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  • Articles  (5)
  • electrodynamics  (3)
  • electromagnetism  (2)
  • Physics  (5)
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  • Articles  (5)
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  • Physics  (5)
  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Foundations of physics 7 (1994), S. 67-74 
    ISSN: 1572-9524
    Keywords: ghost field ; photomagneton ; electromagnetism
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The concepts are introduced of the longitudinal ghost fieldB (3) and photomagnetonB (3)) of electromagnetism:B (3) = 〈B(3)〉 =B(0)〈Ĵ〉/ħ, whereB (0) is the magnetic flux density amplitude andĴ the angular momentum operator of a photon beam. The major implication is that the individual photon hasthree degrees of polarization, the longitudinal one being accompanied by the ghost fieldB (3) which has no energy or linear momentum, and is generated from the angular momentum of the photon.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Foundations of physics 7 (1994), S. 379-384 
    ISSN: 1572-9524
    Keywords: photomagneton ; induction ; electrodynamics
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The recently proposed free space photomagneton, $$\hat B^{(3)} $$ , of electromagnetic radiation produces no intrinsic Faraday induction in a vacuum, but in matter produces phase free magnetization in the inverse Faraday effect.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    Foundations of physics 7 (1994), S. 209-217 
    ISSN: 1572-9524
    Keywords: phtomagneton ; electrodynamics ; conservation laws
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract It is shown that the basic electrodynamical conservation laws are unaffected by the presence in free space of the photomagneton of light, $$\hat B^{\left( 3 \right)} = B^{\left( 0 \right)} \hat J/\rlap{--} h$$ , the fundamental photon property responsible for magnetization by light. The expectation value $$B^{\left( 3 \right)} = \left\langle {\hat B^{\left( 3 \right)} } \right\rangle $$ does not affect the Poynting vector, so that it does not contribute to electromagnetic flux density. The electromagnetic energy density can be expressed in terms ofB (3) through the equation $$\rlap{--} h\omega = \frac{1}{{\mu _0 }}\smallint B^{\left( 3 \right)} \cdot B^{\left( 3 \right) * } dV.$$ When light magnetizes matter, the unitB (3) of magnetic flux density per photon is transferred from light to matter. This is equivalent to an elastic transfer of angular momentum. Experimental indications for the existence ofB (3) are discussed.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    Springer
    Foundations of physics 9 (1996), S. 463-473 
    ISSN: 1572-9524
    Keywords: B (3) field ; gravitation ; electromagnetism ; unification
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The emergence of theB (3) field in vacuo has shown that electromagnetism is non-Abelian and similar in structure to gravitation. In this paper the Christoffel symbol used in general relativity is developed for electromagnetism in curvilinear coordinates: The former becomes describable as the antisymmetric part of the gravitational Ricci tensor. Therefore gravitation and electromagnetism are respectively the symmetric and antisymmetric parts of thesame Ricci tensor within a proportionality factor. Both fields are obtained from the Riemann curvature tensor, both are expressions of curvature in spacetime.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    Springer
    Foundations of physics 9 (1996), S. 397-405 
    ISSN: 1572-9524
    Keywords: electrodynamics ; gravitation ; unification ; B (3) field ; Ricci tensor
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The equations of free-space electrodynamics are derived directly from the Riemann curvature tensor and the Bianchi identity of general relativity by contracting on two indices to give a novel antisymmetric Ricci tensor. Within a factore/h, this is the field-strength tensor Gμν of free-space electrodynamics. The Bianchi identity for Gμν describes free-space electrodynamics in a manner analogous to, but more general than, Maxwell's equations for electrodynamics, the critical difference being the existence in general and special relativity of the Evans-Vigier fieldB (3).
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