TY - JOUR

T1 - Infrared catastrophe averted by Hertz potential

AU - Zwanziger, Daniel

N1 - Copyright:
Copyright 2015 Elsevier B.V., All rights reserved.

PY - 1979

Y1 - 1979

N2 - A computational scheme for quantum electrodynamics is developed from first principles in which infrared divergences are not encountered. The gist of the method is that the photon propagator is properly -igμν(k2+iε)-1[(12)kσkσ)]wln(-λ-2k2-iε). Here λ is a parameter which plays the role of the photon mass, but which cancels out of cross sections for any finite value (λ→0 is never taken). The subscript w means weak derivative, so a partial integration on k, with neglect of boundary terms, is always understood in Feynman integrals. This makes integrals converge which otherwise would be logarithmically divergent. For sufficiently convergent integrals the partial integration may be undone and the conventional value results because [(12)kσkσ)]ln(-λ-2k2-iε)=1.. It is shown that the above propagator is not merely an artificial device, but results if the vector potential Aμ is derived from a Hertz potential Πλμ=-Πμλ, Aμ=μΠλμ, which is a local field. The real-photon infrared divergences do not occur when the integral over real photons is obtained from the discontinuity in the k0 plane of the above propagator. A contribution to the real-photon integral at strictly zero frequency, resembling a third polarization state of the photon, is isolated and evaluated explicitly. The S matrix and physical subspaces are defined.

AB - A computational scheme for quantum electrodynamics is developed from first principles in which infrared divergences are not encountered. The gist of the method is that the photon propagator is properly -igμν(k2+iε)-1[(12)kσkσ)]wln(-λ-2k2-iε). Here λ is a parameter which plays the role of the photon mass, but which cancels out of cross sections for any finite value (λ→0 is never taken). The subscript w means weak derivative, so a partial integration on k, with neglect of boundary terms, is always understood in Feynman integrals. This makes integrals converge which otherwise would be logarithmically divergent. For sufficiently convergent integrals the partial integration may be undone and the conventional value results because [(12)kσkσ)]ln(-λ-2k2-iε)=1.. It is shown that the above propagator is not merely an artificial device, but results if the vector potential Aμ is derived from a Hertz potential Πλμ=-Πμλ, Aμ=μΠλμ, which is a local field. The real-photon infrared divergences do not occur when the integral over real photons is obtained from the discontinuity in the k0 plane of the above propagator. A contribution to the real-photon integral at strictly zero frequency, resembling a third polarization state of the photon, is isolated and evaluated explicitly. The S matrix and physical subspaces are defined.

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U2 - 10.1103/PhysRevD.19.3614

DO - 10.1103/PhysRevD.19.3614

M3 - Article

AN - SCOPUS:33744612382

SN - 1550-7998

VL - 19

SP - 3614

EP - 3634

JO - Physical review D: Particles and fields

JF - Physical review D: Particles and fields

IS - 12

ER -