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Entangled States and Quantum Causality Threshold in the General Theory of Relativity

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dc.creator Rabounski D.
dc.creator Borissova L.
dc.creator Smarandache F.
dc.date 2005
dc.date.accessioned 2013-06-01T12:14:58Z
dc.date.available 2013-06-01T12:14:58Z
dc.date.issued 2013-06-01
dc.identifier http://www.ptep-online.com/index_files/2005/PP-02-09.PDF
dc.identifier http://www.doaj.org/doaj?func=openurl&genre=article&issn=15555534&date=2005&volume=2&issue=&spage=101
dc.identifier.uri http://koha.mediu.edu.my:8181/jspui/handle/123456789/8806
dc.description This article shows, Synge-Weber's classical problem statement about two particles interacting by a signal can be reduced to the case where the same particle is located in two different points A and B of the basic space-time in the same moment of time, so the states A and B are entangled. This particle, being actual two particles in the entangled states A and B, can interact with itself radiating a photon (signal) in the point A and absorbing it in the point B. That is our goal, to introduce entangled states into General Relativity. Under specific physical conditions the entangled particles in General Relativity can reach a state where neither particle A nor particle B can be the cause of future events. We call this specific state Quantum Causality Threshold.
dc.publisher HEXIS (Arizona, USA)
dc.source Progress in Physics
dc.subject General Relativity
dc.subject Causality Principle
dc.title Entangled States and Quantum Causality Threshold in the General Theory of Relativity


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