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Philosophy of Physical Science

Edited by Hans Halvorson (Princeton University)
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  1. Valia Allori & Nino Zanghì (2009). On the Classical Limit of Quantum Mechanics. Foundations of Physics 39 (1):20-32.
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  2. James L. Anderson (2003). Timekeeping in an Expanding Universe. In A. Ashtekar (ed.), Revisiting the Foundations of Relativistic Physics. 275--280.
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  3. Philip W. Anderson, Contributors.
    Is string theory a futile exercise as physics, as I believe it to be? It is an interesting mathematical specialty and has produced and will produce mathematics useful in other contexts, but it seems no more vital as mathematics than other areas of very abstract or specialized math, and doesn't on that basis justify the incredible amount of effort expended on it.
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  4. Aitor Anduaga (2008). The Realist Interpretation of the Atmosphere. Studies in History and Philosophy of Science Part B 39 (3):465-510.
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  5. R. M. Angelo & A. D. Ribeiro (2015). Wave–Particle Duality: An Information-Based Approach. Foundations of Physics 45 (11):1407-1420.
    Recently, Bohr’s complementarity principle was assessed in setups involving delayed choices. These works argued in favor of a reformulation of the aforementioned principle so as to account for situations in which a quantum system would simultaneously behave as wave and particle. Here we defend a framework that, supported by well-known experimental results and consistent with the decoherence paradigm, allows us to interpret complementarity in terms of correlations between the system and an informer. Our proposal offers formal definition and operational interpretation (...)
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  6. Angus Armitage (1952). Sun, Stand Thou Still. The Life & Work of Copernicus the Astronomer. British Journal for the Philosophy of Science 3 (10):200-200.
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  7. Masanari Asano, Irina Basieva, Andrei Khrennikov, Masanori Ohya, Yoshiharu Tanaka & Ichiro Yamato (2015). Quantum Information Biology: From Information Interpretation of Quantum Mechanics to Applications in Molecular Biology and Cognitive Psychology. Foundations of Physics 45 (10):1362-1378.
    We discuss foundational issues of quantum information biology —one of the most successful applications of the quantum formalism outside of physics. QIB provides a multi-scale model of information processing in bio-systems: from proteins and cells to cognitive and social systems. This theory has to be sharply distinguished from “traditional quantum biophysics”. The latter is about quantum bio-physical processes, e.g., in cells or brains. QIB models the dynamics of information states of bio-systems. We argue that the information interpretation of quantum mechanics (...)
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  8. D. Atkinson & J. C. R. Bloch, QCD in the Infrared with Exact Angular Integrations.
    In a previous paper we have shown that in quantum chromodynamics the gluon propagator vanishes in the infrared limit, while the ghost propagator is more singular than a simple pole. These results were obtained after angular averaging, but in the current paper we go beyond this approximation and perform an exact calculation of the angular integrals. The powers of the infrared behaviour of the propagators are changed substantially. We find the very intriguing result that the gluon propagator vanishes in the (...)
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  9. David Atkinson, Dirac's Quantum Jump.
    This minicourse on quantum mechanics is intended for students who have already been rather well exposed to the subject at an elementary level. It is assumed that they have surmounted the first conceptual hurdles and also have struggled with the Schrödinger equation in one dimension.
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  10. David Atkinson, Infrared and Ultraviolet Coupling in Qcd.
    The coupled Dyson-Schwinger equations for the gluon and ghost propagators in QCD are shown to have solutions that correspond to a unique running coupling that has a nite infrared xed point and the expected logarithmic decrease in the ultraviolet. The infrared coupling is large enough to support chiral symmetry breaking and quarks are not con ned, but they cannot be isolated.
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  11. David Atkinson (2009). Nonconservation of Energy and Loss of Determinism I. Infinitely Many Colliding Balls. Foundations of Physics 39 (8):937-957.
    An infinite number of elastically colliding balls is considered in a classical, and then in a relativistic setting. Energy and momentum are not necessarily conserved globally, even though each collision does separately conserve them. This result holds in particular when the total mass of all the balls is finite, and even when the spatial extent and temporal duration of the process are also finite. Further, the process is shown to be indeterministic: there is an arbitrary parameter in the general solution (...)
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  12. David Atkinson & Porter Johnson, Nonconservation of Energy and Loss of Determinism.
