Quantum Theory Cannot Consistently Describe the Use of Itself
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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. -
Quantum Violation of Classical Physics in Macroscopic Systems
Quantum VIOLATION OF CLASSICAL PHYSICS IN MACROSCOPIC SYSTEMS Lucas Clemente Ludwig Maximilian University OF Munich Max Planck INSTITUTE OF Quantum Optics Quantum VIOLATION OF CLASSICAL PHYSICS IN MACROSCOPIC SYSTEMS Lucas Clemente Dissertation AN DER Fakultät für Physik DER Ludwig-Maximilians-Universität München VORGELEGT VON Lucas Clemente AUS München München, IM NoVEMBER 2015 TAG DER mündlichen Prüfung: 26. Januar 2016 Erstgutachter: Prof. J. IGNACIO Cirac, PhD Zweitgutachter: Prof. Dr. Jan VON Delft WEITERE Prüfungskommissionsmitglieder: Prof. Dr. HarALD Weinfurter, Prof. Dr. Armin Scrinzi Reality is that which, when you stop believing in it, doesn’t go away. “ — Philip K. Dick How To Build A Universe That Doesn’t Fall Apart Two Days Later, a speech published in the collection I Hope I Shall Arrive Soon Contents Abstract xi Zusammenfassung xiii List of publications xv Acknowledgments xvii 0 Introduction 1 0.1 History and motivation . 3 0.2 Local realism and Bell’s theorem . 5 0.3 Contents of this thesis . 10 1 Conditions for macrorealism 11 1.1 Macroscopic realism . 13 1.2 Macrorealism per se following from strong non-invasive measurability 15 1.3 The Leggett-Garg inequality . 17 1.4 No-signaling in time . 19 1.5 Necessary and sufficient conditions for macrorealism . 21 1.6 No-signaling in time for quantum measurements . 25 1.6.1 Without time evolution . 26 1.6.2 With time evolution . 27 1.7 Conclusion and outlook . 28 Appendix 31 1.A Proof that NSIT0(1)2 is sufficient for NIC0(1)2 . 31 2 Macroscopic classical dynamics from microscopic quantum behavior 33 2.1 Quantifying violations of classicality . -
Particle Or Wave: There Is No Evidence of Single Photon Delayed Choice
Particle or wave: there is no evidence of single photon delayed choice. Michael Devereux* Los Alamos National Laboratory (Retired) Abstract Wheeler supposed that the way in which a single photon is measured in the present could determine how it had behaved in the past. He named such retrocausation delayed choice. Over the last forty years many experimentalists have claimed to have observed single-photon delayed choice. Recently, however, researchers have proven that the quantum wavefunction of a single photon assumes the identical mathematical form of the solution to Maxwell’s equations for that photon. This efficacious understanding allows for a trenchant analysis of delayed-choice experiments and denies their retrocausation conclusions. It is now usual for physicists to employ Bohr’s wave-particle complementarity theory to distinguish wave from particle aspects in delayed- choice observations. Nevertheless, single-photon, delayed-choice experiments, provide no evidence that the photon actually acts like a particle, or, instead, like a wave, as a function of a future measurement. And, a recent, careful, Stern-Gerlach analysis has shown that the supposition of concurrent wave and particle characteristics in the Bohm-DeBroglie theory is not tenable. PACS 03.65.Ta, 03.65.Ud 03.67.-a, 42.50.Ar, 42.50.Xa 1. Introduction. Almost forty years ago Wheeler suggested that there exists a type of retrocausation, which he called delayed choice, in certain physical phenomena [1]. Specifically, he said that the past behavior of some quantum systems could be determined by how they are observed in the present. “The past”, he wrote, “has no existence except as it is recorded in the present” [2]. -
A Critic Looks at Qbism Guido Bacciagaluppi
A Critic Looks at QBism Guido Bacciagaluppi To cite this version: Guido Bacciagaluppi. A Critic Looks at QBism. 2013. halshs-00996289 HAL Id: halshs-00996289 https://halshs.archives-ouvertes.fr/halshs-00996289 Preprint submitted on 26 May 2014 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. A Critic Looks at QBism Guido Bacciagaluppi∗ 30 April 2013 Abstract This chapter comments on that by Chris Fuchs on qBism. It presents some mild criticisms of this view, some based on the EPR and Wigner’s friend scenarios, and some based on the quantum theory of measurement. A few alternative suggestions for implementing a sub- jectivist interpretation of probability in quantum mechanics conclude the chapter. “M. Braque est un jeune homme fort audacieux. [...] Il m´eprise la forme, r´eduit tout, sites et figures et maisons, `ades sch´emas g´eom´etriques, `ades cubes. Ne le raillons point, puisqu’il est de bonne foi. Et attendons.”1 Thus commented the French art critic Louis Vauxcelles on Braque’s first one- man show in November 1908, thereby giving cubism its name. Substituting spheres and tetrahedra for cubes might be more appropriate if one wishes to apply the characterisation to qBism — the view of quantum mechanics and the quantum state developed by Chris Fuchs and co-workers (for a general reference see either the paper in this volume, or Fuchs (2010)). -
