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Acta Physica Sinica

POLARIZABILITIES OF HIGH RYDBERG ALKALI ATOMS

HE XING-HONG, Baiwen Li, ZHANG CHENG-XIU, 中国科学院武汉物理研究所波谱与原子分子物理开放研究实验室

Published Jan 1, 1989• 14 citations
Publisher

Abstract

A potential model for atoms is employed to calculate the scalar and tensor polarizabilities of Rydberg states (15≤n≤55) of Na, K, Rb and Cs. The results are very close to the experimental values. The scaling relations of the polarizabilities a = An*7 + Bn*6 are also established, and the results obtained from them also agree with experimental data satisfatorily.

DOI
10.7498/aps.38.1717

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A potential model for atoms is employed to calculate the scalar and tensor polarizabilities of Rydberg states (15≤n≤55) of Na, K, Rb and Cs. The results are very close to the experimental values. The scaling relations of the polarizabilities a = An7 + Bn6 are also established, and the results obtained from them also agree with experimental data satisfatorily.
Up to the present, although experimental studies about the polarizabilities of alkali-metal Rydberg atoms have involved the states with principal quantum numbers $n\ensuremath{\le}80$, theoretical calculations are limited to the states with $n\ensuremath{\le}50$. In this work, we calculate the scalar and tensor polarizabilities of the nS1/2n{S}_{1/2}nS1/2​, nP1/2,3/2n{P}_{1/2,3/2}nP1/2,3/2​, and nD3/2,5/2n{D}_{3/2,5/2}nD3/2,5/2​ Rydberg states of Rb with principal quantum number nnn up to 140 employing a model potential and the BBB-spline expansion technique. We obtain the polarizabilities that are in good agreement with the existing theoretical and experimental data.
Calculations of the static electric-dipole scalar and tensor polarizabilities are presented for two alkali-metal atoms, Rb and Cs, for the $nS, n{P}_{\textonehalf{},\phantom{\rule{0.16em}{0ex}}3/2}$, and nD3/2,5/2n{D}_{3/2,\phantom{\rule{0.16em}{0ex}}5/2}nD3/2,5/2​ states with large principal quantum numbers up to n=50n=50n=50. The calculations are performed within an effective one-electron approximation, based on the Dirac-Fock Hamiltonian with a semiempirical core-polarization potential. The obtained results are compared with those from a simpler semiempirical approach and with available experimental data.
A comprehensive set of transition probabilities and radiative lifetimes of Rydberg states of alkali atoms (for Na, K, Cs, n<or=30; and for Rb, n<or=50) is obtained by using a simple, exactly solvable potential model for atoms. The results agree well with the available experimental values and other theoretical ones. Scaling relations for evaluating transition probabilities and lifetimes of high Rydberg states are also discussed. The well known (n*) -5 scaling law of the transition probabilities A n(inf) not=n(inf) / with n' approximately=n>>1 is generally valid; however, the authors also find deviations from this law for some d to p and f to d transitions for Rb. A third-power polynomial is found to be better than the currently used exponential scaling law in predicting the lifetimes of even higher excited states.
We have calculated the long-range interaction potential curves of highly excited Rydberg atom pairs for the combinations Li–Li, Na–Na, K–K, Rb–Rb and Cs–Cs in a perturbative approach. The dispersion C -coefficients are determined for all symmetries of molecular states that correlate to the n s– n s, n p– n p and n d– n d asymptotes. Fitted parameters are given for the scaling of the C -coefficients as a function of the principal quantum number n for all homonuclear pairs of alkali metal atoms.
The scalar and tensor dynamic polarizabilities of the first excited 2P1∕2,3∕2^{2}P_{1∕2,3∕2}2P1∕2,3∕2​ states of the alkali-metal atoms Na\mathrm{Na}Na, K\mathrm{K}K, and Rb\mathrm{Rb}Rb are calculated using relativistic many-body perturbation theory. Comparison with experimental measurements of the static polarizabilities suggests that the errors in the theoretical predictions do not exceed 1%. The dynamic polarizabilities at imaginary frequencies are employed to calculate the long-range van der Waals coefficients for the interaction of ground-state helium atoms with the excited alkali-metal atoms to a probable error of less than 2%.
We report a comprehensive set of calculations of the lifetimes of Rydberg states in alkali-metal atoms, using realistic potentials to represent the atomic core. The effects due to core polarizability, spin-orbit interaction, and blackbody radiation are explicitly included. A complete cross reference listing of all available experimental lifetimes is also attempted. The results compare well with experiment for all principal quantum numbers nnn examined and should provide guidance for future experimental investigations. The relation of the present approach to other works is discussed.