    An infinite number of elastically colliding balls is considered in a classical, and then in a relativistic setting. Energy and momentum are not necessarily conserved globally, even though each collision does separately conserve them. This result holds in particular when the total mass of all the balls is finite, and even when the spatial extent and temporal duration of the process are also finite. Further, the process is shown to be indeterministic: there is an arbitrary parameter in the general solution (...)
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  13. Harald Atmanspacher, Mind and Matter as Asymptotically Disjoint, Inequivalent Representations with Broken Time-Reversal Symmetry.
    body. While the latter areas are discussed mainly in fields such as the philosophy of mind, cognitive Many philosophical and scientific discussions of top-.
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  14. Harald Atmanspacher (2006). Complementarity in Classical Dynamical Systems. Foundations of Physics 36 (2):291-306.
    The concept of complementarity, originally defined for non-commuting observables of quantum systems with states of non-vanishing dispersion, is extended to classical dynamical systems with a partitioned phase space. Interpreting partitions in terms of ensembles of epistemic states (symbols) with corresponding classical observables, it is shown that such observables are complementary to each other with respect to particular partitions unless those partitions are generating. This explains why symbolic descriptions based on an ad hoc partition of an underlying phase space description should (...)
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  15. Alexia Auffèves & Philippe Grangier (2016). Contexts, Systems and Modalities: A New Ontology for Quantum Mechanics. Foundations of Physics 46 (2):121-137.
    In this article we present a possible way to make usual quantum mechanics fully compatible with physical realism, defined as the statement that the goal of physics is to study entities of the natural world, existing independently from any particular observer’s perception, and obeying universal and intelligible rules. Rather than elaborating on the quantum formalism itself, we propose a new quantum ontology, where physical properties are attributed jointly to the system, and to the context in which it is embedded. In (...)
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  16. Randall E. Auxier (1999). The Bluffton Charge. The Personalist Forum 15 (1):193-196.
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  17. Francesco Avanzini, Barbara Fresch & Giorgio J. Moro (2016). Pilot-Wave Quantum Theory with a Single Bohm’s Trajectory. Foundations of Physics 46 (5):575-605.
    The representation of a quantum system as the spatial configuration of its constituents evolving in time as a trajectory under the action of the wave-function, is the main objective of the de Broglie–Bohm theory. However, its standard formulation is referred to the statistical ensemble of its possible trajectories. The statistical ensemble is introduced in order to establish the exact correspondence between the probability density on the spatial configurations and the quantum distribution, that is the squared modulus of the wave-function. In (...)
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  18. Jeremy Avigad, A Decision Procedure for Linear “Big o” Equations.
    Let F be the set of functions from an infinite set, S, to an ordered ring, R.
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  19. J. A. B. (1961). The Philosophy of Inorganic Compounds. Review of Metaphysics 14 (4):724-724.
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  20. L. K. B. (1956). Tres Clases de Introduccion a la Filosofia de la Naturaleza. Review of Metaphysics 10 (1):176-176.
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  21. Emmon Bach (1986). The Algebra of Events. Linguistics and Philosophy 9 (1):5--16.
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  22. Miriam Backens & Ali Nabi Duman (2016). A Complete Graphical Calculus for Spekkens’ Toy Bit Theory. Foundations of Physics 46 (1):70-103.
    While quantum theory cannot be described by a local hidden variable model, it is nevertheless possible to construct such models that exhibit features commonly associated with quantum mechanics. These models are also used to explore the question of \-ontic versus \-epistemic theories for quantum mechanics. Spekkens’ toy theory is one such model. It arises from classical probabilistic mechanics via a limit on the knowledge an observer may have about the state of a system. The toy theory for the simplest possible (...)
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  23. Jonathan Bain & John Norton (2001). What Should Philosophers of Science Learn From the History of the Electron? In A. Warwick (ed.), Histories of the Electron: The Birth of Microphysics. 451--465.
    We have now celebrated the centenary of J. J. Thomson’s famous paper (1897) on the electron and have examined one hundred years of the history of our first fundamental particle. What should philosophers of science learn from this history? To some, the fundamental moral is already suggested by the rapid pace of this history. Thomson’s concern in 1897 was to demonstrate that cathode rays are electrified particles and not aetherial vibrations, the latter being the “almost unanimous opinion of German physicists” (...)