Contemporary Physics Uncollapsing the Wavefunction by Undoing
This article was downloaded by: [University of California, Riverside] On: 18 February 2010 Access details: Access Details: [subscription number 918975371] Publisher Taylor & Francis Informa Ltd Registered in England and Wales Registered Number: 1072954 Registered office: Mortimer House, 37- 41 Mortimer Street, London W1T 3JH, UK Contemporary Physics Publication details, including instructions for authors and subscription information: http://www.informaworld.com/smpp/title~content=t713394025 Uncollapsing the wavefunction by undoing quantum measurements Andrew N. Jordan a; Alexander N. Korotkov b a Department of Physics and Astronomy, University of Rochester, Rochester, New York, USA b Department of Electrical Engineering, University of California, Riverside, CA, USA First published on: 12 February 2010 To cite this Article Jordan, Andrew N. and Korotkov, Alexander N.(2010) 'Uncollapsing the wavefunction by undoing quantum measurements', Contemporary Physics, 51: 2, 125 — 147, First published on: 12 February 2010 (iFirst) To link to this Article: DOI: 10.1080/00107510903385292 URL: http://dx.doi.org/10.1080/00107510903385292 PLEASE SCROLL DOWN FOR ARTICLE Full terms and conditions of use: http://www.informaworld.com/terms-and-conditions-of-access.pdf This article may be used for research, teaching and private study purposes. Any substantial or systematic reproduction, re-distribution, re-selling, loan or sub-licensing, systematic supply or distribution in any form to anyone is expressly forbidden. The publisher does not give any warranty express or implied or make any representation that the contents will be complete or accurate or up to date. The accuracy of any instructions, formulae and drug doses should be independently verified with primary sources. The publisher shall not be liable for any loss, actions, claims, proceedings, demand or costs or damages whatsoever or howsoever caused arising directly or indirectly in connection with or arising out of the use of this material. -
The Consistent Histories Approach to the Stern-Gerlach Experiment
The Consistent Histories Approach to the Stern-Gerlach Experiment Ian Wilson An undergraduate thesis advised by Dr. David Craig submitted to the Department of Physics, Oregon State University in partial fulfillment of the requirements for the degree BSc in Physics Submitted on May 8, 2020 Acknowledgments I would like to thank Dr. David Craig, for guiding me through an engaging line of research, as well as Dr. David McIntyre, Dr. Elizabeth Gire, Dr. Corinne Manogue and Dr. Janet Tate for developing the quantum curriculum from which this thesis is rooted. I would also like to thank all of those who gave me the time, space, and support I needed while writing this. This includes (but is certainly not limited to) my partner Brooke, my parents Joy and Kevin, my housemate Cheyanne, the staff of Interzone, and my friends Saskia, Rachel and Justin. Abstract Standard quantum mechanics makes foundational assumptions to describe the measurement process. Upon interaction with a “classical measurement apparatus”, a quantum system is subjected to postulated “state collapse” dynamics. We show that framing measurement around state collapse and ill-defined classical observers leads to interpretational issues, and artificially limits the scope of quantum theory. This motivates describing measurement as a unitary process instead. In the context of the Stern-Gerlach experiment, the measurement of an electron’s spin angular momentum is explained as the entanglement of its spin and position degrees of freedom. Furthermore, the electron-environment interaction is also detailed as part of the measurement process. The environment plays the role of a record keeper, establishing the “facts of the universe” to make the measurement’s occurrence objective. -
Theoretical Physics Group Decoherent Histories Approach: a Quantum Description of Closed Systems
