2007
DOI: 10.1103/physreva.75.052720
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Ionization of sodium and rubidiumnS,nP, andnDRydberg atoms by blackbody radiation

Abstract: Results of theoretical calculations of ionization rates of Rb and Na Rydberg atoms by blackbody radiation (BBR) are presented. Calculations have been performed for nS, nP and nD states of Na and Rb, which are commonly used in a variety of experiments, at principal quantum numbers n=8-65 and at three ambient temperatures of 77, 300 and 600 K. A peculiarity of our calculations is that we take into account the contributions of BBR-induced redistribution of population between Rydberg states prior to photoionizatio… Show more

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Cited by 43 publications
(65 citation statements)
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“…(II) Due to the Rydberg blockade, each Rydberg-excited atom blocks further excitations within a radius R c leading to density-density correlations which resemble those of a gas of hard-spheres. After a short time, the Rydberg density reaches steady state, however over time Rydberg atoms start to decay by a combination of blackbody photoionization [12] and ionizing collisions with atoms in the ground and intermediate states [23], which leads to a gradual increase in the number of charged particles in the system. (III) Once a critical number of ions N crit accumulates the resulting space charge can trap subsequently produced electrons.…”
Section: Fig 1 (Color Online)mentioning
confidence: 99%
“…(II) Due to the Rydberg blockade, each Rydberg-excited atom blocks further excitations within a radius R c leading to density-density correlations which resemble those of a gas of hard-spheres. After a short time, the Rydberg density reaches steady state, however over time Rydberg atoms start to decay by a combination of blackbody photoionization [12] and ionizing collisions with atoms in the ground and intermediate states [23], which leads to a gradual increase in the number of charged particles in the system. (III) Once a critical number of ions N crit accumulates the resulting space charge can trap subsequently produced electrons.…”
Section: Fig 1 (Color Online)mentioning
confidence: 99%
“…Nevertheless, in order to improve the precision of the numerical calculations of BBR-induced depopulation rates we took into account transitions to all lower states and to the upper states with n ′ < n + 40. Omission of higher discrete states and continuum states reduces the accuracy by less than 0.5% [26,27]. The range of validity of the commonly used theoretical model of interaction of Rydberg atoms with blackbody radiation was discussed by Farley and Wing [4].…”
Section: Bbr-induced Depopulation Of Rydberg Statesmentioning
confidence: 99%
“…However, because this growth is slow, other processes must be considered that might contribute to the growth in the number of visible ion cores after 1 D 2 excitations, such as population redistribution to states with attractive potentials by blackbody radiation (BBR) and BBR-induced photoionization. Calculations for hydrogen, helium, and the alkali metals [74][75][76] suggest that while the rates for excitation or deexcitation of Rydberg states by BBR depend on the particular atomic species, the rate for states with n ∼ 50 should be less than ∼1 × 10 4 /s. Whereas such rates might allow up to 10% of the parent 1 D 2 Rydberg states to undergo a transition to states of different on the time scale (∼10 μs) of the present measurements, this is insufficient to significantly increase the overall transition rate.…”
Section: Rydberg Gas Dynamics With Attractive and Repulsive Interamentioning
confidence: 99%