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This paper addresses fundamental theoretical challenges in relativistic Bohmian mechanics by resolving an objection regarding the normalization of space-time configuration density using a new "Arrangement Function." The work is significant for foundational quantum physics research as it seeks to validate probability interpretations within covariant models, directly advancing our understanding of deterministic formulations in quantum theory.
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A Reponse to the Sheldon Goldstein Objection to a Series of Covariant Relativistic Bohmian Models

arXiv3 min read

arXiv:2607.16928v1 Announce Type: new Abstract: In this work we try to answer a very important objection to the Covariant Bohmian Models type Nikoli\'c and Hern\'andez-Zapata that was formulated by the american physicist Sheldon Goldstein (private communication, 2010) about the imposibility to interpret the configuration space-time density found by the authors of these models like a probability density. The problem is that it is very dificult to show that the N space-time configuration density has a finite integral. That is very important in order to normalize the density to produce a PDF (probability density function). All the steps in the demonstrations seemed complete but this objection must be resolved imperatively before to continue using this kind of models with full confidence. Since the aim of Bohmian Mechanics (also known as the De Broglie-Bohm Mechanics) is to provide a precise and objective formulation of Quantum Mechanics free from vagueness and obscurity (Bell point of view at least), addressing this issue is crucial. In this article, we set out to tackle this by employing a specific type of function that we call an "Arrangement Function".

Abstract:In this work we try to answer a very important objection to the Covariant Bohmian Models type Nikolić and Hernández-Zapata that was formulated by the american physicist Sheldon Goldstein (private communication, 2010) about the imposibility to interpret the configuration space-time density found by the authors of these models like a probability density. The problem is that it is very dificult to show that the N space-time configuration density has a finite integral. That is very important in order to normalize the density to produce a PDF (probability density function). All the steps in the demonstrations seemed complete but this objection must be resolved imperatively before to continue using this kind of models with full confidence. Since the aim of Bohmian Mechanics (also known as the De Broglie-Bohm Mechanics) is to provide a precise and objective formulation of Quantum Mechanics free from vagueness and obscurity (Bell point of view at least), addressing this issue is crucial. In this article, we set out to tackle this by employing a specific type of function that we call an "Arrangement Function".

arXiv:2607.16928 [quant-ph]

(or arXiv:2607.16928v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2607.16928 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 268 words

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