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The Superluminal Interpretation of Quantum Mechanics

Sylwester Kornowski

Published May 1, 2015• 2 citations
OpenAlex

Abstract

Here, within the Scale-Symmetric Physics (S-SP), we present a new interpretation of the Quantum Mechanics i.e. the superluminal interpretation (SIQM). Werner Heisenberg used term “the ideological superstructures” to the hidden-variables theory. All known mainstream interpretations of quantum mechanics deserve such a term. It follows from the fact that all mainstream interpretations neglect physical consistency of the 3-dimensional wave functions. A wave function which fills up the Universe cannot be a coherent physical object when distant points of the wave function cannot communicate with superluminal speed. Just period of a local change in the wave function (due to a luminal Standard-Model interaction) cannot be shorter than size of the wave function divided by superluminal speed. The Planck length is the lower limit for size of gravitating particles. Objects with sizes smaller than the Planck length must be non-gravitating so non-relativistic and they must be superluminal. The S-SP, due to the succeeding phase transitions, leads from the objects with sizes smaller than the Planck length (so superluminal) to objects with sizes close to the Planck length (so luminal) and larger. The question is not whether there are in existence some superluminal entanglons responsible for quantum entanglement but why we cannot see their motion directly. And the answer is very simple just they are not the Standard-Model objects, their size is much smaller than the Planck length and the degree of filling of spacetime is very low. Here, within the Scale-Symmetric Physics (S-SP), [1], we present a new interpretation of the Quantum Mechanics i.e. the superluminal interpretation (SIQM). More details concerning the quantum mechanics in the S-SP we can find in following papers [1] – [10]. Werner Heisenberg used term “the ideological superstructures” to the hidden-variables theory. All known interpretations of quantum mechanics deserve such a term. It follows from the fact that all mainstream interpretations neglect physical consistency of the 3-dimensional wave functions. A wave function which fills up the Universe cannot be a coherent physical object when distant points of the wave function cannot communicate with superluminal speed. Just period of a local change in the wave function (due to a luminal Standard-Model interaction) cannot be shorter than size of the wave function divided by superluminal speed. The shortest luminal lifetimes are about 10– s whereas the present-day size of the Universe is about 10 m – it leads to conclusion that there must be in existence a fifth interaction with speed of interaction higher than about 10 m/s. Only then the quantum mechanics can be

Related papers

General Relativity and Quantum Mechanics as the Theories Dependent on the Observer/Detector

Sylwester Kornowski

General Relativity (GR) and Quantum Mechanics (QM) are the theories dependent on the observer/detector so they are not the theories of the independent from observer Nature. In GR it follows from the fact that each act of observation (the photon-detector interaction via exchanges of the invisible superluminal particles responsible for quantum entanglement i.e. there are exchanged the spin-1 entanglons) sets the speed of light in “vacuum” c in relation to the detector (the speed c is in relation to the emitter or a last-interaction object - sometimes it is a detector). In QM it results from the fact that we cannot observe the entanglons directly and because time of observation lasts much longer than the time of exchanges of the invisible superluminal entanglons so there appear wavefunctions, superposition of states, and probabilities to find a particle in different states. Simultaneity of different states of the same particle is an illusion that appears only in the theories dependent on the observer. There must be in existence a more fundamental theory, which should be a theory of Nature independent on the observer - it is the Scale-Symmetric Theory (SST). SST leads to the initial conditions applied in GR and QM and shows that these theories are dependent on the observer. Moreover, SST shows that we cannot unify GR and QM within the same methods. SST shows that Nature behaves classically in a deterministic way but it does not mean that the free will is not in existence.

