. The nature of the resolution and the role of envariance4 to environment-induced superselection or einselection, a quantum process associated with selective loss of infor- D. Existential Interpretation and ‘Quantum Darwinism’4 mation. Einselected pointer states are stable. They can retain correlations with the rest of the Universe in spite II. QUANTUM MEASUREMENTS 5 of the environment. Einselection enforces classicality by A. Quantum conditional dynamics 5 imposing an effective ban on the vast majority of the 1. Controlled not and a bit-by-bit measurement 6 Hilbert space, eliminating especially the flagrantly non- 2. Measurements and controlled shifts. 7 local “Schr¨odinger cat” states. Classical structure of 3. Amplification 7 B. Information transfer in measurements 9 phase space emerges from the quantum Hilbert space in 1. Action per bit 9 the appropriate macroscopic limit: Combination of einse- C. “Collapse” analogue in a classical measurement 9 lection with dynamics leads to the idealizations of a point and of a classical trajectory. In measurements, einselec- III. CHAOS AND LOSS OF CORRESPONDENCE 11 tion replaces quantum entanglement between the appa- A. Loss of the quantum-classical correspondence 11 B. -
Quantum Theory Cannot Consistently Describe the Use of Itself
ARTICLE DOI: 10.1038/s41467-018-05739-8 OPEN Quantum theory cannot consistently describe the use of itself Daniela Frauchiger1 & Renato Renner1 Quantum theory provides an extremely accurate description of fundamental processes in physics. It thus seems likely that the theory is applicable beyond the, mostly microscopic, domain in which it has been tested experimentally. Here, we propose a Gedankenexperiment 1234567890():,; to investigate the question whether quantum theory can, in principle, have universal validity. The idea is that, if the answer was yes, it must be possible to employ quantum theory to model complex systems that include agents who are themselves using quantum theory. Analysing the experiment under this presumption, we find that one agent, upon observing a particular measurement outcome, must conclude that another agent has predicted the opposite outcome with certainty. The agents’ conclusions, although all derived within quantum theory, are thus inconsistent. This indicates that quantum theory cannot be extrapolated to complex systems, at least not in a straightforward manner. 1 Institute for Theoretical Physics, ETH Zurich, 8093 Zurich, Switzerland. Correspondence and requests for materials should be addressed to R.R. (email: [email protected]) NATURE COMMUNICATIONS | (2018) 9:3711 | DOI: 10.1038/s41467-018-05739-8 | www.nature.com/naturecommunications 1 ARTICLE NATURE COMMUNICATIONS | DOI: 10.1038/s41467-018-05739-8 “ 1”〉 “ 1”〉 irect experimental tests of quantum theory are mostly Here, | z ¼À2 D and | z ¼þ2 D denote states of D depending restricted to microscopic domains. Nevertheless, quantum on the measurement outcome z shown by the devices within the D “ψ ”〉 “ψ ”〉 theory is commonly regarded as being (almost) uni- lab. -
Arxiv:1511.01069V1 [Quant-Ph]
To appear in Contemporary Physics Copenhagen Quantum Mechanics Timothy J. Hollowood Department of Physics, Swansea University, Swansea SA2 8PP, U.K. (September 2015) In our quantum mechanics courses, measurement is usually taught in passing, as an ad-hoc procedure involving the ugly collapse of the wave function. No wonder we search for more satisfying alternatives to the Copenhagen interpretation. But this overlooks the fact that the approach fits very well with modern measurement theory with its notions of the conditioned state and quantum trajectory. In addition, what we know of as the Copenhagen interpretation is a later 1950’s development and some of the earlier pioneers like Bohr did not talk of wave function collapse. In fact, if one takes these earlier ideas and mixes them with later insights of decoherence, a much more satisfying version of Copenhagen quantum mechanics emerges, one for which the collapse of the wave function is seen to be a harmless book keeping device. Along the way, we explain why chaotic systems lead to wave functions that spread out quickly on macroscopic scales implying that Schr¨odinger cat states are the norm rather than curiosities generated in physicists’ laboratories. We then describe how the conditioned state of a quantum system depends crucially on how the system is monitored illustrating this with the example of a decaying atom monitored with a time of arrival photon detector, leading to Bohr’s quantum jumps. On the other hand, other kinds of detection lead to much smoother behaviour, providing yet another example of complementarity. Finally we explain how classical behaviour emerges, including classical mechanics but also thermodynamics. -
