Understanding entanglement and resolving the measurement problem
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arXiv
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| Format: | Preprint |
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2025
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| _version_ | 1866915354940276736 |
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| author | Hobson, Art |
| author_facet | Hobson, Art |
| contents | We summarize a recently proposed resolution of the quantum measurement problem. It stems from an insight into entanglement demonstrated in a 1991 experiment involving photon momenta. This experiment shows that, when two superposed quantum systems A and B are entangled, the resulting "pre-measurement state" is not a paradoxical macroscopic superposition of compound states of the two subsystems; for example, Schrodinger's cat is not "smeared" between dead and alive. It is instead a non-local superposition of correlations between states of the subsystems. In Schrodinger's example, an undecayed nucleus is correlated with a live cat, AND a decayed nucleus is correlated with a dead cat, where "AND" indicates the superposition on. This is exactly what we want. We have misinterpreted "dyads" |A> |B> where "A" and "B" are subsystems of a composite system AB. A> |B> does not mean states |A> and |B> both exist. It means instead |B> exists if and only |A> exists, i.e. |A> and |B> are correlated. It is a fact of nature that such correlations are nonlocally coherent: The degree of correlation between A and B depends on the nonlocal phase angle between the arbitrarily distant subsystems. Such coherent correlations are central to the nonlocal collapse of wave functions. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2506_18181 |
| institution | arXiv |
| publishDate | 2025 |
| record_format | arxiv |
| spellingShingle | Understanding entanglement and resolving the measurement problem Hobson, Art Quantum Physics We summarize a recently proposed resolution of the quantum measurement problem. It stems from an insight into entanglement demonstrated in a 1991 experiment involving photon momenta. This experiment shows that, when two superposed quantum systems A and B are entangled, the resulting "pre-measurement state" is not a paradoxical macroscopic superposition of compound states of the two subsystems; for example, Schrodinger's cat is not "smeared" between dead and alive. It is instead a non-local superposition of correlations between states of the subsystems. In Schrodinger's example, an undecayed nucleus is correlated with a live cat, AND a decayed nucleus is correlated with a dead cat, where "AND" indicates the superposition on. This is exactly what we want. We have misinterpreted "dyads" |A> |B> where "A" and "B" are subsystems of a composite system AB. A> |B> does not mean states |A> and |B> both exist. It means instead |B> exists if and only |A> exists, i.e. |A> and |B> are correlated. It is a fact of nature that such correlations are nonlocally coherent: The degree of correlation between A and B depends on the nonlocal phase angle between the arbitrarily distant subsystems. Such coherent correlations are central to the nonlocal collapse of wave functions. |
| title | Understanding entanglement and resolving the measurement problem |
| topic | Quantum Physics |
| url | https://arxiv.org/abs/2506.18181 |