Quantum particles from classical probabilities in phase space
Quantum particles in a potential are described by classical statistical probabilities. We formulate a basic time evolution law for the probability distribution of classical position and momentum such that all known quantum phenomena follow, including interference or tunneling. The appropriate quantu...
Gespeichert in:
| 1. Verfasser: | |
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| Dokumenttyp: | Article (Journal) |
| Sprache: | Englisch |
| Veröffentlicht: |
October 2012
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| In: |
International journal of theoretical physics
Year: 2012, Jahrgang: 51, Heft: 10, Pages: 3236-3273 |
| ISSN: | 1572-9575 |
| DOI: | 10.1007/s10773-012-1205-8 |
| Online-Zugang: | Verlag, Volltext: http://dx.doi.org/10.1007/s10773-012-1205-8 Verlag, Volltext: https://link.springer.com/article/10.1007/s10773-012-1205-8 
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| Verfasserangaben: | C. Wetterich |
MARC
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| 520 | |a Quantum particles in a potential are described by classical statistical probabilities. We formulate a basic time evolution law for the probability distribution of classical position and momentum such that all known quantum phenomena follow, including interference or tunneling. The appropriate quantum observables for position and momentum contain a statistical part which reflects the roughness of the probability distribution. “Zwitters” realize a continuous interpolation between quantum and classical particles. Such objects may provide for an effective one-particle description of classical or quantum collective states as droplets of a liquid, macromolecules or a Bose-Einstein condensate. They may also be used for quantitative fundamental tests of quantum mechanics. We show that the ground state for zwitters has no longer a sharp energy. This feature permits to put quantitative experimental bounds on a small parameter for possible deviations from quantum mechanics. | ||
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