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Physics Letters B

Generalized beable quantum field theory

Shasanka Mohan Roy, Virendra Singh

Published Jan 1, 1990• 9 citations
Publisher
DOI
10.1016/0370-2693(90)92013-9

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We present a way to construct a pilot‐wave model for quantum field theory. The idea is to introduce beables corresponding only to the bosonic degrees of freedom and not to the fermionic degrees of freedom of the quantum state. We provide an illustration and a justification of this idea in the context of quantum electrodynamics. The beables are fields and correspond to the degrees of freedom of the electromagnetic field. The field beables are introduced in a similar way to that of Bohm’s model for the free electromagnetic field. Our approach is analogous to the situation in non‐relativistic quantum theory, where Bell treated spin not as a beable but only as a property of the wavefunction.

arXiv:quant-ph/0602229•AIP conference proceedings•Jan 1, 2006•30 citations
In this thesis we study the de Broglie-Bohm pilot-wave interpretation of quantum theory. We consider the domain of non-relativistic quantum theory, relativistic quantum theory and quantum field theory, and in each domain we consider the possibility of formulating a pilot-wave interpretation. For non-relativistic quantum theory a pilot-wave interpretation in terms of particle beables can readily be formulated. But this interpretation can in general not straightforwardly be generalized to relativistic wave equations. The problems which prevent us from devising a pilot-wave interpretation for relativistic wave equations also plague the standard quantum mechanical interpretation, where these problems led to the conception of quantum field theory. Therefore most of our attention is focussed on the construction of a pilot-wave interpretation for quantum field theory. We thereby favour the field beable approach, developed amongst others by Bohm, Hiley, Holland, Kaloyerou and Valentini. Although the field beable approach can be successfully applied to bosonic quantum field theory, it seems not straightforward to do so for fermionic quantum field theory.
Beable-guided quantum theories (BGQT) are generalizations of quantum theory, inspired by Bell's concept of beables. They modify the quantum probabilities for some specified set of fundamental events, histories, or other elements of quasiclassical reality by probability laws that depend on the realized configuration of beables. For example, they may define an additional probability weight factor for a beable configuration, independent of the quantum dynamics. Beable-guided quantum theories can be fitted to observational data to provide foils against which to compare explanations based on standard quantum theory. For example, a BGQT could, in principle, characterize the effects attributed to dark energy or dark matter, or any other deviation from the predictions of standard quantum dynamics, without introducing extra fields or a cosmological constant. The complexity of the beable-guided theory would then parametrize how far we are from a standard quantum explanation. Less conservatively, we give reasons for taking suitably simple beable-guided quantum theories as serious phenomenological theories in their own right. Among these are the possibility that cosmological models defined by BGQT might in fact fit the empirical data better than any standard quantum explanation, and the fact that BGQT suggest potentially interesting nonstandard ways of coupling quantum matter to gravity.
We present a way to construct a pilot‐wave model for quantum field theory. The idea is to introduce beables corresponding only to the bosonic degrees of freedom and not to the fermionic degrees of freedom of the quantum state. We provide an illustration and a justification of this idea in the context of quantum electrodynamics. The beables are fields and correspond to the degrees of freedom of the electromagnetic field. The field beables are introduced in a similar way to that of Bohm’s model for the free electromagnetic field. Our approach is analogous to the situation in non‐relativistic quantum theory, where Bell treated spin not as a beable but only as a property of the wavefunction.