A WORLD WITHOUT CAUSE and EFFECT Logic-Defying Experiments Into Quantum Causality Scramble the Notion of Time Itself
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Introduction to Dynamical Triangulations
Introduction to Dynamical Triangulations Andrzej G¨orlich Niels Bohr Institute, University of Copenhagen Naxos, September 12th, 2011 Andrzej G¨orlich Causal Dynamical Triangulation Outline 1 Path integral for quantum gravity 2 Causal Dynamical Triangulations 3 Numerical setup 4 Phase diagram 5 Background geometry 6 Quantum fluctuations Andrzej G¨orlich Causal Dynamical Triangulation Path integral formulation of quantum mechanics A classical particle follows a unique trajectory. Quantum mechanics can be described by Path Integrals: All possible trajectories contribute to the transition amplitude. To define the functional integral, we discretize the time coordinate and approximate each path by linear pieces. space classical trajectory t1 time t2 Andrzej G¨orlich Causal Dynamical Triangulation Path integral formulation of quantum mechanics A classical particle follows a unique trajectory. Quantum mechanics can be described by Path Integrals: All possible trajectories contribute to the transition amplitude. To define the functional integral, we discretize the time coordinate and approximate each path by linear pieces. quantum trajectory space classical trajectory t1 time t2 Andrzej G¨orlich Causal Dynamical Triangulation Path integral formulation of quantum mechanics A classical particle follows a unique trajectory. Quantum mechanics can be described by Path Integrals: All possible trajectories contribute to the transition amplitude. To define the functional integral, we discretize the time coordinate and approximate each path by linear pieces. quantum trajectory space classical trajectory t1 time t2 Andrzej G¨orlich Causal Dynamical Triangulation Path integral formulation of quantum gravity General Relativity: gravity is encoded in space-time geometry. The role of a trajectory plays now the geometry of four-dimensional space-time. All space-time histories contribute to the transition amplitude. -
Causality and Determinism: Tension, Or Outright Conflict?
1 Causality and Determinism: Tension, or Outright Conflict? Carl Hoefer ICREA and Universidad Autònoma de Barcelona Draft October 2004 Abstract: In the philosophical tradition, the notions of determinism and causality are strongly linked: it is assumed that in a world of deterministic laws, causality may be said to reign supreme; and in any world where the causality is strong enough, determinism must hold. I will show that these alleged linkages are based on mistakes, and in fact get things almost completely wrong. In a deterministic world that is anything like ours, there is no room for genuine causation. Though there may be stable enough macro-level regularities to serve the purposes of human agents, the sense of “causality” that can be maintained is one that will at best satisfy Humeans and pragmatists, not causal fundamentalists. Introduction. There has been a strong tendency in the philosophical literature to conflate determinism and causality, or at the very least, to see the former as a particularly strong form of the latter. The tendency persists even today. When the editors of the Stanford Encyclopedia of Philosophy asked me to write the entry on determinism, I found that the title was to be “Causal determinism”.1 I therefore felt obliged to point out in the opening paragraph that determinism actually has little or nothing to do with causation; for the philosophical tradition has it all wrong. What I hope to show in this paper is that, in fact, in a complex world such as the one we inhabit, determinism and genuine causality are probably incompatible with each other. -
Causality in Quantum Field Theory with Classical Sources
Causality in Quantum Field Theory with Classical Sources Bo-Sture K. Skagerstam1;a), Karl-Erik Eriksson2;b), Per K. Rekdal3;c) a)Department of Physics, NTNU, Norwegian University of Science and Technology, N-7491 Trondheim, Norway b) Department of Space, Earth and Environment, Chalmers University of Technology, SE-412 96 G¨oteborg, Sweden c)Molde University College, P.O. Box 2110, N-6402 Molde, Norway Abstract In an exact quantum-mechanical framework we show that space-time expectation values of the second-quantized electromagnetic fields in the Coulomb gauge, in the presence of a classical source, automatically lead to causal and properly retarded elec- tromagnetic field strengths. The classical ~-independent and gauge invariant Maxwell's equations then naturally emerge and are therefore also consistent with the classical spe- cial theory of relativity. The fundamental difference between interference phenomena due to the linear nature of the classical Maxwell theory as considered in, e.g., classical optics, and interference effects of quantum states is clarified. In addition to these is- sues, the framework outlined also provides for a simple approach to invariance under time-reversal, some spontaneous photon emission and/or absorption processes as well as an approach to Vavilov-Cherenkovˇ radiation. The inherent and necessary quan- tum uncertainty, limiting a precise space-time knowledge of expectation values of the quantum fields considered, is, finally, recalled. arXiv:1801.09947v2 [quant-ph] 30 Mar 2019 1Corresponding author. Email address: [email protected] 2Email address: [email protected] 3Email address: [email protected] 1. Introduction The roles of causality and retardation in classical and quantum-mechanical versions of electrodynamics are issues that one encounters in various contexts (for recent discussions see, e.g., Refs.[1]-[14]). -