Theoretical Physics Group Department of Physics Decoherent Histories Approach: A Quantum Description of Closed Systems Author: Supervisor: Pak To Cheung Prof. Jonathan J. Halliwell CID: 01830314 A thesis submitted for the degree of MSc Quantum Fields and Fundamental Forces Contents 1 Introduction2 2 Mathematical Formalism9 2.1 General Idea...................................9 2.2 Operator Formulation............................. 10 2.3 Path Integral Formulation........................... 18 3 Interpretation 20 3.1 Decoherent Family............................... 20 3.1a. Logical Conclusions........................... 20 3.1b. Probabilities of Histories........................ 21 3.1c. Causality Paradox........................... 22 3.1d. Approximate Decoherence....................... 24 3.2 Incompatible Sets................................ 25 3.2a. Contradictory Conclusions....................... 25 3.2b. Logic................................... 28 3.2c. Single-Family Rule........................... 30 3.3 Quasiclassical Domains............................. 32 3.4 Many History Interpretation.......................... 34 3.5 Unknown Set Interpretation.......................... 36 4 Applications 36 4.1 EPR Paradox.................................. 36 4.2 Hydrodynamic Variables............................ 41 4.3 Arrival Time Problem............................. 43 4.4 Quantum Fields and Quantum Cosmology.................. 45 5 Summary 48 6 References 51 Appendices 56 A Boolean Algebra 56 B Derivation of Path Integral Method From Operator -
Reformulation of Quantum Mechanics and Strong Complementarity from Bayesian Inference Requirements
Reformulation of quantum mechanics and strong complementarity from Bayesian inference requirements William Heartspring Abstract: This paper provides an epistemic reformulation of quantum mechanics (QM) in terms of inference consistency requirements of objective Bayesianism, which include the principle of maximum entropy under physical constraints. Physical constraints themselves are understood in terms of consistency requirements. The by-product of this approach is that QM must additionally be understood as providing the theory of theories. Strong complementarity - that dierent observers may live in separate Hilbert spaces - follows as a consequence, which resolves the rewall paradox. Other clues pointing to this reformu- lation are analyzed. The reformulation, with the addition of novel transition probability arithmetic, resolves the measurement problem completely, thereby eliminating subjectivity of measurements from quantum mechanics. An illusion of collapse comes from Bayesian updates by observer's continuous outcome data. Dark matter and dark energy pop up directly as entropic tug-of-war in the reformulation. Contents 1 Introduction1 2 Epistemic nature of quantum mechanics2 2.1 Area law, quantum information and spacetime2 2.2 State vector from objective Bayesianism5 3 Consequences of the QM reformulation8 3.1 Basis, decoherence and causal diamond complementarity 12 4 Spacetime from entanglement 14 4.1 Locality: area equals mutual information 14 4.2 Story of Big Bang cosmology 14 5 Evidences toward the reformulation 14 5.1 Quantum redundancy 15 6 Transition probability arithmetic: resolving the measurement problem completely 16 7 Conclusion 17 1 Introduction Hamiltonian formalism and Schrödinger picture of quantum mechanics are assumed through- out the writing, with time t 2 R. Whenever the word entropy is mentioned without addi- tional qualication, it refers to von Neumann entropy. -
Consistent Histories
Chapter 12 Local Weak Property Realism: Consistent Histories Earlier, we surmised that weak property realism can escape the strictures of Bell’s theorem and KS. In this chapter, we look at an interpretation of quantum mechanics that does just that, namely, the Consistent Histories Interpretation (CH). 12.1 Consistent Histories The basic idea behind CH is that quantum mechanics is a stochastic theory operating on quantum histories. A history a is a temporal sequence of properties held by a system. For example, if we just consider spin, for an electron a history could be as follows: at t0, Sz =1; at t1, Sx =1; at t2, Sy = -1, where spin components are measured in units of h /2. The crucial point is that in this interpretation the electron is taken to exist independently of us and to have such spin components at such times, while in the standard view 1, 1, and -1 are just experimental return values. In other words, while the standard interpretation tries to provide the probability that such returns would be obtained upon measurement, CH provides the probability Pr(a) that the system will have history a, that is, such and such properties at different times. Hence, CH adopts non-contextual property realism (albeit of the weak sort) and dethrones measurement from the pivotal position it occupies in the orthodox interpretation. To see how CH works, we need first to look at some of the formal features of probability. 12.2 Probability Probability is defined on a sample space S, the set of all the mutually exclusive outcomes of a state of affairs; each element e of S is a sample point to which one assigns a number Pr(e) satisfying the axioms of probability (of which more later). -
Scientific American