•Nov 1, 2016•0 citations

- Many-Worlds or Collapse of the Wave-Function? -

Tejinder P. Singh

At present, there are two possible, and equally plausible, explanations for the physics of quantum measurement. The first explanation, known as the many-worlds interpretation, does not require any modification of quantum mechanics, and asserts that at the time of measurement the Universe splits into many branches, one branch for every possible alternative. The various branches do not interfere with each other because of decoherence, thus providing a picture broadly consistent with the observed Universe. The second explanation, which requires quantum mechanics to be modified from its presently known form, is that at the time of measurement the wave-function collapses into one of the possible alternatives. The two explanations are mutually exclusive, and up until now, no theoretical reasoning has been put forward to choose one explanation over the other. In this article, we provide an argument which implies that the collapse interpretation is favored over the many-worlds interpretation. Our starting point is the assertion (which we justify) that there ought to exist a reformulation of quantum mechanics which does not refer to a classical spacetime manifold. The need for such a reformulation implies that quantum theory becomes non-linear on the Planck mass/energy scale. Standard linear quantum mechanics is an approximation to this non-linear theory, valid at energy scales much smaller than the Planck scale. Using ideas based on noncommutative | >=

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Non-relativistic quantum theory consistent with principle of locality

Isaac Shnaid

Principle of locality means that any local change (perturbation) of the stationary state wave function field propagates with finite speed, and therefore reaches distant regions of the field with time delay. If a one-particle or multi-particle non-relativistic quantum system is initially in a stationary state, and its wave function field is locally perturbed, then perturbed and non-perturbed sub-regions appear in the region. According to Schrödinger equation, borders of the perturbed sub-region propagate with infinite speed, and the perturbation instantaneously affects all infinite region. It means that Schrödinger equation predicts infinite speed of the wave function perturbations propagation. This feature of classical Schrödinger equation is traditionally interpreted as non-locality of quantum mechanics. From physical point of view, such mathematical behavior of Schrödinger equation solutions is questionable because it is difficult to accept that in real world infinite physical objects can instantaneously appear. We introduce a hypothesis that in reality speed of propagation of the perturbed sub-region borders is equal speed of light. On this basis we develop and analyze a finite propagation speed concept for non-relativistic quantum equations. It leads to local interpretation of non-relativistic quantum mechanics consistent with principle of locality and free of local hidden variables. The theory is applied to analysis of Einstein-Podolsky-Rosen (EPR) paradox, entanglement and properties of perturbed matter waves. We proved that formulated theory agrees with results of classical experiments on electron matter waves diffraction.

arXiv:1307.2510•Jul 9, 2013•0 citations

Classical Interpretation of Quantum Mechanics

Sylwester Kornowski

Here we present the physical side of the quantum mechanics (QM) that emerges from the Scale-Symmetric Theory (SST). We showed that the quantum superposition is misinterpreted. The key to understand QM is the difference between quantum coherence and quantum entanglement. We as well explained what conditions and structures lead to relativistic invariants such as electric charge and spin, and how this affects the superposition.

