This paper presents, for general relativistic case, a theoretical study of Compton effect in the field of a circularly polarized wave under resonant condition β resonances related to a virtual intermediate particle that falls within the mass shell. We derive the expressions for the resonant amplitud
Comment on the longitudinal magnetic field of circularly polarized electromagnetic waves
β Scribed by E. Comay
- Publisher
- Elsevier Science
- Year
- 1996
- Tongue
- English
- Weight
- 264 KB
- Volume
- 261
- Category
- Article
- ISSN
- 0009-2614
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β¦ Synopsis
Consideration of the radiation from a rotating electric dipole leads to the inference that the existence of the recently suggested B (3) longitudinal magnetic field implies a real electric field which increases indefinitely as time elapses. This conclusion is obtained by integrating the magnetic flux around a closed path at the wave zone. The integration yields a non-zero result by virtue of the assumed existence of the B (3) longitudinal field. Thence using Stokes's theorem, Maxwell's equation VΓ B = aE/at completes the proof. Such an electric field is excluded in the theory of the B (3) field, and its increasing nature makes it physically unrealistic. Thus the existence of the B (3) longitudinal magnetic field is inconsistent with Maxwell's theory of electromagnetism.
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