Stochastic electrodynamics

From Wikipedia, the free encyclopedia
For other uses, see SED (disambiguation).


Stochastic electrodynamics (SED) is extends classical electrodynamics (CED) of theoretical physics by adding the hypothesis of a classical Lorentz invariant radiation field having statistical properties similar to that of the electromagnetic zero-point field (ZPF) of quantum electrodynamics (QED).

Key ingredients[edit]

Stochastic electrodynamics combines two convention classical ideas – electromagnetism derived from point charges obeying Maxwell's equations and particle motion driven by Lorentz forces – with one unconventional hypothesis: the classical field has radiation even at T=0. This zero-point radiation is inferred from observations of the (macroscopic) Casimir effect forces at low-temperature. As temperature approaches zero, experimental measurements of the force between two uncharged, conducting plates in a vacuum do not go to zero as classical electrodynamics would predict. Taking this result as evidence of classical zero-point radiation leads to the stochastic electrodynamics model.[1]

Brief history[edit]

Part of a series of articles about
Quantum mechanics
Schrödinger equation
Background
Fundamentals
Experiments
Formulations
Equations
Interpretations
Advanced topics
Scientists

Stochastic electrodynamics is a term for a collection of research efforts of many different styles based on the ansatz that there exists a Lorentz invariant random electromagnetic radiation. The basic ideas have been around for a long time; but Marshall (1963) and Brafford seem to have been the originators of the more concentrated efforts starting in the 1960s.[2] Thereafter Timothy Boyer, Luis de la Peña and Ana María Cetto were perhaps the most prolific contributors in the 1970s and beyond.[3][4][5][6][7][8][9][10][11] Others have made contributions, alterations and proposals concentrating on the application of SED to problems in QED. A separate thread has been the investigation of an earlier proposal by Walther Nernst attempting to use the SED notion of a classical ZPF to explain inertial mass as due to a vacuum reaction.

In 2010, Cavalleri et al. introduced SEDS ('pure' SED, as they call it, plus spin) as a fundamental improvement which they claim potentially overcomes all the known drawbacks to SED. They also claim SEDS resolves four observed effects that are so far unexplained by QED, i.e., 1) the physical origin of the ZPF, and its natural upper cutoff; 2) an anomaly in experimental studies of the neutrino rest mass; 3) the origin and quantitative treatment of 1/f noise; and 4) the high-energy tail (~ 1021 eV) of cosmic rays. Two double-slit electron diffraction experiments are proposed to discriminate between QM and SEDS.[12]

In 2013 Auñon et al. showed that Casimir and Van der Waals interactions are a particular case of stochastic forces from electromagnetic sources when the broad Planck's spectrum is chosen and the wavefields are non-correlated.[13] Addressing fluctuating partially coherent light emitters with a tailored spectral energy distribution in the optical range, this establishes the link between stochastic electrodynamics and coherence theory;[14] henceforth putting forward a way to optically create and control both such zero-point fields as well as Lifshitz forces [15] of thermal fluctuations. In addition, this opens the path to build many more stochastic forces on employing narrow-band light sources for bodies with frequency-dependent responses.

Scope of SED[edit]

SED has been used in attempts to provide a classical explanation for effects previously considered to require quantum mechanics (here restricted to the Schrödinger equation and the Dirac equation and QED) for their explanation. It has also been used to motivate a classical ZPF-based underpinning for gravity and inertia. There is no universal agreement on the successes and failures of SED, either in its congruence with standard theories of quantum mechanics, QED, and gravity, or in its compliance with observation. The following SED-based explanations are relatively uncontroversial and are free of criticism at the time of writing:

The following SED-based calculations and SED-related claims are more controversial and some have been subject to published criticism:

See also[edit]

References[edit]

