Anomalous Magnetic Moment of the Electron without QED
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2026
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| _version_ | 1866901861103042560 |
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| author | Zamboni, Lino |
| author_facet | Zamboni, Lino |
| contents | <p>In 1965, the Nobel Prize was awarded for the modern formulation of Quantum <br>Electrodynamics (QED) to R.P. Feynman for his diagrammatic method, J. Schwinger for the <br>operator method, and S.-I. Tomonaga for his relativistic derivation. Subsequently, P. Kusch <br>performed a precise measurement of the electron's anomalous magnetic moment, <br>providing a critical test validating QED's computational methods, which proved to be <br>extremely accurate. <br>Nevertheless, QED is based on a physically unrealistic assumption—mathematically <br>circumvented—that the electron is a dimensionless point particle endowed with physical <br>properties "ex abrupto." <br>This work, developed within a deterministic and non-local dBBZ (modified de Broglie–Bohm) <br>theory, models the electron as an entangled and distributed structure, as proposed in <br>previous studies. It enables the calculation of the electron's anomalous magnetic moment <br>as a consequence of its intrinsic structure, without employing QED techniques. <br>The method involves calculating, for each orbital, the anomalous moment modified to <br>account for the influence of existing magnetic fields. Subsequently, entanglement is <br>imposed on the sum of these moments, and from the total orbital anomalous moment thus <br>obtained, the theoretical magnetic anomaly is derived and compared with the <br>corresponding experimental value, yielding relative errors on the order of 10^-12. <br>This procedure, which allows for greater theoretical precision than current methods, <br>necessitates a similar, albeit more complex, calculation of the muon's anomalous magnetic <br>moment. This is because a specific parameter, termed the "source parameter," selected <br>within an allowable range, requires dual verification to be adopted with high precision. <br>The theoretical determination of the muon's anomalous magnetic moment is also <br>presented in a subsequent document, employing analogous computational procedures.</p> <p> </p> |
| format | Recurso digital |
| id | zenodo_https___doi_org_10_5281_zenodo_19181914 |
| institution | Zenodo |
| language | eng |
| publishDate | 2026 |
| publisher | Zenodo |
| record_format | zenodo |
| spellingShingle | Anomalous Magnetic Moment of the Electron without QED Zamboni, Lino Electron anomalous magnetic moment , intra-particle entanglement , structured electron model , Bohmiam mechanics extension , quantum electrodynamics alternative , precision calculation . <p>In 1965, the Nobel Prize was awarded for the modern formulation of Quantum <br>Electrodynamics (QED) to R.P. Feynman for his diagrammatic method, J. Schwinger for the <br>operator method, and S.-I. Tomonaga for his relativistic derivation. Subsequently, P. Kusch <br>performed a precise measurement of the electron's anomalous magnetic moment, <br>providing a critical test validating QED's computational methods, which proved to be <br>extremely accurate. <br>Nevertheless, QED is based on a physically unrealistic assumption—mathematically <br>circumvented—that the electron is a dimensionless point particle endowed with physical <br>properties "ex abrupto." <br>This work, developed within a deterministic and non-local dBBZ (modified de Broglie–Bohm) <br>theory, models the electron as an entangled and distributed structure, as proposed in <br>previous studies. It enables the calculation of the electron's anomalous magnetic moment <br>as a consequence of its intrinsic structure, without employing QED techniques. <br>The method involves calculating, for each orbital, the anomalous moment modified to <br>account for the influence of existing magnetic fields. Subsequently, entanglement is <br>imposed on the sum of these moments, and from the total orbital anomalous moment thus <br>obtained, the theoretical magnetic anomaly is derived and compared with the <br>corresponding experimental value, yielding relative errors on the order of 10^-12. <br>This procedure, which allows for greater theoretical precision than current methods, <br>necessitates a similar, albeit more complex, calculation of the muon's anomalous magnetic <br>moment. This is because a specific parameter, termed the "source parameter," selected <br>within an allowable range, requires dual verification to be adopted with high precision. <br>The theoretical determination of the muon's anomalous magnetic moment is also <br>presented in a subsequent document, employing analogous computational procedures.</p> <p> </p> |
| title | Anomalous Magnetic Moment of the Electron without QED |
| topic | Electron anomalous magnetic moment , intra-particle entanglement , structured electron model , Bohmiam mechanics extension , quantum electrodynamics alternative , precision calculation . |
| url | https://doi.org/10.5281/zenodo.19181914 |