Abstract
AN atom is in an excited state S′ with energy E′. It falls to a state S with lower energy E and emits a photon with frequency v. According to a basic postulate of quantum mechanics, this frequency is related to the energies by The theoretical calculation of E and E′ is carried out in the rest-frame of the atom, and so it would appear that v in equation (1) is the frequency observed in that frame. Conservation of momentum, however, demands that the atom recoils when the photon is emitted, and so there is not one rest-frame but two—the rest-frame of S′ and the rest-frame of S. It is true that the recoil is small and consequently the two rest-frames are nearly the same. But in spectroscopy wavelengths are sometimes given with 8-figure accuracy, and it is interesting to inquire whether such (or higher) accuracy is consistent with neglect of the small difference between the two rest-frames.
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References
Messiah, A., Quantum Mechanics, 23, 1041 (North–Holl, and Publishing Company, Amsterdam, 1965).
Landau, L., and Lifshitz, E., The Classical Theory of Fields, 32 (Addison-Wesley Press Inc., Cambridge, Massachusetts, 1951).
Feynman, R. P., and Hibbs, A. R., Quantum Mechanics and Path Integrals, 256 (McGraw-Hill Book Co., New York, 1965).
Handbuch der Physik, Atoms I, 35, 282 (Springer-Verlag, Berlin, 1957).
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SYNGE, J. Energy Levels and Lorentz Invariance. Nature 228, 271–272 (1970). https://doi.org/10.1038/228271a0
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DOI: https://doi.org/10.1038/228271a0
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