  1. ^ Boyer, Timothy H. (March 2019). "Stochastic Electrodynamics: The Closest Classical Approximation to Quantum Theory". Atoms. 7 (1): 29. arXiv:1903.00996. Bibcode:2019Atoms...7...29B. doi:10.3390/atoms7010029. ISSN 2218-2004.
  2. ^ Marshall, T. W. (1963). "Random Electrodynamics". Proceedings of the Royal Society A. 276 (1367): 475–491. Bibcode:1963RSPSA.276..475M. doi:10.1098/rspa.1963.0220. S2CID 202575160.
  3. ^ Boyer, Timothy H. (1975). "Random electrodynamics: The theory of classical electrodynamics with classical electromagnetic zero-point radiation". Phys. Rev. D. 11 (4): 790–808. Bibcode:1975PhRvD..11..790B. doi:10.1103/PhysRevD.11.790.
  4. ^ Boyer, T. H. (1980). "A Brief Survey of Stochastic Electrodynamics". Foundations of Radiation Theory and Quantum Electrodynamics. pp. 49–64. ISBN 0-306-40277-7.
  5. ^ Boyer, Timothy H. (1985). "The Classical Vacuum". Scientific American. 253 (2): 70–78. Bibcode:1985SciAm.253b..70B. doi:10.1038/scientificamerican0885-70.
  6. ^ de la Pena, L. & Cetto, A. M. (1996). The Quantum Dice: An Introduction to Stochastic Electrodynamics. Dordrecht: Kluwer. ISBN 0-7923-3818-9. OCLC 33281109. ISBN 0-7923-3818-9
  7. ^ de la Pena, L. & Cetto, A. M. (2005). "Contribution from stochastic electrodynamics to the understanding of quantum mechanics". arXiv:quant-ph/0501011.
  8. ^ Pena, Luis de la; Cetto, Ana Maria; Valdes-Hernandez, Andrea (2014). The Emerging Quantum: The Physics Behind Quantum Mechanics. p. 19. doi:10.1007/978-3-319-07893-9. ISBN 978-3-319-07892-2.
  9. ^ de la Peña, L.; Cetto, A. M.; Valdés-Hernandes, A. (2014). "The zero-point field and the emergence of the quantum". International Journal of Modern Physics E. 23 (9): 1450049. Bibcode:2014IJMPE..2350049D. doi:10.1142/S0218301314500499. ISSN 0218-3013.
  10. ^ de la Peña, L.; Cetto, A. M.; Valdés-Hernandes, A. (2014). Theo M Nieuwenhuizen; Claudia Pombo; Claudio Furtado; Andrei Yu Khrennikov; Inácio A Pedrosa; Václav Špička (eds.). Quantum Foundations and Open Quantum Systems: Lecture Notes of the Advanced School. World Scientific. p. 399. ISBN 978-981-4616-74-4.
  11. ^ Grössing, Gerhard (2014). "Emergence of quantum mechanics from a sub-quantum statistical mechanics". International Journal of Modern Physics B. 28 (26): 1450179. arXiv:1304.3719. Bibcode:2014IJMPB..2850179G. doi:10.1142/S0217979214501793. ISSN 0217-9792. S2CID 119180551.
  12. ^ Giancarlo Cavalleri; Francesco Barbero; Gianfranco Bertazzi; Eros Cesaroni; Ernesto Tonni; Leonardo Bosi; Gianfranco Spavieri & George Gillies (2010). "A quantitative assessment of stochastic electrodynamics with spin (SEDS): Physical principles and novel applications". Frontiers of Physics in China. 5 (1): 107–122. Bibcode:2010FrPhC...5..107C. doi:10.1007/s11467-009-0080-0. S2CID 121408910.
  13. ^ Juan Miguel Auñon; Cheng Wei Qiu; Manuel Nieto-Vesperinas (2013). "Tailoring photonic forces on a magnetodielectric nanoparticle with a fluctuating optical source" (PDF). Physical Review A. 88 (4): 043817. Bibcode:2013PhRvA..88d3817A. doi:10.1103/PhysRevA.88.043817. hdl:10261/95567.
  14. ^ Leonard Mandel; Emil Wolf (1995). Optical Coherence and Quantum Optics. Cambridge, UK: Cambridge University Press. ISBN 9780521417112.
  15. ^ E. M. Lifshitz, Dokl. Akad. Nauk SSSR 100, 879 (1955).
  16. ^ Boyer, T. H. (1973). "Retarded van der Waals forces at all distances derived from classical electrodynamics with classical electromagnetic zero-point radiation". Physical Review A. 7 (6): 1832–40. Bibcode:1973PhRvA...7.1832B. doi:10.1103/PhysRevA.7.1832.
  17. ^ Boyer, T. H. (1973). "Diamagnetism of a free particle in classical electron theory with classical electromagnetic zero-point radiation". Physical Review A. 21 (1): 66–72. Bibcode:1980PhRvA..21...66B. doi:10.1103/PhysRevA.21.66.
  18. ^ Boyer, T. H. (1980). "Thermal effects of acceleration through random classical radiation". Physical Review D. 21 (8): 2137–48. Bibcode:1980PhRvD..21.2137B. doi:10.1103/PhysRevD.21.2137.
  19. ^ M. Ibison; B. Haisch (1996). "Quantum and Classical Statistics of the Electromagnetic Zero-Point Field". Physical Review A. 54 (4): 2737–2744. arXiv:quant-ph/0106097. Bibcode:1996PhRvA..54.2737I. doi:10.1103/PhysRevA.54.2737. PMID 9913785. S2CID 2104654.
  20. ^ H. E. Puthoff (1987). "Ground state of hydrogen as a zero-point-fluctuation-determined state". Physical Review D. 35 (20): 3266–3269. Bibcode:1987PhRvD..35.3266P. doi:10.1103/PhysRevD.35.3266. PMID 9957575.
  21. ^ Kracklauer, A. F. (1999). "Pilot Wave Steerage: A Mechanism and Test". Foundations of Physics Letters. 12 (2): 441–453. doi:10.1023/A:1021629310707. S2CID 18510049.
  22. ^ B. Haisch; A. Rueda; H. E. Puthoff (1994). "Inertia as a zero-point-field Lorentz force". Physical Review A. 49 (2): 678–694. Bibcode:2009PhRvA..79a2114L. doi:10.1103/PhysRevA.79.012114. PMID 9910287.
  23. ^ J-L. Cambier (January 2009). "Inertial Mass from Stochastic Electrodynamics". In M. Millis; E. Davis (eds.). Frontiers of Propulsion Science (Progress in Astronautics and Aeronautics). AIAA. pp. 423–454. ISBN 9781563479564.
  24. ^ A. D. Sakharov (1968). "Vacuum Quantum Fluctuations in Curved Space and the Theory of Gravitation". Soviet Physics Doklady. 12: 1040. Bibcode:1968SPhD...12.1040S.


Retrieved from "https://en.wikipedia.org/w/index.php?title=Stochastic_electrodynamics&oldid=1207489206"