•Dec 1, 2018•0 citations

The World in the Wave Function

David J. Wallace

David Lewis famously quipped that he was willing to take metaphysical lessons from quantum mechanics only when it cleaned up its own act by providing interpretations or modifications of the formalism shorn of appeal to consciousness, irreducibly macroscopic notions, or outright instrumentalism. By the first decade of the twenty-first century, multiple approaches to quantum mechanics had been developed to a degree which met Lewis’s challenge: dynamical-collapse theories, Bohm-style hidden-variable theories, and Everett-style many-worlds theories, for all their respective problems and challenges, all offer ways of understanding quantum mechanics that metaphysicians can reasonably engage with. And so the last twenty years have seen a resurgence in the metaphysics of quantum mechanics, the question of what ontology and ideology is appropriate to a quantum universe. The metaphysics of quantum mechanics is not independent of the quantum measurement problem but does not coincide with it, either: there is a widespread view that adopting, say, the Everett interpretation still leaves significant ontological questions undecided, and conversely, a given answer to those questions might answer them for a dynamical-collapse theory too.Wave function realism has become a leading contender for the metaphysics of quantum mechanics, particularly in the case of dynamical-collapse and Everettian approaches. The starting point is nonrelativistic quantum mechanics expressed in configuration space: mathematically, the subject matter of the theory is a complex function of 3N variables, evolving under the Schrödinger equation (perhaps interrupted by occasional stochastic collapses). Traditionally those 3N variables are interpreted as the three coordinates of position of N particles—but in wave function realism, they are interpreted as points in a new, high-dimensional space. Quantum mechanics, according to the wave function realist, fundamentally concerns the undulations of the wave function in this space; three-dimensional goings-on are emergent, high-level, derivative.Alyssa Ney has been a leading figure in the development of wave function realism for most of its existence. Her articles advocating and developing the position have been highly influential, and the present book can be seen as the culmination of this line of her research and is the definitive statement of wave function realism as of 2021. Despite its comparative brevity, the book is too rich to be adequately described—far less critiqued—in this brief review; my goal is to give an overview of the main themes and arguments, and to make a few critical remarks along the way.The World in the Wavefunction is not formally divided into parts, but it can profitably be thought of that way. Chapters 1 through 3 develop the core case for wave function realism. Chapter 4 defends the position from the frequent criticism that it is restricted to nonrelativistic physics, by providing a version of wave function realism appropriate to quantum field theory. And chapters 5 through 7 are an extended exploration of how the observed three-dimensional world can be understood as emerging from a high-dimensional fundamental reality.The case Ney makes in chapters 1 through 3 for wavefunction realism is modest and cautious. In chapter 1 she provides a fairly standard—though elegantly expressed—case for the prima facie plausibility of wave function realism simply based on the fact that standard formulations of quantum mechanics are written in 3N dimensions, and on the (related) fact that entanglement means we cannot interpret quantum mechanics simply in terms of spatially localized particles and nothing else. But in chapter 2 she explicitly argues against any attempt to strengthen these plausibility arguments into reasons why wave function realism must be adopted; indeed, she provides a detailed and sympathetic taxonomy of the alternatives to wave function realism that have been developed, all of which she regards as entirely viable. (Chapter 2 of the book could profitably be used as introductory reading for a general graduate course on quantum metaphysics.) For Ney, the question of which metaphysics to adopt is a standard metaphysician’s question, to be answered by weighing strengths and weaknesses of the various alternatives against one another.In chapter 3, Ney identifies two such strengths for wave function realism. First, it is separable: we can specify the complete state of the universe point-by-point on the fundamental space, without any need to appeal to irreducible holism. Second, it is dynamically local: expressed in 3N-dimensional space, the Schrödinger dynamics involve no action at a distance.Ney makes the case for separability at length. Her case for dynamical locality is brief: she regards it as a straightforward consequence of the fact that the Schrödinger equation is a differential equation, so that the rate of change of the wave function at a point x depends only on the wave function arbitrarily close to x. But I think there is more worth investigating here: after all, the nonrelativistic Schrödinger equation may be a differential equation, but it is a parabolic differential equation, with no maximum speed of propagation: the rate of change of the wave function at x may depend only on a neighborhood of x, but the value of the wavefunction at x an arbitrarily short time later depends on the wave function everywhere in space. (And this is not—or not straightforwardly—just an artifact of ignoring relativity.)But in any case, why think that a separable, local theory is preferable to the alternative? Ney claims that separability and locality are more intuitive and lead to a more comprehensible ontology—and she makes an unabashed defense of intuitiveness and explicability as theoretical virtues. She is quite explicit that