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Linear Stochastic Electrodynamics [PDF]
, 1996 In the foregoing chapter it was observed that the use of a conventional perturbative approach in SED leads to unperturbed solutions obeying classical equations of motion, whereas they should be stochastic and somehow contain ‟, if they are expected to describe the quantum world; in other words, that not even the zero-order motions of the sed system in ...
Luis de la Peña, Ana María Cetto
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Excited states in stochastic electrodynamics
Physical Review A, 1988We show that the set of Wigner functions associated with the excited states of the harmonic oscillator constitutes a complete set of functions over the phase space. An arbitrary probability distribution can be expanded in terms of these Wigner functions.
H. M. França, T.W. Marshall
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The physics of stochastic electrodynamics
Il Nuovo Cimento B, 1986The problem of the electron immersed in the random zeropoint radiation field and described by the stochastic Abraham-Lorentz equation is analysed from a new point of view. First an approximate treatment of the (statistically) stationary motion of this system is performed by using a local linearization procedure applicable to nonlinear periodic problems.
Ana María Cetto, L. de la Peña
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The Pullback Mechanism in Stochastic Electrodynamics
AIP Conference Proceedings, 2007An argument is given why the classical theory called Stochastic Electrodynamics may reproduce scattering and ionization experiments of electrons on atomic hydrogen.
Th. M. Nieuwenhuizen +5 more
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Spin and paramagnetism in classical stochastic electrodynamics
Physical Review A, 1989Etude des proprietes statistiques du spin S et du dipole magnetique pr d'une particule a 2 constituants lies par une force harmonique. On determine la relation entre S et μ et conclut que ∼h 2 . Le systeme contient des forces paramagnetiques et une comparaison avec l'experience montre un excellent accord avec l'electrodynamique ...
A. V. Barranco +2 more
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The propagator of stochastic electrodynamics
Physical Review D, 1981The ''elementary propagator'' for the position of a free charged particle subject to the zero-point electromagnetic field with Lorentz-invariant spectral density proportional..omega../sup 3/ is obtained. The nonstationary process for the position is solved by the stationary process for the acceleration.
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The Foundations of Linear Stochastic Electrodynamics
Foundations of Physics, 2006An analysis is briefly presented of the possible causes of the failure of stochastic electrodynamics (SED) when applied to systems with nonlinear forces, on the basis that the main principles of the theory are correct. In light of this analysis, an alternative approach to the theory is discussed, whose postulates allow to establish contact with quantum
Ana María Cetto +2 more
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Stochastic electrodynamics for the free particle
Journal of Mathematical Physics, 1983The theory of stochastic electrodynamics is applied to the free particle and to the particle moving in a homogeneous field, leading to a complete temperature- and time-dependent description in phase space. After a transient time, the marginal description in configuration space coincides entirely with quantum mechanics, while the phase-space description
A. Jáuregui, L. de la Peña
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The extended charge in stochastic electrodynamics
Il Nuovo Cimento B Series 11, 1985We derive a covariant equation for the motion of the extended charge and show how a consistent description is achieved for nonrelativistic velocities. If the external force is generated by the classical stochastic zero-point electromagnetic field, the equation of motion has the form of a Langevin equation with memory.
G. C. Santos, H. M. França
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Lie algebras of classical and stochastic electrodynamics
International Journal of Theoretical Physics, 1994The Lie algebras associated with infinitesimal symmetry transformations of third-order differential equations of interest to classical electrodynamics and stochastic electrodynamics have been obtained. The structure constants for a general case are presented and the Lie algebra for each particular application is easily achieved. By the method used here
J. D. M. Vianna, J. J. Soares Neto
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