Take the Nature Publishing Group survey for the chance to win a MacBookFind out Air more Physics Scientific American (June 2013), 308, 46-51 Published online: 14 May 2013 | doi:10.1038/scientificamerican0613-46 Quantum Weirdness? It's All in Your Mind Hans Christian von Baeyer A new version of quantum theory sweeps away the bizarre paradoxes of the microscopic world. The cost? Quantum information exists only in your imagination CREDIT: Caleb Charland In Brief Quantum mechanics is an incredibly successful theory but one full of strange paradoxes. A recently developed model called Quantum Bayesianism (or QBism) combines quantum theory with probability theory in an effort to eliminate the paradoxes or put them in a less troubling form. QBism reimagines the entity at the heart of quantum paradoxes—the wave function. Scientists use wave functions to calculate the probability that a particle will have a certain property, such as being in one place and not another. But paradoxes arise when physicists assume that a wave function is real. QBism maintains that the wave function is solely a mathematical tool that an observer uses to assign his or her personal belief that a quantum system will have a specific property. In this conception, the wave function does not exist in the world—rather it merely reflects an individual's subjective mental state. ADDITIONAL IMAGES AND ILLUSTRATIONS [QUANTUM PHILOSOPHY] Four Interpretations of Quantum Mechanics [THOUGHT EXPERIMENT] The Fix for Quantum Absurdity Flawlessly accounting for the behavior of matter on scales from the subatomic to the astronomical, quantum mechanics is the most successful theory in all the physical sciences. -
New Journal of Physics the Open–Access Journal for Physics
New Journal of Physics The open–access journal for physics The rise and fall of redundancy in decoherence and quantum Darwinism C Jess Riedel1,2,5, Wojciech H Zurek1,3 and Michael Zwolak1,4 1 Theoretical Division/CNLS, LANL, Los Alamos, NM 87545, USA 2 Department of Physics, University of California, Santa Barbara, CA 93106, USA 3 Santa Fe Institute, Santa Fe, NM 87501, USA 4 Department of Physics, Oregon State University, Corvallis, OR 97331, USA E-mail: [email protected] New Journal of Physics 14 (2012) 083010 (20pp) Received 9 March 2012 Published 10 August 2012 Online at http://www.njp.org/ doi:10.1088/1367-2630/14/8/083010 Abstract. A state selected at random from the Hilbert space of a many-body system is overwhelmingly likely to exhibit highly non-classical correlations. For these typical states, half of the environment must be measured by an observer to determine the state of a given subsystem. The objectivity of classical reality—the fact that multiple observers can agree on the state of a subsystem after measuring just a small fraction of its environment—implies that the correlations found in nature between macroscopic systems and their environments are exceptional. Building on previous studies of quantum Darwinism showing that highly redundant branching states are produced ubiquitously during pure decoherence, we examine the conditions needed for the creation of branching states and study their demise through many-body interactions. We show that even constrained dynamics can suppress redundancy to the values typical of random states on relaxation timescales, and prove that these results hold exactly in the thermodynamic limit. -
Quantum Weirdness? It’S All in Your Mind
PHYSICS QUANTUM WEIRDNESS? IT’S ALL IN YOUR MIND A new version of quantum theory sweeps away the bizarre paradoxes of the microscopic world. The cost? Quantum information exists only in your imagination By Hans Christian von Baeyer lawlessly accounting for the behavior of matter on scales from the subatomic to the astronomical, quantum mechanics is the most successful theory in all the physical sciences. It is also the weirdest. In the quantum realm, particles seem to be in two places at once, information appears to travel faster than the speed of light, and cats can be dead and alive at the same time. Physicists have Fgrappled with the quantum world’s apparent paradoxes for nine decades, with little to show for their struggles. Unlike evolution and cosmology, whose truths have been incorporated into the gen eral intellectual landscape, quantum theory is still considered (even by many physicists) to be a bizarre anomaly, a powerful reci pe book for building gadgets but good for little else. The deep con fusion about the meaning of quantum theory will continue to add 46 Scientific American, June 2013 Photograph by Caleb Charland June 2013, ScientificAmerican.com 47 fuel to the perception that the deep things it is so urgently try hammer is also in a superposition, as is the THOUGHT EXPERIMENT Hans Christian von Baeyer is a theoretical particle ing to tell us about our world are irrelevant to everyday life and physicist and Chancellor Professor emeritus at the College vial of poison. And most grotesquely, the too weird to matter. of William and Mary, where he taught for 38 years.