Abstract
The radiative properties of atomic systems are, in general, much more complicated than those discussed in the previous chapter, in which we considered optical spectra of single multilevel atoms separated by large distances. The complication arises from the fact that in practice atomic separations are small, even in low density atomic beams, and can be of the order of a resonant wavelength.
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Notes
- 1.
It should be kept in mind that there is no radiation in the direction parallel to the transition dipole moments of the atoms because \(\Phi (\bar{\varvec{r}})=0\) for \(\varvec{r}\parallel \varvec{\upmu }\).
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Ficek, Z., Tanaś, R. (2017). Collective Multiatom Spectroscopy. In: Quantum-Limit Spectroscopy. Springer Series in Optical Sciences, vol 200. Springer, New York, NY. https://doi.org/10.1007/978-1-4939-3740-0_4
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