Quantum Nondemolition Photon Detection in Circuit QED and the Quantum Zeno Effect
PHYSICAL REVIEW A 79, 052115 ͑2009͒ Quantum nondemolition photon detection in circuit QED and the quantum Zeno effect Ferdinand Helmer,1 Matteo Mariantoni,2,3 Enrique Solano,1,4 and Florian Marquardt1 1Department of Physics, Center for NanoScience, and Arnold Sommerfeld Center, Ludwig-Maximilians-Universität, Theresienstrasse 37, D-80333 Munich, Germany 2Walther-Meissner-Institut, Bayerische Akademie der Wissenschaften, Walther-Meissner-Str. 8, D-85748 Garching, Germany 3Physics Department, Technische Universität München, James-Franck-Str., D-85748 Garching, Germany 4Departamento de Quimica Fisica, Universidad del Pais Vasco-Euskal Herriko Unibertsitatea, 48080 Bilbao, Spain ͑Received 17 December 2007; revised manuscript received 15 January 2009; published 20 May 2009͒ We analyze the detection of itinerant photons using a quantum nondemolition measurement. An important example is the dispersive detection of microwave photons in circuit quantum electrodynamics, which can be realized via the nonlinear interaction between photons inside a superconducting transmission line resonator. We show that the back action due to the continuous measurement imposes a limit on the detector efficiency in such a scheme. We illustrate this using a setup where signal photons have to enter a cavity in order to be detected dispersively. In this approach, the measurement signal is the phase shift imparted to an intense beam passing through a second cavity mode. The restrictions on the fidelity are a consequence of the quantum Zeno effect, and we discuss both analytical results and quantum trajectory simulations of the measurement process. DOI: 10.1103/PhysRevA.79.052115 PACS number͑s͒: 03.65.Ta, 03.65.Xp, 42.50.Lc I. INTRODUCTION to be already prepared in a certain state. -
Demnächst Auch in Ihrem Laptop?
The Measurement Problem Johannes Kofler Quantum Foundations Seminar Max Planck Institute of Quantum Optics Munich, December 12th 2011 The measurement problem Different aspects: • How does the wavefunction collapse occur? Does it even occur at all? • How does one know whether something is a system or a measurement apparatus? When does one apply the Schrödinger equation (continuous and deterministic evolution) and when the projection postulate (discontinuous and probabilistic)? • How real is the wavefunction? Does the measurement only reveal pre-existing properties or “create reality”? Is quantum randomness reducible or irreducible? • Are there macroscopic superposition states (Schrödinger cats)? Where is the border between quantum mechanics and classical physics? The Kopenhagen interpretation • Wavefunction: mathematical tool, “catalogue of knowledge” (Schrödinger) not a description of objective reality • Measurement: leads to collapse of the wavefunction (Born rule) • Properties: wavefunction: non-realistic randomness: irreducible • “Heisenberg cut” between system and apparatus: “[T]here arises the necessity to draw a clear dividing line in the description of atomic processes, between the measuring apparatus of the observer which is described in classical concepts, and the object under observation, whose behavior is represented by a wave function.” (Heisenberg) • Classical physics as limiting case and as requirement: “It is decisive to recognize that, however far the phenomena transcend the scope of classical physical explanation, the -
Annual Report to Industry Canada Covering The
Annual Report to Industry Canada Covering the Objectives, Activities and Finances for the period August 1, 2008 to July 31, 2009 and Statement of Objectives for Next Year and the Future Perimeter Institute for Theoretical Physics 31 Caroline Street North Waterloo, Ontario N2L 2Y5 Table of Contents Pages Period A. August 1, 2008 to July 31, 2009 Objectives, Activities and Finances 2-52 Statement of Objectives, Introduction Objectives 1-12 with Related Activities and Achievements Financial Statements, Expenditures, Criteria and Investment Strategy Period B. August 1, 2009 and Beyond Statement of Objectives for Next Year and Future 53-54 1 Statement of Objectives Introduction In 2008-9, the Institute achieved many important objectives of its mandate, which is to advance pure research in specific areas of theoretical physics, and to provide high quality outreach programs that educate and inspire the Canadian public, particularly young people, about the importance of basic research, discovery and innovation. Full details are provided in the body of the report below, but it is worth highlighting several major milestones. These include: In October 2008, Prof. Neil Turok officially became Director of Perimeter Institute. Dr. Turok brings outstanding credentials both as a scientist and as a visionary leader, with the ability and ambition to position PI among the best theoretical physics research institutes in the world. Throughout the last year, Perimeter Institute‘s growing reputation and targeted recruitment activities led to an increased number of scientific visitors, and rapid growth of its research community. Chart 1. Growth of PI scientific staff and associated researchers since inception, 2001-2009. -
