Rationalization of EPR Coincidence Experiments
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arXiv
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| Format: | Preprint |
| Publié: |
2007
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| _version_ | 1866915222296461312 |
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| author | Sanctuary, B. C. |
| author_facet | Sanctuary, B. C. |
| contents | Coincidence experiments on EPR pairs show strong violations of Bell's Inequalities at certain filter settings which is widely believed to mean that local hidden variable models cannot explain these results. In this paper it is shown that the 'non-separable' singlet density matrix can be represented as a sum of separable density matrices which are products of individual non-hermitian spin operator states. This decomposition is consistent with the intuitive notion that after separation from the singlet the two physical systems should be described by a product state. In spite of the non-hermiticity, the values of the relevant spin observables are real. A new local hidden variable model inspired by this decomposition is discussed. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_0710_1910 |
| institution | arXiv |
| publishDate | 2007 |
| record_format | arxiv |
| spellingShingle | Rationalization of EPR Coincidence Experiments Sanctuary, B. C. General Physics Coincidence experiments on EPR pairs show strong violations of Bell's Inequalities at certain filter settings which is widely believed to mean that local hidden variable models cannot explain these results. In this paper it is shown that the 'non-separable' singlet density matrix can be represented as a sum of separable density matrices which are products of individual non-hermitian spin operator states. This decomposition is consistent with the intuitive notion that after separation from the singlet the two physical systems should be described by a product state. In spite of the non-hermiticity, the values of the relevant spin observables are real. A new local hidden variable model inspired by this decomposition is discussed. |
| title | Rationalization of EPR Coincidence Experiments |
| topic | General Physics |
| url | https://arxiv.org/abs/0710.1910 |