her reasons are pragmatic: intuitive theories benefit students and teachers; they are better suited to help us develop new theories; they speak better to the reasons why many students (Ney included) want to study physics in the first place. The implied metaphilosophy here is fascinating and it would be good to see it developed further in subsequent work: Ney seems to reject the mainstream modern approach to ontology (in which these pragmatic virtues are not obviously relevant to the truth of wave function realism) in favor of something neo-Carnapian where (so far as I can see) the goal of a quantum ontology is to help us get a deeper understanding of quantum mechanics, and that’s all there is to it. This also fits naturally with the pluralism she urges, in which approaches other than hers can also be valuable.Chapter 4—on relativistic generalizations of wavefunction realism—attempts both a conceptual and a technical task. The conceptual task is to argue that wavefunction realism per se is not wedded to any particular theory or choice of Hilbert-space basis within the theory: rather, wave function realism is any strategy that reifies a high-dimensional space in order to produce a separable local quantum ontology. If so, there is no block in principle to a relativistic generalization of the approach: we just need to find some appropriate high-dimensional space to describe the quantum state in relativistic quantum theory.The general philosophical point is well taken and convincingly defended (though it’s important to note that while arbitrary choices of Hilbert-space basis will give a separable theory, there is no reason to assume they will give a dynamically local theory: even something as simple as shifting from the position to the momentum basis in nonrelativistic quantum mechanics transforms the Schrödinger equation into something explicitly nonlocal). Unfortunately, I don’t think Ney succeeds in giving a clear statement of the high-dimensional space she has in mind for quantum field theory. This is one place where her laudable goal of making the book intelligible to nonspecialists becomes problematic: she makes many suggestive and interesting comments on quantum field theory, but there is no explicit, precise, mathematical statement of her view that can be contrasted with the explicit, precise, mathematical representation of the state in nonrelativistic quantum mechanics as a complex function on 3N-dimensional space.In the last part of the book—concerned with the emergence of ordinary three-dimensional ontology—Ney begins (chapter 5) by rebutting influential arguments by Tim Maudlin, Valia Allori, Sheldon Goldstein, and others that it is empirically incoherent for a physical theory not to make precise, nonemergent, nonderivative statements about matter in three-dimensional space (for a theory not to have a primitive ontology, to use the standard term for it). Ney argues—persuasively, to me—that it is perfectly compatible with the way science usually works for a theory to make statements about the observable only in an indirect, derivative way, so that while it might be a desideratum for a theory to have a primitive ontology, it is not compulsory for it to do so in order to be empirically adequate. She goes on, though, to note that a satisfactory quantum metaphysics had better recover the existence of ordinary three-dimensional objects, on Moorean grounds: we are really confident that those objects exist!Chapter 6 is largely critical: an extended exegesis of the functionalist strategy for recovering higher-order ontology developed by David Albert, myself, and others. She raises two main criticisms of the functionalist strategy: it fails to distinguish between the wave function simulating three-dimensional objects and constituting those objects; it is restricted to recovering classical three-dimensional ontology, whereas we want to recover quantum-mechanical phenomena in three dimensions too. (The former objection is a development of criticisms by Bradley Monton, Tim Maudlin, and others; the latter is novel so far as I know.) For reasons of space, I won’t attempt to reply on behalf of the functionalist, but Ney certainly puts the challenge with admirable clarity.The final chapter of the book presents Ney’s positive account of emergent ontology, based not on functionalism but on considerations of symmetry (though she concedes that the separation is not completely sharp). Simplifying Ney’s subtle position: the permutation symmetries of quantum mechanics give a clear dynamical reason to regard certain decompositions of 3N-dimensional space (intuitively: those that decompose it into the N-fold product of Euclidean space) as preferred; that then licenses the metaphysical hypothesis that a localized wave function in 3N-dimensional space has, as its parts, particles in three-dimensional space. If the wave function is not localized (as will be the case generically, at least for the Everett interpretation), then we can think of those particles as being partially localized in various different regions of space.I have to say that I am not convinced this works, at least without a dynamical-collapse mechanism: in the Everett interpretation, it will yield an ontology where all the particles are completely delocalized. We only see a somewhat localized description of matter in three dimensions when we restrict to an Everett branch, and that restriction is normally motivated on functionalist grounds. But this may simply reflect subtleties of Ney’s intriguing proposal that I am not fully grasping at present.In summary, I congratulate Ney for a rich, subtle, and provocative account of wave function realism. Her edited collection of papers (coedited with Albert), The Wave Function, set the agenda for much of the metaphysics of quantum mechanics in the 2010s; The World in the Wave Function has a good chance of doing the same for the 2020s.

