Separation of Bell states
| dc.creator | Sanctuary, B. C. | |
| dc.date | 2007-05-24 | |
| dc.date | 2009-02-15 | |
| dc.date.accessioned | 2026-07-07T12:41:07Z | |
| dc.date.available | 2026-07-07T12:41:07Z | |
| dc.description | The four Bell states can be represented by separable coherent states which are products of individual non-hermitian spin operators. In the absence of interactions, the non-hermitian states are predicted to form a new quantum state of spin magnitude 1/sqrt(2) rather than 1/2. Properties of these states show that an isolated spin is a resonance state with zero net angular momentum, consistent with a point particle. In addition, the Bell states are shown to take on the identical mathematical form when the two spins are bound (local) or unbound (non-local). The bound Bell states are resonances between four states. When the separate, they do so from only one of its resonance states and their ensemble average defines the unbound Bell states. The bound and unbound Bell states have the same mathematical form due to the persistence of the rotationally invariance of sigma(1)dot sigma(2). | |
| dc.description | 14 pages, no figures, complete re-write of previous submission | |
| dc.identifier | https://arxiv.org/abs/0705.3657 | |
| dc.identifier | http://arxiv.org/abs/0705.3657 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/219661 | |
| dc.subject | General Physics | |
| dc.title | Separation of Bell states | |
| dc.type | text |