Time and Causality in General Relativity
Time and Causality in General Relativity Ettore Minguzzi Universit`aDegli Studi Di Firenze FQXi International Conference. Ponta Delgada, July 10, 2009 FQXi Conference 2009, Ponta Delgada Time and Causality in General Relativity 1/8 Light cone A tangent vector v 2 TM is timelike, lightlike, causal or spacelike if g(v; v) <; =; ≤; > 0 respectively. Time orientation and spacetime At every point there are two cones of timelike vectors. The Lorentzian manifold is time orientable if a continuous choice of one of the cones, termed future, can be made. If such a choice has been made the Lorentzian manifold is time oriented and is also called spacetime. Lorentzian manifolds and light cones Lorentzian manifolds A Lorentzian manifold is a Hausdorff manifold M, of dimension n ≥ 2, endowed with a Lorentzian metric, that is a section g of T ∗M ⊗ T ∗M with signature (−; +;:::; +). FQXi Conference 2009, Ponta Delgada Time and Causality in General Relativity 2/8 Time orientation and spacetime At every point there are two cones of timelike vectors. The Lorentzian manifold is time orientable if a continuous choice of one of the cones, termed future, can be made. If such a choice has been made the Lorentzian manifold is time oriented and is also called spacetime. Lorentzian manifolds and light cones Lorentzian manifolds A Lorentzian manifold is a Hausdorff manifold M, of dimension n ≥ 2, endowed with a Lorentzian metric, that is a section g of T ∗M ⊗ T ∗M with signature (−; +;:::; +). Light cone A tangent vector v 2 TM is timelike, lightlike, causal or spacelike if g(v; v) <; =; ≤; > 0 respectively. -
Causality in the Quantum World
VIEWPOINT Causality in the Quantum World A new model extends the definition of causality to quantum-mechanical systems. by Jacques Pienaar∗ athematical models for deducing cause-effect relationships from statistical data have been successful in diverse areas of science (see Ref. [1] and references therein). Such models can Mbe applied, for instance, to establish causal relationships between smoking and cancer or to analyze risks in con- struction projects. Can similar models be extended to the microscopic world governed by the laws of quantum me- chanics? Answering this question could lead to advances in quantum information and to a better understanding of the foundations of quantum mechanics. Developing quantum Figure 1: In statistics, causal models can be used to extract extensions of causal models, however, has proven challeng- cause-effect relationships from empirical data on a complex ing because of the peculiar features of quantum mechanics. system. Existing models, however, do not apply if at least one For instance, if two or more quantum systems are entangled, component of the system (Y) is quantum. Allen et al. have now it is hard to deduce whether statistical correlations between proposed a quantum extension of causal models. (APS/Alan them imply a cause-effect relationship. John-Mark Allen at Stonebraker) the University of Oxford, UK, and colleagues have now pro- posed a quantum causal model based on a generalization of an old principle known as Reichenbach’s common cause is a third variable that is a common cause of both. In the principle [2]. latter case, the correlation will disappear if probabilities are Historically, statisticians thought that all information conditioned to the common cause. -
Study of Quantum Spin Correlations of Relativistic Electron Pairs
Study of quantum spin correlations of relativistic electron pairs Project status Nov. 2015 Jacek Ciborowski Marta Włodarczyk, Michał Drągowski, Artem Poliszczuk (UW) Joachim Enders, Yuliya Fritsche (TU Darmstadt) Warszawa 20.XI.2015 Quantum spin correlations In this exp: e1,e2 – electrons under study a, b - directions of spin projections (+- ½) 4 combinations for e1 and e2: ++, --, +-, -+ Probabilities: P++ , P+- , P-+ , P- - (ΣP=1) Correlation function : C = P++ + P-- - P-+ - P-+ Historical perspective • Einstein Podolsky Rosen (EPR) paradox (1935): QM is not a complete local realistic theory • Bohm & Aharonov formulation involving spin correlations (1957) • Bell inequalities (1964) a local realistic theory must obey a class of inequalities • practical approach to Bell’s inequalities: counting aacoincidences to measure correlations The EPR paradox Boris Podolsky Nathan Rosen Albert Einstein (1896-1966) (1909-1995) (1979-1955) A. Afriat and F. Selleri, The Einstein, Podolsky and Rosen Paradox (Plenum Press, New York and London, 1999) Bohm’s version with the spin Two spin-1/2 fermions in a singlet state: E.g. if spin projection of 1 on Z axis is measured 1/2 spin projection of 2 must be -1/2 All projections should be elements of reality (QM predicts that only S2 and David Bohm (1917-1992) Sz can be determined) Hidden variables? ”Quantum Theory” (1951) Phys. Rev. 85(1952)166,180 The Bell inequalities J.S.Bell: Impossible to reconcile the concept of hidden variables with statistical predictions of QM If local realism quantum correlations -
