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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Published in | Foundations of physics Vol. 52; no. 4 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
New York
Springer US
01.08.2022
Springer Nature B.V |
Subjects | |
Online Access | Get full text |
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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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Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 14 |
ISSN: | 0015-9018 1572-9516 |
DOI: | 10.1007/s10701-022-00605-6 |