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  • Articles  (5)
  • electrodynamics  (3)
  • photon mass  (2)
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  • Articles  (5)
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  • 1
    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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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Foundations of physics 8 (1995), S. 279-286 
    ISSN: 1572-9524
    Keywords: B (3) field ; photon mass
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The connection between finite photon mass and the fieldB (3) is developed with reference to special relativity in the vacuum. The existence of the physical and longitudinal fieldB (3) implies that there are three degrees of polarization associated with the photon, which cannot therefore be a massless boson. The fieldB (3) can be observed experimentally through the magnetization of a plasma with microwave pulses, and this experiment serves to demonstrate unequivocally the existence of photon mass.
    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 8 (1995), S. 83-92 
    ISSN: 1572-9524
    Keywords: B (3) field ; photon mass
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The longitudinal vacuum fieldB (3) is an experimental observable which produces by magnetization a well-defined square-root beam power density dependence. Its longitudinal polarization implies that the helicities of the photon are +1, 0, and −1, and that the little group of the Poincaré group is the rotation group 0(3) of a massive boson. The mass of the photon (m) is therefore related directly toB (3) through the Proca equation, and it is concluded that experimental evidence forB (3) is also evidence for finitem.
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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).
    Type of Medium: Electronic Resource
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