The Philosophical Review•Oct 1, 2022•2 citations

Superluminal relativity and physical reality

Guasp Carrascosa, Miguel

This work is a revised version (Version 2) of a previous paper by the author, presented in a manner intended to emphasize more clearly the connection between its epistemological postulates and the subsequent development of its formalism. Several modifications have been introduced, and new sections have been added. As in the first version, the study concerns the physical interpretation of the imaginary quantities that arise in the formulation of superluminal relativity (including complex coordinates, velocities, angles, charges, and masses). In this framework, the kinematics of tachyons is analyzed, and the nature of the imaginary velocities appearing therein is examined. Furthermore, it is shown that a physical interpretation of the complex quantities (masses and charges) occurring both in quantum mechanics and in superluminal relativity is indeed possible. In this context, the complex nature of the electric charge is investigated, with particular attention to its divisibility. It is demonstrated that singular fractions of the electric charge exist whose squared values coincide with the observed quark charges. Within the same conceptual framework, the physical nature of a complex mass is also explored. It is shown that the imaginary component of such a mass implies that its gravitational field intensity behaves as a wave, propagating with the velocity of the wave associated with the particle itself. It is further demonstrated that the corresponding wavelength coincides with that given by the De Broglie relation, and that the resulting wave equation—second order in both spatial and temporal coordinates—is compatible with the Klein–Gordon wave equation. This constitutes a significant indication of the physical character of the associated wave and suggests an alternative interpretation to the orthodox probabilistic view of quantum mechanics.