Quantum Eraser
Quantum Eraser March 18, 2015 It was in 1935 that Albert Einstein, with his collaborators Boris Podolsky and Nathan Rosen, exploiting the bizarre property of quantum entanglement (not yet known under that name which was coined in Schrödinger (1935)), noted that QM demands that systems maintain a variety of ‘correlational properties’ amongst their parts no matter how far the parts might be sepa- rated from each other (see 1935, the source of what has become known as the EPR paradox). In itself there appears to be nothing strange in this; such cor- relational properties are common in classical physics no less than in ordinary experience. Consider two qualitatively identical billiard balls approaching each other with equal but opposite velocities. The total momentum is zero. After they collide and rebound, measurement of the velocity of one ball will naturally reveal the velocity of the other. But the EPR argument coupled this observation with the orthodox Copen- hagen interpretation of QM, which states that until a measurement of a par- ticular property is made on a system, that system cannot, in general, be said to possess any definite value of that property. It is easy to see that if dis- tant correlations are preserved through measurement processes that ‘bring into being’ the measured values there is a prima facie conflict between the Copenhagen interpretation and the relativistic stricture that no information can be transmitted faster than the speed of light. Suppose, for example, we have a system with some property which is anti-correlated (in real cases, this property could be spin). -
Required Readings
HPS/PHIL 93872 Spring 2006 Historical Foundations of the Quantum Theory Don Howard, Instructor Required Readings: Topic: Readings: Planck and black-body radiation. Martin Klein. “Planck, Entropy, and Quanta, 19011906.” The Natural Philosopher 1 (1963), 83-108. Martin Klein. “Einstein’s First Paper on Quanta.” The Natural Einstein and the photo-electric effect. Philosopher 2 (1963), 59-86. Max Jammer. “Regularities in Line Spectra”; “Bohr’s Theory The Bohr model of the atom and spectral of the Hydrogen Atom.” In The Conceptual Development of series. Quantum Mechanics. New York: McGraw-Hill, 1966, pp. 62- 88. The Bohr-Sommerfeld “old” quantum Max Jammer. “The Older Quantum Theory.” In The Conceptual theory; Einstein on transition Development of Quantum Mechanics. New York: McGraw-Hill, probabilities. 1966, pp. 89-156. The Bohr-Kramers-Slater theory. Max Jammer. “The Transition to Quantum Mechanics.” In The Conceptual Development of Quantum Mechanics. New York: McGraw-Hill, 1966, pp. 157-195. Bose-Einstein statistics. Don Howard. “‘Nicht sein kann was nicht sein darf,’ or the Prehistory of EPR, 1909-1935: Einstein’s Early Worries about the Quantum Mechanics of Composite Systems.” In Sixty-Two Years of Uncertainty: Historical, Philosophical, and Physical Inquiries into the Foundations of Quantum Mechanics. Arthur Miller, ed. New York: Plenum, 1990, pp. 61-111. Max Jammer. “The Formation of Quantum Mechanics.” In The Schrödinger and wave mechanics; Conceptual Development of Quantum Mechanics. New York: Heisenberg and matrix mechanics. McGraw-Hill, 1966, pp. 196-280. James T. Cushing. “Early Attempts at Causal Theories: A De Broglie and the origins of pilot-wave Stillborn Program.” In Quantum Mechanics: Historical theory. -
Can Quantum-Mechanical Description of Physical Reality Be Considered
Can quantum-mechanical description of physical reality be considered incomplete? Gilles Brassard Andr´eAllan M´ethot D´epartement d’informatique et de recherche op´erationnelle Universit´ede Montr´eal, C.P. 6128, Succ. Centre-Ville Montr´eal (QC), H3C 3J7 Canada {brassard, methotan}@iro.umontreal.ca 13 June 2005 Abstract In loving memory of Asher Peres, we discuss a most important and influential paper written in 1935 by his thesis supervisor and men- tor Nathan Rosen, together with Albert Einstein and Boris Podolsky. In that paper, the trio known as EPR questioned the completeness of quantum mechanics. The authors argued that the then-new theory should not be considered final because they believed it incapable of describing physical reality. The epic battle between Einstein and Bohr arXiv:quant-ph/0701001v1 30 Dec 2006 intensified following the latter’s response later the same year. Three decades elapsed before John S. Bell gave a devastating proof that the EPR argument was fatally flawed. The modest purpose of our paper is to give a critical analysis of the original EPR paper and point out its logical shortcomings in a way that could have been done 70 years ago, with no need to wait for Bell’s theorem. We also present an overview of Bohr’s response in the interest of showing how it failed to address the gist of the EPR argument. Dedicated to the memory of Asher Peres 1 Introduction In 1935, Albert Einstein, Boris Podolsky and Nathan Rosen published a paper that sent shock waves in the physics community [5], especially in Copenhagen. -
