Self-Localized Quasi-Particle Excitation in Quantum Electrodynamics and Its Physical Interpretation

The self-localized quasi-particle excitation of the electron-positron field (EPF) is found for the first time in the framework of a standard form of the quantum electrodynamics. This state is interpreted as the ''physical'' electron (positron) and it allows one to solve the follo...

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Published in:Symmetry, Integrability and Geometry: Methods and Applications
Date:2007
Main Authors: Feranchuk, I.D., Feranchuk, S.I.
Format: Article
Language:English
Published: Інститут математики НАН України 2007
Online Access:https://nasplib.isofts.kiev.ua/handle/123456789/147222
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Journal Title:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Cite this:Self-Localized Quasi-Particle Excitation in Quantum Electrodynamics and Its Physical Interpretation / I.D. Feranchuk, S.I. Feranchuk // Symmetry, Integrability and Geometry: Methods and Applications. — 2007. — Т. 3. — Бібліогр.: 37 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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author Feranchuk, I.D.
Feranchuk, S.I.
author_facet Feranchuk, I.D.
Feranchuk, S.I.
citation_txt Self-Localized Quasi-Particle Excitation in Quantum Electrodynamics and Its Physical Interpretation / I.D. Feranchuk, S.I. Feranchuk // Symmetry, Integrability and Geometry: Methods and Applications. — 2007. — Т. 3. — Бібліогр.: 37 назв. — англ.
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container_title Symmetry, Integrability and Geometry: Methods and Applications
description The self-localized quasi-particle excitation of the electron-positron field (EPF) is found for the first time in the framework of a standard form of the quantum electrodynamics. This state is interpreted as the ''physical'' electron (positron) and it allows one to solve the following problems: i) to express the ''primary'' charge e0 and the mass m0 of the ''bare'' electron in terms of the observed values of e and m of the ''physical'' electron without any infinite parameters and by essentially nonperturbative way; ii) to consider μ-meson as another self-localized EPF state and to estimate the ratio mμ/m; iii) to prove that the self-localized state is Lorentz-invariant and its energy spectrum corresponds to the relativistic free particle with the observed mass m; iv) to show that the expansion in a power of the observed charge e << 1 corresponds to the strong coupling expansion in a power of the ''primary'' charge e₀⁻¹ ~ e when the interaction between the ''physical'' electron and the transverse electromagnetic field is considered by means of the perturbation theory and all terms of this series are free from the ultraviolet divergence.
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institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
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last_indexed 2025-12-07T17:12:52Z
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spelling Feranchuk, I.D.
Feranchuk, S.I.
2019-02-13T19:20:42Z
2019-02-13T19:20:42Z
2007
Self-Localized Quasi-Particle Excitation in Quantum Electrodynamics and Its Physical Interpretation / I.D. Feranchuk, S.I. Feranchuk // Symmetry, Integrability and Geometry: Methods and Applications. — 2007. — Т. 3. — Бібліогр.: 37 назв. — англ.
1815-0659
2000 Mathematics Subject Classification: 81V05; 81V10; 83C47
https://nasplib.isofts.kiev.ua/handle/123456789/147222
The self-localized quasi-particle excitation of the electron-positron field (EPF) is found for the first time in the framework of a standard form of the quantum electrodynamics. This state is interpreted as the ''physical'' electron (positron) and it allows one to solve the following problems: i) to express the ''primary'' charge e0 and the mass m0 of the ''bare'' electron in terms of the observed values of e and m of the ''physical'' electron without any infinite parameters and by essentially nonperturbative way; ii) to consider μ-meson as another self-localized EPF state and to estimate the ratio mμ/m; iii) to prove that the self-localized state is Lorentz-invariant and its energy spectrum corresponds to the relativistic free particle with the observed mass m; iv) to show that the expansion in a power of the observed charge e << 1 corresponds to the strong coupling expansion in a power of the ''primary'' charge e₀⁻¹ ~ e when the interaction between the ''physical'' electron and the transverse electromagnetic field is considered by means of the perturbation theory and all terms of this series are free from the ultraviolet divergence.
This paper is a contribution to the Proceedings of the Seventh International Conference “Symmetry in Nonlinear Mathematical Physics” (June 24–30, 2007, Kyiv, Ukraine). Authors are grateful to ICTP Of fice of External Activities for the financial support of the participation in the International Conference “Symmetry in Nonlinear Mathematical Physics” (June 24–30, 2007, Kyiv, Ukraine).
en
Інститут математики НАН України
Symmetry, Integrability and Geometry: Methods and Applications
Self-Localized Quasi-Particle Excitation in Quantum Electrodynamics and Its Physical Interpretation
Article
published earlier
spellingShingle Self-Localized Quasi-Particle Excitation in Quantum Electrodynamics and Its Physical Interpretation
Feranchuk, I.D.
Feranchuk, S.I.
title Self-Localized Quasi-Particle Excitation in Quantum Electrodynamics and Its Physical Interpretation
title_full Self-Localized Quasi-Particle Excitation in Quantum Electrodynamics and Its Physical Interpretation
title_fullStr Self-Localized Quasi-Particle Excitation in Quantum Electrodynamics and Its Physical Interpretation
title_full_unstemmed Self-Localized Quasi-Particle Excitation in Quantum Electrodynamics and Its Physical Interpretation
title_short Self-Localized Quasi-Particle Excitation in Quantum Electrodynamics and Its Physical Interpretation
title_sort self-localized quasi-particle excitation in quantum electrodynamics and its physical interpretation
url https://nasplib.isofts.kiev.ua/handle/123456789/147222
work_keys_str_mv AT feranchukid selflocalizedquasiparticleexcitationinquantumelectrodynamicsanditsphysicalinterpretation
AT feranchuksi selflocalizedquasiparticleexcitationinquantumelectrodynamicsanditsphysicalinterpretation