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Abstract
Atomic phenomena are described mainly on the basis of non-relativistic quantum mechanics. Relativistic effects can generally be accounted for in a satisfactory way with perturbative methods. In the 1990s it became increasingly apparent, that a better understanding of the classical dynamics of an atomic system can lead to a deeper appreciation of various features in its observable quantum mechanical properties, see e.g. [RW94, CK97, FE97, BB97, SS98, BR09], Sect. 5.3.
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Notes
- 1.
It is also common usage to express φ c in terms of the spherical Bessel functions of the second kind , y l (z) = −n l (z): φ c(kr) = −kr y l (kr), cf. (A.51) in Appendix A.4.
- 2.
We use the term "momentum representation" when we write the wave functions as functions of momentum p or as functions of wave number k = p∕ħ.
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Friedrich, H. (2017). Review of Quantum Mechanics. In: Theoretical Atomic Physics. Graduate Texts in Physics. Springer, Cham. https://doi.org/10.1007/978-3-319-47769-5_1
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