2020
DOI: 10.3390/physics2010002
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QED Response of the Vacuum

Abstract: We present a new perspective on the link between quantum electrodynamics (QED) and Maxwell’s equations. We demonstrate that the interpretation of the electric displacement vector D = ε 0 E , where E is the electric field vector and ε 0 is the permittivity of the vacuum, as vacuum polarization is consistent with QED. A free electromagnetic field polarizes the vacuum, but the polarization and magnetization currents cancel giving zero source current. The speed of light is a universal consta… Show more

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Cited by 6 publications
(5 citation statements)
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“…The above calculation is compatible with quantum electrodynamics, as is also the calculation by Leuchs et al [33]. Now N(t) = N 0 e −Γ p−Ps t , where N 0 and N(t) are, respectively, the number of photonexcited parapositronium VFs at the initial time t = 0 and the later time t. It then follows that N(t)/N 0 = e −Γ p−Ps t is the probability that a photon-excited parapositronium VF has not decayed electromagnetically during a time t. The probability that photon-excited parapositronium VF has decayed during the time t is 1 − N(t)/N 0 = 1 − e −Γ p−Ps t .…”
Section: Calculation Of the Density Of Parapositronium Vfs Available ...supporting
confidence: 84%
“…The above calculation is compatible with quantum electrodynamics, as is also the calculation by Leuchs et al [33]. Now N(t) = N 0 e −Γ p−Ps t , where N 0 and N(t) are, respectively, the number of photonexcited parapositronium VFs at the initial time t = 0 and the later time t. It then follows that N(t)/N 0 = e −Γ p−Ps t is the probability that a photon-excited parapositronium VF has not decayed electromagnetically during a time t. The probability that photon-excited parapositronium VF has decayed during the time t is 1 − N(t)/N 0 = 1 − e −Γ p−Ps t .…”
Section: Calculation Of the Density Of Parapositronium Vfs Available ...supporting
confidence: 84%
“…The diverging vacuum polarization integral may be handled by effective running permittivity ( ) 0 r ε instead of renormalizing the electric charge [14]. The vacuum polarization one-loop Feynman diagram for an electron-positron pair is shown below as a reference for the proposed pion tetrahedron Td π vacuum polarization Feynman diagram (Figure 9).…”
Section: Pion Tetrahedron and Vacuum Polarizationmentioning
confidence: 99%
“…Charge, linear momentum, and angular momentum are conserved, so annihilation of a photon is accompanied by creation of a particle-antiparticle pair, as illustrated in Figure 2. An important point for the goal of this study is that the current induced in the vacuum by the four-potential, A µ , due to virtual pairs can be expressed as [46]…”
Section: Figurementioning
confidence: 99%
“…This leads to a result that seems to be physically unreasonable: the photon mass is infinite [48], and the contribution of the virtual electron-positron pairs to the vacuum polarization diverges. However, on the other hand, this diverging vacuum susceptibility makes sense because of the screening of a point charge in a dielectric [46]. The observable, or effective charge, positioned in the vacuum is given by e 2 eff = e 2 bare /χ vac (k 2 , Λ).…”
Section: Figurementioning
confidence: 99%