•Nov 14, 2025•0 citations
Here, within the Scale-Symmetric Physics (S-SP), we present a new interpretation of the Quantum Mechanics i.e. the superluminal interpretation (SIQM). Werner Heisenberg used term “the ideological superstructures” to the hidden-variables theory. All known mainstream interpretations of quantum mechanics deserve such a term. It follows from the fact that all mainstream interpretations neglect physical consistency of the 3-dimensional wave functions. A wave function which fills up the Universe cannot be a coherent physical object when distant points of the wave function cannot communicate with superluminal speed. Just period of a local change in the wave function (due to a luminal Standard-Model interaction) cannot be shorter than size of the wave function divided by superluminal speed. The Planck length is the lower limit for size of gravitating particles. Objects with sizes smaller than the Planck length must be non-gravitating so non-relativistic and they must be superluminal. The S-SP, due to the succeeding phase transitions, leads from the objects with sizes smaller than the Planck length (so superluminal) to objects with sizes close to the Planck length (so luminal) and larger. The question is not whether there are in existence some superluminal entanglons responsible for quantum entanglement but why we cannot see their motion directly. And the answer is very simple just they are not the Standard-Model objects, their size is much smaller than the Planck length and the degree of filling of spacetime is very low. Here, within the Scale-Symmetric Physics (S-SP), [1], we present a new interpretation of the Quantum Mechanics i.e. the superluminal interpretation (SIQM). More details concerning the quantum mechanics in the S-SP we can find in following papers [1] – [10]. Werner Heisenberg used term “the ideological superstructures” to the hidden-variables theory. All known interpretations of quantum mechanics deserve such a term. It follows from the fact that all mainstream interpretations neglect physical consistency of the 3-dimensional wave functions. A wave function which fills up the Universe cannot be a coherent physical object when distant points of the wave function cannot communicate with superluminal speed. Just period of a local change in the wave function (due to a luminal Standard-Model interaction) cannot be shorter than size of the wave function divided by superluminal speed. The shortest luminal lifetimes are about 10– s whereas the present-day size of the Universe is about 10 m – it leads to conclusion that there must be in existence a fifth interaction with speed of interaction higher than about 10 m/s. Only then the quantum mechanics can be
General Relativity (GR) and Quantum Mechanics (QM) are the theories dependent on the observer/detector so they are not the theories of the independent from observer Nature. In GR it follows from the fact that each act of observation (the photon-detector interaction via exchanges of the invisible superluminal particles responsible for quantum entanglement i.e. there are exchanged the spin-1 entanglons) sets the speed of light in “vacuum” c in relation to the detector (the speed c is in relation to the emitter or a last-interaction object - sometimes it is a detector). In QM it results from the fact that we cannot observe the entanglons directly and because time of observation lasts much longer than the time of exchanges of the invisible superluminal entanglons so there appear wavefunctions, superposition of states, and probabilities to find a particle in different states. Simultaneity of different states of the same particle is an illusion that appears only in the theories dependent on the observer. There must be in existence a more fundamental theory, which should be a theory of Nature independent on the observer - it is the Scale-Symmetric Theory (SST). SST leads to the initial conditions applied in GR and QM and shows that these theories are dependent on the observer. Moreover, SST shows that we cannot unify GR and QM within the same methods. SST shows that Nature behaves classically in a deterministic way but it does not mean that the free will is not in existence.
At present, there are two possible, and equally plausible, explanations for the physics of quantum measurement. The first explanation, known as the many-worlds interpretation, does not require any modification of quantum mechanics, and asserts that at the time of measurement the Universe splits into many branches, one branch for every possible alternative. The various branches do not interfere with each other because of decoherence, thus providing a picture broadly consistent with the observed Universe. The second explanation, which requires quantum mechanics to be modified from its presently known form, is that at the time of measurement the wave-function collapses into one of the possible alternatives. The two explanations are mutually exclusive, and up until now, no theoretical reasoning has been put forward to choose one explanation over the other. In this article, we provide an argument which implies that the collapse interpretation is favored over the many-worlds interpretation. Our starting point is the assertion (which we justify) that there ought to exist a reformulation of quantum mechanics which does not refer to a classical spacetime manifold. The need for such a reformulation implies that quantum theory becomes non-linear on the Planck mass/energy scale. Standard linear quantum mechanics is an approximation to this non-linear theory, valid at energy scales much smaller than the Planck scale. Using ideas based on noncommutative | >=
Principle of locality means that any local change (perturbation) of the stationary state wave function field propagates with finite speed, and therefore reaches distant regions of the field with time delay. If a one-particle or multi-particle non-relativistic quantum system is initially in a stationary state, and its wave function field is locally perturbed, then perturbed and non-perturbed sub-regions appear in the region. According to Schrödinger equation, borders of the perturbed sub-region propagate with infinite speed, and the perturbation instantaneously affects all infinite region. It means that Schrödinger equation predicts infinite speed of the wave function perturbations propagation. This feature of classical Schrödinger equation is traditionally interpreted as non-locality of quantum mechanics. From physical point of view, such mathematical behavior of Schrödinger equation solutions is questionable because it is difficult to accept that in real world infinite physical objects can instantaneously appear. We introduce a hypothesis that in reality speed of propagation of the perturbed sub-region borders is equal speed of light. On this basis we develop and analyze a finite propagation speed concept for non-relativistic quantum equations. It leads to local interpretation of non-relativistic quantum mechanics consistent with principle of locality and free of local hidden variables. The theory is applied to analysis of Einstein-Podolsky-Rosen (EPR) paradox, entanglement and properties of perturbed matter waves. We proved that formulated theory agrees with results of classical experiments on electron matter waves diffraction.