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  24. A. P. Bakulev, N. N. Bogoljubov & A. M. Kurbatov (1986). The Principle of Thermodynamic Equivalence in Statistical Mechanics: The Method of Approximating Hamiltonian. Foundations of Physics 16 (9):871-882.
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  25. Yuri Balashov (1999). Zero-Value Physical Quantities. Synthese 119 (3):253-286.
    To state an important fact about the photon, physicists use such expressions as (1) “the photon has zero (null, vanishing) mass” and (2) “the photon is (a) massless (particle)” interchangeably. Both (1) and (2) express the fact that the photon has no non-zero mass. However, statements (1) and (2) disagree about a further fact: (1) attributes to the photon the property of zero-masshood whereas (2) denies that the photon has any mass at all. But is there really a difference between (...)
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  26. Siluan F. Baldin (1942). Energy as the Basic Concept for a Unified Interpretation of Physical Phenomena. Philosophy of Science 9 (3):294-305.
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  27. Leslie E. Ballentine (forthcoming). Propensity, Probability, and Quantum Theory. Foundations of Physics:1-33.
    Quantum mechanics and probability theory share one peculiarity. Both have well established mathematical formalisms, yet both are subject to controversy about the meaning and interpretation of their basic concepts. Since probability plays a fundamental role in QM, the conceptual problems of one theory can affect the other. We first classify the interpretations of probability into three major classes: inferential probability, ensemble probability, and propensity. Class is the basis of inductive logic; deals with the frequencies of events in repeatable experiments; describes (...)
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  28. Aristides Baltas (1991). On Some Structural Aspects of Physical Problems. Synthese 89 (2):299 - 320.
    Bachelard's concept of the problématique is used in order to classify physical problems and their interrelations. This classification is effectuated along two dimensions. Along the horizontal dimension, physical problems are divided into the kinds that the different modes of physics' development define. These modes are themselves determined by the interplay among the conceptual system, the object and the experimentation transactions specific to physics. Along the vertical dimension, physical problems are classified according to the different stages of maturation they have to (...)
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  29. Sorin Bangu (2011). On the Role of Bridge Laws in Intertheoretic Relations. Philosophy of Science 78 (5):1108-1119.
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  30. Sorin Bangu (2006). Pythagorean Heuristic in Physics. Perspectives on Science 14 (4):387-416.
    : Some of the great physicists' belief in the existence of a connection between the aesthetical features of a theory (such as beauty and simplicity) and its truth is still one of the most intriguing issues in the aesthetics of science. In this paper I explore the philosophical credibility of a version of this thesis, focusing on the connection between the mathematical beauty and simplicity of a theory and its truth. I discuss a heuristic interpretation of this thesis, attempting to (...)
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  31. Julian B. Barbour & Bruno Bertotti (1977). Gravity and Inertia in a Machian Framework. Nuovo Cimento 38:1--27.
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  32. V. Barger (1969). Phenomenological Theories of High Energy Scattering. New York, W. A. Benjamin.
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  33. Patrick A. Barker (1988). Physics of the Universe a Universe of Strings : A Theory of Everything : The Gyroquantum Theory. Monograph Collection (Matt - Pseudo).
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  34. H. Barreau (1980). Pour le centenaire d'Albert Einstein: Einstein et les concepts d'espace et de temps. Revue de Métaphysique et de Morale 85 (3):357 - 369.
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  35. Irina Basieva & Andrei Khrennikov (2015). On the Possibility to Combine the Order Effect with Sequential Reproducibility for Quantum Measurements. Foundations of Physics 45 (10):1379-1393.
    In this paper we study the problem of a possibility to use quantum observables to describe a possible combination of the order effect with sequential reproducibility for quantum measurements. By the order effect we mean a dependence of probability distributions on the order of measurements. We consider two types of the sequential reproducibility: adjacent reproducibility ) and separated reproducibility). The first one is reproducibility with probability 1 of a result of measurement of some observable A measured twice, one A measurement (...)
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  36. Ted Bastin (1974). Probability in a Discrete Model of Particles and Observations. Synthese 29 (1-4):203 - 227.
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  37. Vadim Batitsky & Zoltan Domotor (2007). When Good Theories Make Bad Predictions. Synthese 157 (1):79 - 103.