Appendix: the Interaction Picture
Appendix: The Interaction Picture The technique of expressing operators and quantum states in the so-called interaction picture is of great importance in treating quantum-mechanical problems in a perturbative fashion. It plays an important role, for example, in the derivation of the Born–Markov master equation for decoherence detailed in Sect. 4.2.2. We shall review the basics of the interaction-picture approach in the following. We begin by considering a Hamiltonian of the form Hˆ = Hˆ0 + V.ˆ (A.1) Here Hˆ0 denotes the part of the Hamiltonian that describes the free (un- perturbed) evolution of a system S, whereas Vˆ is some added external per- turbation. In applications of the interaction-picture formalism, Vˆ is typically assumed to be weak in comparison with Hˆ0, and the idea is then to deter- mine the approximate dynamics of the system given this assumption. In the following, however, we shall proceed with exact calculations only and make no assumption about the relative strengths of the two components Hˆ0 and Vˆ . From standard quantum theory, we know that the expectation value of an operator observable Aˆ(t) is given by the trace rule [see (2.17)], & ' & ' ˆ ˆ Aˆ(t) =Tr Aˆ(t)ˆρ(t) =Tr Aˆ(t)e−iHtρˆ(0)eiHt . (A.2) For reasons that will immediately become obvious, let us rewrite this expres- sion as & ' ˆ ˆ ˆ ˆ ˆ ˆ Aˆ(t) =Tr eiH0tAˆ(t)e−iH0t eiH0te−iHtρˆ(0)eiHte−iH0t . (A.3) ˆ In inserting the time-evolution operators e±iH0t at the beginning and the end of the expression in square brackets, we have made use of the fact that the trace is cyclic under permutations of the arguments, i.e., that Tr AˆBˆCˆ ··· =Tr BˆCˆ ···Aˆ , etc. -
Information and Entropy in Quantum Theory
Information and Entropy in Quantum Theory O J E Maroney Ph.D. Thesis Birkbeck College University of London Malet Street London WC1E 7HX arXiv:quant-ph/0411172v1 23 Nov 2004 Abstract Recent developments in quantum computing have revived interest in the notion of information as a foundational principle in physics. It has been suggested that information provides a means of interpreting quantum theory and a means of understanding the role of entropy in thermodynam- ics. The thesis presents a critical examination of these ideas, and contrasts the use of Shannon information with the concept of ’active information’ introduced by Bohm and Hiley. We look at certain thought experiments based upon the ’delayed choice’ and ’quantum eraser’ interference experiments, which present a complementarity between information gathered from a quantum measurement and interference effects. It has been argued that these experiments show the Bohm interpretation of quantum theory is untenable. We demonstrate that these experiments depend critically upon the assumption that a quantum optics device can operate as a measuring device, and show that, in the context of these experiments, it cannot be consistently understood in this way. By contrast, we then show how the notion of ’active information’ in the Bohm interpretation provides a coherent explanation of the phenomena shown in these experiments. We then examine the relationship between information and entropy. The thought experiment connecting these two quantities is the Szilard Engine version of Maxwell’s Demon, and it has been suggested that quantum measurement plays a key role in this. We provide the first complete description of the operation of the Szilard Engine as a quantum system. -
Modified Two-Slit Experiments and Complementarity
