International Journal of High Energy Physics

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The Unitary Unified Quantum Field Theory

Received: 13 May 2015    Accepted: 14 May 2015    Published: 09 June 2015
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Abstract

The paper proposes a model of an unitary unified quantum field theory (UUQFT) where the particle is represented as a wave packet. The frequency dispersion equation is chosen so that the packet periodically appears and disappears without changing its form. The envelope of the process is identified with a conventional wave function. Equation of such a field is nonlinear and relativisti cally invariant. With proper adjustments, they are reduced to Dirac, Schrödinger and Hamilton-Jacobi equations. A number of new experimental effects are predicted both for high and low energies.

DOI 10.11648/j.ijhep.s.2015020401.12
Published in International Journal of High Energy Physics (Volume 2, Issue 4-1, August 2015)

This article belongs to the Special Issue Symmetries in Relativity, Quantum Theory, and Unified Theories

Page(s) 8-32
Creative Commons

This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited.

Copyright

Copyright © The Author(s), 2024. Published by Science Publishing Group

Keywords

Wave Packet, Dispersion, Unitary Quantum Theory, Unified Theory, Corpuscular-Wave Dualism, Elementary Particle, Unified Field, Vacuum Fluctuations

References
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[2] Boichenko V.A., Sapogin L.G. (1984). On the Equation of the Unitary Quantum Theory. Annales de la Fondation Louis de Broglie, vol. 9, No.3, p.221.
[3] O.Costa de Beauregard. (1957). Theorie Synthetique de la Relativite Restreinte et des Quanta (Gauther-Villars, Paris, 1957).
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[5] Darwin C.G. (1927). Proc.Roy.Soc., A117, p.258.
[6] Feynman R. etc. (1965). Quantum Mechanics and Path Integrals, McGraw-Hill, New York.
[7] Heisenberg W. (1966). Introduction to the Unified Field Theory of Elementary Particles, Interscience, London, New York, Sydney.
[8] Klauder J.R. etc. (1968). Fundamentals of Quantum Optics,W.A.Benjamin, Inc.,New York, Amsterdam.
[9] Liu W., et al. (1999). Phys. Rev. Lett. v. 82, 711.
[10] Lyamov V.E., Sapogin L.G. (1968) “About the motion of wave packets in dispersive medium”, Journal “Specialnaya radioelectronika”, №1, pр.17-25, Moscow, (Russian).
[11] Maris H.J., (2000). On the Fission of Elementary Particles and the Evidence for the Fractional Electrons in Liquid Helium. Journal of Low Temperature Physics, vol.120, page 173.
[12] Sapogin L.G. (1973). United Field and Quantum Mechanics, System Researches (Physical Researches) Acad. Science USSR, Vladivostok, 2, pp. 54-84, (Russian).
[13] Sapogin L.G. (1979). On Unitary Quantum Mechanics. Nuovo Cimento, vol. 53A, No 2, p.251.
[14] Sapogin L.G. (1980). A Unitary Quantum Field Theory. Annales de la Fondation Louis de Broglie, vol.5, No 4, p.285-300.
[15] Sapogin L.G. (1982). A Statistical Theory of Measurements in Unitary Quantum Mechanics. Nuovo Cimento, vol.70B, No.1, p.80.
[16] Sapogin L.G. (1982). A Statistical Theory of the Detector in Unitary Quantum Mechanics. Nuovo Cimento, vol.71B, No. 3, p.246.
[17] Sapogin L.G., Boichenko V.A. (1988). On the Solution of One Non-linear Equation. Nuovo Cimento, vol.102B, No 4, p.433.
[18] Sapogin L.G., Boichenko V.A. (1991). On the Charge and Mass of Particles in Unitary Quantum Theory. Nuovo Cimento, vol.104A, No 10, p.1483.
[19] Sapogin L.G., Ryabov Yu.A., Utchastkin V.I. (2003). Unitary Quantum Theory and a New Energy Sources. Ed. MADI, Moscow, (Russian).
[20] Sapogin L.G., Ryabov Yu.A, Boichenko V.A. (2005). Unitary Quantum Theory and a New Sources of Energy, Archer Enterprises, Geneva, NY, USA.
[21] Sapogin L.G., Ryabov Yu. A., Boichenko V. A. (2008). Unitary Quantum Theory and a New Sources of Energy, Ed. Science-Press, Moscow, (Russian, transl. from English).
[22] Sapogin L.G., Ryabov Yu. A. (2008). On the mass spectrum of elementary particles in Unitary Quantum Theory, The Old and New Concepts of Physics, Vol. 5, No 3.
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Author Information
  • Department of Physics, Technical University (MADI), Leningradsky pr. 64, Moscow, Russia

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    Leo G. Sapogin. (2015). The Unitary Unified Quantum Field Theory. International Journal of High Energy Physics, 2(4-1), 8-32. https://doi.org/10.11648/j.ijhep.s.2015020401.12

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    ACS Style

    Leo G. Sapogin. The Unitary Unified Quantum Field Theory. Int. J. High Energy Phys. 2015, 2(4-1), 8-32. doi: 10.11648/j.ijhep.s.2015020401.12

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    AMA Style

    Leo G. Sapogin. The Unitary Unified Quantum Field Theory. Int J High Energy Phys. 2015;2(4-1):8-32. doi: 10.11648/j.ijhep.s.2015020401.12

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  • @article{10.11648/j.ijhep.s.2015020401.12,
      author = {Leo G. Sapogin},
      title = {The Unitary Unified Quantum Field Theory},
      journal = {International Journal of High Energy Physics},
      volume = {2},
      number = {4-1},
      pages = {8-32},
      doi = {10.11648/j.ijhep.s.2015020401.12},
      url = {https://doi.org/10.11648/j.ijhep.s.2015020401.12},
      eprint = {https://download.sciencepg.com/pdf/10.11648.j.ijhep.s.2015020401.12},
      abstract = {The paper proposes a model of an unitary unified quantum field theory (UUQFT) where the particle is represented as a wave packet. The frequency dispersion equation is chosen so that the packet periodically appears and disappears without changing its form. The envelope of the process is identified with a conventional wave function. Equation of such a field is nonlinear and relativisti cally invariant. With proper adjustments, they are reduced to Dirac, Schrödinger and Hamilton-Jacobi equations. A number of new experimental effects are predicted both for high and low energies.},
     year = {2015}
    }
    

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    JO  - International Journal of High Energy Physics
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    AB  - The paper proposes a model of an unitary unified quantum field theory (UUQFT) where the particle is represented as a wave packet. The frequency dispersion equation is chosen so that the packet periodically appears and disappears without changing its form. The envelope of the process is identified with a conventional wave function. Equation of such a field is nonlinear and relativisti cally invariant. With proper adjustments, they are reduced to Dirac, Schrödinger and Hamilton-Jacobi equations. A number of new experimental effects are predicted both for high and low energies.
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