How to split the electron in one dimension

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dc.creatorKolomeisky, Eugene B.
dc.creatorNewman, T. J.
dc.creatorStraley, J. P.
dc.date2001-03-07
dc.date.accessioned2026-07-07T02:40:42Z
dc.date.available2026-07-07T02:40:42Z
dc.descriptionUsing the example of the Davydov soliton - a large acoustic polaron in one dimension - we demonstrate that the electron wave function can be fissioned in two or more long-lived, well-localized and spatially arbitrarily far separated fragments. The phenomenon of wave function splitting is a result of the electron-medium interaction, and takes place under a variety of conditions provided the initial wave function of the electron is localized and has at least one node.
dc.description4 pages, 2 figures
dc.identifierhttps://arxiv.org/abs/cond-mat/0103174
dc.identifierhttp://arxiv.org/abs/cond-mat/0103174
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/17464
dc.subjectCondensed Matter
dc.subjectQuantum Physics
dc.titleHow to split the electron in one dimension
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