David Lewis famously quipped that he was willing to take metaphysical lessons from quantum mechanics only when it cleaned up its own act by providing interpretations or modifications of the formalism shorn of appeal to consciousness, irreducibly macroscopic notions, or outright instrumentalism. By the first decade of the twenty-first century, multiple approaches to quantum mechanics had been developed to a degree which met Lewis’s challenge: dynamical-collapse theories, Bohm-style hidden-variable theories, and Everett-style many-worlds theories, for all their respective problems and challenges, all offer ways of understanding quantum mechanics that metaphysicians can reasonably engage with. And so the last twenty years have seen a resurgence in the metaphysics of quantum mechanics, the question of what ontology and ideology is appropriate to a quantum universe. The metaphysics of quantum mechanics is not independent of the quantum measurement problem but does not coincide with it, either: there is a widespread view that adopting, say, the Everett interpretation still leaves significant ontological questions undecided, and conversely, a given answer to those questions might answer them for a dynamical-collapse theory too.Wave function realism has become a leading contender for the metaphysics of quantum mechanics, particularly in the case of dynamical-collapse and Everettian approaches. The starting point is nonrelativistic quantum mechanics expressed in configuration space: mathematically, the subject matter of the theory is a complex function of 3N variables, evolving under the Schrödinger equation (perhaps interrupted by occasional stochastic collapses). Traditionally those 3N variables are interpreted as the three coordinates of position of N particles—but in wave function realism, they are interpreted as points in a new, high-dimensional space. Quantum mechanics, according to the wave function realist, fundamentally concerns the undulations of the wave function in this space; three-dimensional goings-on are emergent, high-level, derivative.Alyssa Ney has been a leading figure in the development of wave function realism for most of its existence. Her articles advocating and developing the position have been highly influential, and the present book can be seen as the culmination of this line of her research and is the definitive statement of wave function realism as of 2021. Despite its comparative brevity, the book is too rich to be adequately described—far less critiqued—in this brief review; my goal is to give an overview of the main themes and arguments, and to make a few critical remarks along the way.The World in the Wavefunction is not formally divided into parts, but it can profitably be thought of that way. Chapters 1 through 3 develop the core case for wave function realism. Chapter 4 defends the position from the frequent criticism that it is restricted to nonrelativistic physics, by providing a version of wave function realism appropriate to quantum field theory. And chapters 5 through 7 are an extended exploration of how the observed three-dimensional world can be understood as emerging from a high-dimensional fundamental reality.The case Ney makes in chapters 1 through 3 for wavefunction realism is modest and cautious. In chapter 1 she provides a fairly standard—though elegantly expressed—case for the prima facie plausibility of wave function realism simply based on the fact that standard formulations of quantum mechanics are written in 3N dimensions, and on the (related) fact that entanglement means we cannot interpret quantum mechanics simply in terms of spatially localized particles and nothing else. But in chapter 2 she explicitly argues against any attempt to strengthen these plausibility arguments into reasons why wave function realism must be adopted; indeed, she provides a detailed and sympathetic taxonomy of the alternatives to wave function realism that have been developed, all of which she regards as entirely viable. (Chapter 2 of the book could profitably be used as introductory reading for a general graduate course on quantum metaphysics.) For Ney, the question of which metaphysics to adopt is a standard metaphysician’s question, to be answered by weighing strengths and weaknesses of the various alternatives against one another.In chapter 3, Ney identifies two such strengths for wave function realism. First, it is separable: we can specify the complete state of the universe point-by-point on the fundamental space, without any need to appeal to irreducible holism. Second, it is dynamically local: expressed in 3N-dimensional space, the Schrödinger dynamics involve no action at a distance.Ney makes the case for separability at length. Her case for dynamical locality is brief: she regards it as a straightforward consequence of the fact that the Schrödinger equation is a differential equation, so that the rate of change of the wave function at a point x depends only on the wave function arbitrarily close to x. But I think there is more worth investigating here: after all, the nonrelativistic Schrödinger equation may be a differential equation, but it is a parabolic differential equation, with no maximum speed of propagation: the rate of change of the wave function at x may depend only on a neighborhood of x, but the value of the wavefunction at x an arbitrarily short time later depends on the wave function everywhere in space. (And this is not—or not straightforwardly—just an artifact of ignoring relativity.)But in any case, why think that a separable, local theory is preferable to the alternative? Ney claims that separability and locality are more intuitive and lead to a more comprehensible ontology—and she makes an unabashed defense of intuitiveness and explicability as theoretical virtues. She is quite explicit that her reasons are pragmatic: intuitive theories benefit students and teachers; they are better suited to help us develop new theories; they speak better to the reasons why many students (Ney included) want to study physics in the first place. The implied metaphilosophy here is fascinating and it would be good to see it developed further in subsequent work: Ney seems to reject the mainstream modern approach to ontology (in which these pragmatic virtues are not obviously relevant to the truth of wave function realism) in favor of something neo-Carnapian where (so far as I can see) the goal of a quantum ontology is to help us get a deeper understanding of quantum mechanics, and that’s all there is to it. This also fits naturally with the pluralism she urges, in which approaches other than hers