A Brief Introduction to Temporality and Causality
A Brief Introduction to Temporality and Causality Kamran Karimi D-Wave Systems Inc. Burnaby, BC, Canada [email protected] Abstract Causality is a non-obvious concept that is often considered to be related to temporality. In this paper we present a number of past and present approaches to the definition of temporality and causality from philosophical, physical, and computational points of view. We note that time is an important ingredient in many relationships and phenomena. The topic is then divided into the two main areas of temporal discovery, which is concerned with finding relations that are stretched over time, and causal discovery, where a claim is made as to the causal influence of certain events on others. We present a number of computational tools used for attempting to automatically discover temporal and causal relations in data. 1. Introduction Time and causality are sources of mystery and sometimes treated as philosophical curiosities. However, there is much benefit in being able to automatically extract temporal and causal relations in practical fields such as Artificial Intelligence or Data Mining. Doing so requires a rigorous treatment of temporality and causality. In this paper we present causality from very different view points and list a number of methods for automatic extraction of temporal and causal relations. The arrow of time is a unidirectional part of the space-time continuum, as verified subjectively by the observation that we can remember the past, but not the future. In this regard time is very different from the spatial dimensions, because one can obviously move back and forth spatially. -
K-Causal Structure of Space-Time in General Relativity
PRAMANA °c Indian Academy of Sciences Vol. 70, No. 4 | journal of April 2008 physics pp. 587{601 K-causal structure of space-time in general relativity SUJATHA JANARDHAN1;¤ and R V SARAYKAR2 1Department of Mathematics, St. Francis De Sales College, Nagpur 440 006, India 2Department of Mathematics, R.T.M. Nagpur University, Nagpur 440 033, India ¤Corresponding author E-mail: sujata [email protected]; r saraykar@redi®mail.com MS received 3 January 2007; revised 29 November 2007; accepted 5 December 2007 Abstract. Using K-causal relation introduced by Sorkin and Woolgar [1], we generalize results of Garcia-Parrado and Senovilla [2,3] on causal maps. We also introduce causality conditions with respect to K-causality which are analogous to those in classical causality theory and prove their inter-relationships. We introduce a new causality condition fol- lowing the work of Bombelli and Noldus [4] and show that this condition lies in between global hyperbolicity and causal simplicity. This approach is simpler and more general as compared to traditional causal approach [5,6] and it has been used by Penrose et al [7] in giving a new proof of positivity of mass theorem. C0-space-time structures arise in many mathematical and physical situations like conical singularities, discontinuous matter distributions, phenomena of topology-change in quantum ¯eld theory etc. Keywords. C0-space-times; causal maps; causality conditions; K-causality. PACS Nos 04.20.-q; 02.40.Pc 1. Introduction The condition that no material particle signals can travel faster than the velocity of light ¯xes the causal structure for Minkowski space-time. -
Location and Causality in Quantum Theory
Location and Causality in Quantum Theory A dissertation submitted to the University of Manchester for the degree of Master of Science by Research in the Faculty of Engineering and Physical Sciences 2013 Robert A Dickinson School of Physics and Astronomy Contents 1 Introduction 8 1.1 Causality . .8 1.2 Relativistic causality . .9 1.3 The structure of this document . 10 2 Correlations 12 2.1 Operational descriptions . 12 2.2 Restrictions on non-local correlations in a classical theory . 12 2.3 Parameter spaces of general correlations . 14 2.3.1 Imaginable parameter spaces for one binary observer . 15 2.3.2 One-way signalling between two observers . 15 2.3.3 Imaginable parameter spaces for two spacelike-separated binary observers . 17 2.3.4 The parameter space in nature for two spacelike-separated binary observers . 21 2.3.5 The parameter space in quantum theory for two spacelike- separated binary observers . 22 2.3.6 Parameter spaces for three or more spacelike-separated binary observers . 24 3 Hilbert Space 26 3.1 The Postulates and their implications . 26 3.2 Operational stochastic quantum theory . 28 3.2.1 Internal unknowns regarding the initial state . 29 3.2.2 External unknowns regarding the initial state . 30 3.2.3 Internal unknowns regarding the measurement . 30 3.2.4 External unknowns regarding the measurement . 31 3.2.5 The generalised update rule . 31 3.3 Causality in quantum mechanics . 33 3.3.1 The no-signalling condition . 33 3.3.2 Special cases . 35 3.4 From discrete to continuous sets of outcomes .