Role of the Electromagnetic Vacuum in the Transition from Classical to Quantum Mechanics

We revisit the nonrelativistic problem of a bound, charged particle subject to the random zero-point radiation field ( zpf ), with the purpose of revealing the mechanism that takes it from the initially classical description to the final quantum-mechanical one. The combined effect of the zpf and the...

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Bibliographic Details
Published inFoundations of physics Vol. 52; no. 4
Main Authors Cetto, Ana María, de la Peña, Luis
Format Journal Article
LanguageEnglish
Published New York Springer US 01.08.2022
Springer Nature B.V
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Summary:We revisit the nonrelativistic problem of a bound, charged particle subject to the random zero-point radiation field ( zpf ), with the purpose of revealing the mechanism that takes it from the initially classical description to the final quantum-mechanical one. The combined effect of the zpf and the radiation reaction force results, after a characteristic time lapse, in the loss of the initial conditions and the concomitant irreversible transition of the dynamics to a stationary regime controlled by the field. In this regime, the canonical variables x ,  p become expressed in terms of the dipolar response functions to a set of field modes. A proper ordering of the response coefficients leads to the matrix representation of quantum mechanics, as was proposed in the early days of the theory, and to the basic commutator x ^ , p ^ = i ħ . Further, the connection with the corresponding Fokker–Planck equation valid in the Markov approximation, allows one to obtain the (nonrelativistic) radiative corrections of qed . These results reaffirm the essentially electrodynamic and stochastic nature of the quantum phenomenon, as proposed by stochastic electrodynamics.
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ISSN:0015-9018
1572-9516
DOI:10.1007/s10701-022-00605-6