    Chaos-related obstructions to predictability have been used to challenge accounts of theory validation based on the agreement between theoretical predictions and experimental data . These challenges are incomplete in two respects: they do not show that chaotic regimes are unpredictable in principle and, as a result, that there is something conceptually wrong with idealized expectations of correct predictions from acceptable theories, and they do not explore whether chaos-induced predictive failures of deterministic models can be remedied by stochastic modeling. In this (...)
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  38. Mark H. Bauer (1951). Cosmic Radiation and its Biological Effects. Thought: A Journal of Philosophy 26 (3):476-477.
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  39. Maximilian Beck (1946). The Static Character of Time and Flux. New Scholasticism 20 (2):179-182.
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  40. John Bell, Cosmological Theories and the Question of the Existence of a Creator.
    In a Vedic hymn, Reality or Being is proclaimed as having “arisen from Nothing”. By contrast, in Jaina cosmology time has no beginning; the universe, uncreated, has always existed.In Plato’s Timaeus the universe is conceived as not having existed eternally, but as having been created at some past time by a demiurge acting on pre-existing substance. We are all familiar with the arresting first line of Genesis.
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  41. Nue Belnap, Branching Space-Time, Postprint January, 2003.
    ``Branching space-time'' is a simple blend of relativity and indeterminism. Postulates and definitions rigorously describe the ``causal order'' relation between possible point events. The key postulate is a version of ``everything has a causal origin''; key defined terms include ``history'' and ``choice point.'' Some elementary but helpful facts are proved. Application is made to the status of causal contemporaries of indeterministic events, to how ``splitting'' of histories happens, to indeterminism without choice, and to Einstein-Podolsky-Rosen distant correlations.
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  42. D. W. Belousek (forthcoming). Interpretation and Ontology in Modern Physics. Metascience.
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  43. Wm Bender (1934). The Method of Physical Coincidences and the Scale Coordinate. Philosophy of Science 1 (3):253-272.
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  44. Abram Cornelius Benjamin (1955). Operationism. Springfield, Ill.,Thomas.
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  45. A. F. Bennett (forthcoming). Duffin–Kemmer–Petiau Particles Are Bosons. Foundations of Physics:1-19.
    The parametrized Duffin–Kemmer–Petiau wave equation is formulated for many relativistic particles of spin-0 or spin-1. The first-quantized formulation lacks the fields of creation and annihilation operators which satisfy commutation relations subject to causality conditions, and which are essential to the Quantum Field Theoretic proof of the spin-statistics connection. It is instead proved that the wavefunctions for identical particles must be symmetric by extension of the nonrelativistic argument of Jabs. The causal commutators of Quantum Field Theory restrict entanglement to separations of (...)
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  46. Arnold Benz (1997). Die Zukunft des Universums Zufall, Chaos, Gott?
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  47. Ran Ber & Erez Zohar (2016). Remote State Preparation for Quantum Fields. Foundations of Physics 46 (7):804-814.
    Remote state preparation is generation of a desired state by a remote observer. In spite of causality, it is well known, according to the Reeh–Schlieder theorem, that it is possible for relativistic quantum field theories, and a “physical” process achieving this task, involving superoscillatory functions, has recently been introduced. In this work we deal with non-relativistic fields, and show that remote state preparation is also possible for them, hence obtaining a Reeh–Schlieder-like result for general fields. Interestingly, in the nonrelativistic case, (...)
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  48. Sayantani Bera, Sandro Donadi, Kinjalk Lochan & Tejinder P. Singh (2015). A Comparison Between Models of Gravity Induced Decoherence. Foundations of Physics 45 (12):1537-1560.
    It has been suggested in the literature that spatial coherence of the wave function can be dynamically suppressed by fluctuations in the spacetime geometry. These fluctuations represent the minimal uncertainty that is present when one probes spacetime geometry with a quantum probe. Two similar models have been proposed, one by Diósi and one by Karolyhazy and collaborators, based on apparently unrelated minimal spacetime bounds. The two models arrive at somewhat different expressions for the dependence of the localization coherence length on (...)
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  49. Carlton W. Berenda (1945). On Birkhoff's and Einstein's Relativity Theory. Philosophy of Science 12 (2):116-119.
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