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JOURNALS // Pis'ma v Zhurnal Èksperimental'noi i Teoreticheskoi Fiziki // Archive

Pis'ma v Zh. Èksper. Teoret. Fiz., 2016 Volume 103, Issue 1, Pages 62–66 (Mi jetpl4834)

This article is cited in 3 papers

MISCELLANEOUS

Rules of correspondence in atomic physics

A. M. Dyugaevab, E. V. Lebedevac

a Max-Planck-Institut für Physik Komplexer Systeme, D-01187, Dresden, Germany
b Landau Institute for Theoretical Physics, Russian Academy of Sciences, Chernogolovka, Moscow region, 142432, Russia
c Institute of Solid State Physics, Russian Academy of Sciences, Chernogolovka, Moscow region, 142432, Russia

Abstract: The Smirnov method of analytic continuation (B.M. Smirnov, Sov. Phys. JETP $\mathbf{20}$, 345 (1964)) has been justified and developed for atomic physics. It has been shown that the polarizability of alkali atoms $\alpha$, their van der Waals interaction constant $C_6$, and the oscillator strength of the transition to the first $P$ state $f_{01}$ are related to the parameter $\langle r^2\rangle$ and gap in the spectrum $\frac{3}{2}\frac{f}{\Delta}\approx \frac{3}{2}\alpha\Delta\approx (3C_6\Delta)^{1/2}\approx\langle r^2\rangle$. The average square of the coordinate of the valence electron $\langle r^2\rangle$ in the first approximation has a hydrogen dependence $J_1=\frac{1}{2\nu^2}$ on the filling factor $\nu$, which is defined in terms of the first ionization potential.

Received: 05.11.2015

DOI: 10.7868/S0370274X16010112


 English version:
Journal of Experimental and Theoretical Physics Letters, 2016, 103:1, 57–61

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