can also be valuable.Chapter 4—on relativistic generalizations of wavefunction realism—attempts both a conceptual and a technical task. The conceptual task is to argue that wavefunction realism per se is not wedded to any particular theory or choice of Hilbert-space basis within the theory: rather, wave function realism is any strategy that reifies a high-dimensional space in order to produce a separable local quantum ontology. If so, there is no block in principle to a relativistic generalization of the approach: we just need to find some appropriate high-dimensional space to describe the quantum state in relativistic quantum theory.The general philosophical point is well taken and convincingly defended (though it’s important to note that while arbitrary choices of Hilbert-space basis will give a separable theory, there is no reason to assume they will give a dynamically local theory: even something as simple as shifting from the position to the momentum basis in nonrelativistic quantum mechanics transforms the Schrödinger equation into something explicitly nonlocal). Unfortunately, I don’t think Ney succeeds in giving a clear statement of the high-dimensional space she has in mind for quantum field theory. This is one place where her laudable goal of making the book intelligible to nonspecialists becomes problematic: she makes many suggestive and interesting comments on quantum field theory, but there is no explicit, precise, mathematical statement of her view that can be contrasted with the explicit, precise, mathematical representation of the state in nonrelativistic quantum mechanics as a complex function on 3N-dimensional space.In the last part of the book—concerned with the emergence of ordinary three-dimensional ontology—Ney begins (chapter 5) by rebutting influential arguments by Tim Maudlin, Valia Allori, Sheldon Goldstein, and others that it is empirically incoherent for a physical theory not to make precise, nonemergent, nonderivative statements about matter in three-dimensional space (for a theory not to have a primitive ontology, to use the standard term for it). Ney argues—persuasively, to me—that it is perfectly compatible with the way science usually works for a theory to make statements about the observable only in an indirect, derivative way, so that while it might be a desideratum for a theory to have a primitive ontology, it is not compulsory for it to do so in order to be empirically adequate. She goes on, though, to note that a satisfactory quantum metaphysics had better recover the existence of ordinary three-dimensional objects, on Moorean grounds: we are really confident that those objects exist!Chapter 6 is largely critical: an extended exegesis of the functionalist strategy for recovering higher-order ontology developed by David Albert, myself, and others. She raises two main criticisms of the functionalist strategy: it fails to distinguish between the wave function simulating three-dimensional objects and constituting those objects; it is restricted to recovering classical three-dimensional ontology, whereas we want to recover quantum-mechanical phenomena in three dimensions too. (The former objection is a development of criticisms by Bradley Monton, Tim Maudlin, and others; the latter is novel so far as I know.) For reasons of space, I won’t attempt to reply on behalf of the functionalist, but Ney certainly puts the challenge with admirable clarity.The final chapter of the book presents Ney’s positive account of emergent ontology, based not on functionalism but on considerations of symmetry (though she concedes that the separation is not completely sharp). Simplifying Ney’s subtle position: the permutation symmetries of quantum mechanics give a clear dynamical reason to regard certain decompositions of 3N-dimensional space (intuitively: those that decompose it into the N-fold product of Euclidean space) as preferred; that then licenses the metaphysical hypothesis that a localized wave function in 3N-dimensional space has, as its parts, particles in three-dimensional space. If the wave function is not localized (as will be the case generically, at least for the Everett interpretation), then we can think of those particles as being partially localized in various different regions of space.I have to say that I am not convinced this works, at least without a dynamical-collapse mechanism: in the Everett interpretation, it will yield an ontology where all the particles are completely delocalized. We only see a somewhat localized description of matter in three dimensions when we restrict to an Everett branch, and that restriction is normally motivated on functionalist grounds. But this may simply reflect subtleties of Ney’s intriguing proposal that I am not fully grasping at present.In summary, I congratulate Ney for a rich, subtle, and provocative account of wave function realism. Her edited collection of papers (coedited with Albert), The Wave Function, set the agenda for much of the metaphysics of quantum mechanics in the 2010s; The World in the Wave Function has a good chance of doing the same for the 2020s.
This work is a revised version (Version 2) of a previous paper by the author, presented in a manner intended to emphasize more clearly the connection between its epistemological postulates and the subsequent development of its formalism. Several modifications have been introduced, and new sections have been added. As in the first version, the study concerns the physical interpretation of the imaginary quantities that arise in the formulation of superluminal relativity (including complex coordinates, velocities, angles, charges, and masses). In this framework, the kinematics of tachyons is analyzed, and the nature of the imaginary velocities appearing therein is examined. Furthermore, it is shown that a physical interpretation of the complex quantities (masses and charges) occurring both in quantum mechanics and in superluminal relativity is indeed possible. In this context, the complex nature of the electric charge is investigated, with particular attention to its divisibility. It is demonstrated that singular fractions of the electric charge exist whose squared values coincide with the observed quark charges. Within the same conceptual framework, the physical nature of a complex mass is also explored. It is shown that the imaginary component of such a mass implies that its gravitational field intensity behaves as a wave, propagating with the velocity of the wave associated with the particle itself. It is further demonstrated that the corresponding wavelength coincides with that given by the De Broglie relation, and that the resulting wave equation—second order in both spatial and temporal coordinates—is compatible with the Klein–Gordon wave equation. This constitutes a significant indication of the physical character of the associated wave and suggests an alternative interpretation to the orthodox probabilistic view of quantum mechanics.