Einstein-Podolsky-Rosen-Bohm experiment with massive particles as a test of relativistic center-of-mass position operator

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dc.creatorCzachor, Marek
dc.date1996-03-12
dc.date.accessioned2026-07-07T06:13:47Z
dc.date.available2026-07-07T06:13:47Z
dc.descriptionThe nonrelativistic singlet state average $\langle ψ|{\vec a}\cdot\vec σ\otimes {\vec b}\cdot\vec σ|ψ\rangle =-\vec a\cdot\vec b $ can be relativistically generalized if one defines spin {\it via\/} the relativistic center-of-mass operator. The relativistic correction is quadratic in $v/c$ and can be measured in Einstein-Podolsky-Rosen-Bohm-type experiments with massive spin-1/2 particles. A deviation from the nonrelativistic formula would indicate that for relativistic nonzero-spin particles centers of mass and charge do not coincide.
dc.descriptionrevtex, 3 pages
dc.identifierhttps://arxiv.org/abs/quant-ph/9603017
dc.identifierhttp://arxiv.org/abs/quant-ph/9603017
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/93228
dc.subjectQuantum Physics
dc.titleEinstein-Podolsky-Rosen-Bohm experiment with massive particles as a test of relativistic center-of-mass position operator
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