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EGAS41 - Swansea University

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41 st EGAS CP 121 Gdańsk 2009<br />

Quasiclassical calculations of BBR-induced depopulation rates<br />

and effective lifetimes of alkali-metal Rydberg atoms<br />

I.I. Beterov ∗ , I.I. Ryabtsev, D.B. Tretyakov, V.M. Entin, N.N. Bezuglov<br />

Institute of Semiconductor Physics SB RAS, Novosibirsk, Russia<br />

∗ Corresponding author: beterov@isp.nsc.ru<br />

Rates of depopulation by blackbody radiation (BBR) and effective lifetimes of all alkalimetal<br />

nS, nP and nD Rydberg states have been numerically calculated for n = 10 −<br />

80 at the ambient temperatures of 77, 300 and 600 K [1]. Quasiclassical formulas of<br />

Dyachkov and Pankratov [2] were used to calculate the radial matrix elements of the<br />

dipole transitions from Rydberg states. The advantage of the used quasiclassical model is<br />

its relative simplicity that nevertheless provides a good agreement with more sophisticated<br />

quantum-mechanical calculations.<br />

We have also obtained a simple formula for estimates of BBR-induced depopulation<br />

rates that is valid for both low and high values of n (in atomic units):<br />

Γ BBR =<br />

4<br />

3n 5 eff c3 1<br />

exp [ 1/(n 3 eff T)] − 1<br />

(1)<br />

Here n eff is the effective quantum number and c is the speed of light. For practical use<br />

a modified Eq. (1) can be written in units of [s −1 ] for temperature taken in Kelvins:<br />

Γ BBR = A<br />

n D eff<br />

2.14 × 10 10<br />

exp [ 315780 × B/(n C eff T)] − 1<br />

[<br />

s<br />

−1 ] . (2)<br />

The scaling coefficients A, B, C and D, obtained for all alkali-metal atoms [1], were<br />

introduced for better approximation of the numerical results. For high n ∼ 80 the error<br />

of the approximation is less than 8%, while for n ∼ 50 it is as low as 3.5%. Good agreement<br />

was observed with the recent experimental results [3] for Rb nS and nD states, while for<br />

nP states the theoretical curve goes below the experimental points. This points towards<br />

the need of new measurements in an extended n range.<br />

Acknowledgment<br />

This work was supported by the Russian Academy of Science and Russian Foundation for Basic<br />

Research.<br />

References<br />

[1] I.I. Beterov, I.I. Ryabtsev, D.B. Tretyakov, V.M. Entin,<br />

http://arxiv.org/abs/0810.0339<br />

[2] L.G. Dyachkov, P.M. Pankratov, J. Phys. B: At. Mol. Opt. Phys. 27, 461 (1994)<br />

[3] V.A. Nascimento, L.L. Caliri, A.L. de Oliveira, V.S. Bagnato and L.G. Marcassa,<br />

Phys. Rev. A 74, 054501 (2006)<br />

181

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