Tunneling as a classical escape rate induced by the vacuum zero-point radiation

dc.creatorFaria, A. J.
dc.creatorFranca, H. M.
dc.creatorSponchiado, R. C.
dc.date2004-09-17
dc.date.accessioned2026-07-07T06:10:53Z
dc.date.available2026-07-07T06:10:53Z
dc.descriptionWe make a brief review of the Kramers escape rate theory for the probabilistic motion of a particle in a potential well U(x), and under the influence of classical fluctuation forces. The Kramers theory is extended in order to take into account the action of the thermal and zero-point random electromagnetic fields on a charged particle. The result is physically relevant because we get a non null escape rate over the potential barrier at low temperatures (T -> 0). It is found that, even if the mean energy is much smaller than the barrier height, the classical particle can escape from the potential well due to the action of the zero-point fluctuating fields. These stochastic effects can be used to give a classical interpretation to some quantum tunneling phenomena. Relevant experimental data are used to illustrate the theoretical results.
dc.description11 pages, 3 figures. To be published in "Quanta, Relativity and Electromagnetism: The Search for Unity in Physics", Proceedings of a Symposium in Honor of Jean-Pierre Vigier (Paris, September, 2003). Kluwer Academic Publishers
dc.identifierhttps://arxiv.org/abs/quant-ph/0409119
dc.identifierhttp://arxiv.org/abs/quant-ph/0409119
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/92378
dc.subjectQuantum Physics
dc.titleTunneling as a classical escape rate induced by the vacuum zero-point radiation
dc.typetext

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