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 |
|