Journal of Quantum Information Science, 2012, 2, 35-40 http://dx.doi.org/10.4236/jqis.2012.22007 Published Online June 2012 (http://www.SciRP.org/journal/jqis) Modified Two-Slit Experiments and Complementarity Tabish Qureshi Centre for Theoretical Physics, Jamia Millia Islamia, New Delhi, India Email: [email protected] Received March 17, 2012; revised April 25, 2012; accepted May 5, 2012 ABSTRACT Some modified two-slit interference experiments claim to demonstrate a violation of Bohr’s complementarity principle. A typical such experiment is theoretically analyzed using wave-packet dynamics. The flaw in the analysis of such ex- periments is pointed out and it is demonstrated that they do not violate complementarity. In addition, it is quite gener- ally proved that if the state of a particle is such that the modulus square of the wave-function yields an interference pat- tern, then it necessarily loses which-path information. Keywords: Complementarity; Wave-Particle Duality; Two-Slit Experiment 1. Introduction pattern, one cannot get the which-way information. The authors have a clever scheme for establishing the exis- It is generally accepted that the wave and particle aspects tence of the interference pattern without actually observ- of quantum systems are mutually exclusive. Niels Bohr ing it. First, the exact locations of the dark fringes are elevated this concept, which is probably born out of the determined by observing the interference pattern. Then, uncertainty principle, to the status of a separate principle, thin wires are placed in the exact locations of the dark the principle of complementarity [1]. fringes. The argument is that if the interference pattern Since then, the complementarity principle has been exists, sliding in wires through the dark fringes will not demonstrated in various experiments, the most common affect the intensity of light on the two detectors. -
Measurement Theories in Quantum Mechanics
Measurement Theories in Quantum Mechanics Cortland M. Setlow March 3, 2006 2 Contents 1 Introduction 1 1.1 Intent .. 1 1.2 Overview. 1 1.3 New Theories from Old 3 2 A Brief Review of Mechanics 7 2.1 Newtonian Mechanics: F = mn 8 2.1.1 Newton's Laws of Motion. 8 2.1.2 Mathematics and the Connection to Experiment 9 2.2 Hamiltonian and Lagrangian Mechanics . 10 2.2.1 Lagrangian Mechanics . 10 2.2.2 Hamiltonian Mechanics 12 2.2.3 Conclusions ....... 13 2.3 The Hamiltonian in Quantum Mechanics 14 2.4 The Lagrangian in Quantum Mechanics 14 2.5 Conclusion . .......... 15 3 The Measurement Problem 17 3.1 Introduction . 17 3.2 Quantum Mysteries. 18 i ii CONTENTS 3.2.1 Probability Rules . 18 3.2.2 Probability in Experiments: Diffraction 19 3.3 Conclusions .......... 20 3.3.1 Additional Background 20 3.3.2 Summary ..... 21 4 Solutions to Quantum Problems 23 4.1 Introduction . 23 4.2 Orthodox Theory 23 4.2.1 Measurement in the Orthodox Theory . 24 4.2.2 Criticisms of Orthodox Measurement 24 4.2.3 Conclusions ... 25 4.3 Ghirardi-Rimini-Weber . 25 4.3.1 Dynamics 26 4.3.2 Motivation. 26 4.3.3 Criticisms 28 4.4 Hidden Variables 30 4.4.1 Dynamics of Bohm's Hidden Variables Interpretation. 31 4.4.2 Introducing the Hidden Variables .... 32 4.4.3 But What About von Neumann's Proof? . 33 4.4.4 Relativity and the Quantum Potential 34 4.5 Everett's Relative State Formulation 34 4.5.1 Motivation . -
Einselection Without Pointer States
Einselection without pointer states Einselection without pointer states - Decoherence under weak interaction Christian Gogolin Universit¨atW¨urzburg 2009-12-16 C. Gogolin j Universit¨atW¨urzburg j 2009-12-16 1 / 26 Einselection without pointer states j Introduction New foundation for Statistical Mechanics X Thermodynamics X Statistical Mechanics Second Law ergodicity equal a priory probabilities Classical Mechanics [2, 3] C. Gogolin j Universit¨atW¨urzburg j 2009-12-16 2 / 26 Einselection without pointer states j Introduction New foundation for Statistical Mechanics X Thermodynamics X Statistical Mechanics Second Law ergodicity ? equal a priory probabilities Classical Mechanics ? [2, 3] C. Gogolin j Universit¨atW¨urzburg j 2009-12-16 2 / 26 Einselection without pointer states j Introduction New foundation for Statistical Mechanics X Thermodynamics X Statistical Mechanics [2, 3] C. Gogolin j Universit¨atW¨urzburg j 2009-12-16 2 / 26 Einselection without pointer states j Introduction New foundation for Statistical Mechanics X Thermodynamics X Statistical Mechanics * Quantum Mechanics X [2, 3] C. Gogolin j Universit¨atW¨urzburg j 2009-12-16 2 / 26 quantum mechanical orbitals discrete energy levels coherent superpositions hopping Einselection without pointer states j Introduction Why do electrons hop between energy eigenstates? C. Gogolin j Universit¨atW¨urzburg j 2009-12-16 3 / 26 discrete energy levels hopping Einselection without pointer states j Introduction Why do electrons hop between energy eigenstates? quantum mechanical orbitals coherent superpositions C. Gogolin j Universit¨atW¨urzburg j 2009-12-16 3 / 26 Einselection without pointer states j Introduction Why do electrons hop between energy eigenstates? quantum mechanical orbitals discrete energy levels coherent superpositions hopping C.