A finite model for electrodynamics by introducing a form factor fHD2(ℓ2□)=1+(-ℓ2□)2 into the kinetic term of Maxwell theory
In this paper, a higher-derivative model for electrodynamics is presented in a D+1 dimensional Minkowski space-time by introducing a form factor into the kinetic term of Maxwell theory as -1/4µ0 FµνFµν→ -1/4µ0 FµνFHD2(ℓ2□)Fµν , where is a characteristic length scale. Our calculations show that for...
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Published in: | Iranian Journal of Physics Research Vol. 23; no. 2; pp. 429 - 442 |
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Main Authors: | , |
Format: | Journal Article |
Language: | English Persian |
Published: |
Isfahan University of Technology
01-09-2023
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Subjects: | |
Online Access: | Get full text |
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Summary: | In this paper, a higher-derivative model for electrodynamics is presented in a D+1 dimensional Minkowski space-time by introducing a form factor into the kinetic term of Maxwell theory as -1/4µ0 FµνFµν→ -1/4µ0 FµνFHD2(ℓ2□)Fµν , where is a characteristic length scale. Our calculations show that for DÊÎ{3, 4, 5} the electrostatic potential of a point charge is finite at the position of the point charge in this higher-derivative modification of Maxwell's theory. For D=3 the explicit form of the potential and the electric field of a point charge are obtained analytically in this higher-derivative electrodynamics. According to numerical estimations, the upper bound for the characteristic length scale ℓ is ℓmax ~1/100ℓelectroweak , where ℓelectroweak= 10-18m is the electroweak length scale. Finally, it should be emphasized that for ℓ<<1 the results of this paper are compatible with the results of ordinary Maxwell theory. |
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ISSN: | 1682-6957 2345-3664 |
DOI: | 10.47176/ijpr.23.2.71720 |