Radiative lifetimes of highly excited states in rubidium
2014 Measurements have been made of the natural radiative lifetimes of highly excited rubidium (9 ~ n ~ 18) S and D states. These results, as well as those already published concerning P and F states, agree well with the theoretical lifetimes calculated by the Bates-Damgaard method. J. Physique 41 (1980) 119-121 1 FTVRIER 1980, Classification Physics Abstracts 32.70 In the past few years, measurements of the radiative lifetimes of highly excited states of alkali atoms have been reported [1-3]. These results would clearly be of interest for physicists working in atomic physics, plasma physics, astrophysics. Moreover they allow interesting comparisons with theoretical calculations. We have already published measurements of the radiative lifetimes for some Rydberg P and F states in rubidium [4, 5]. In order to obtain a consistent set of lifetime values for a given alkali atom, we present here measurements concerning the nS and nD states of rubidium (9 n 18). Comparison is given between the obtained experimental values and the theoretical ones calculated by using a modified Bates-Damgaard Method [6, 7] (here after refered as B.D.). We use the classical method of time resolved laser induced fluorescence [4]. Rubidium atoms contained in a cell are excited in a given high-lying nS or nD state by stepwise pulsed excitation via the first resonant 5P state. For convenience the 5p3,2 state is chosen as the intermediate state for the excitation of the nS levels, the observation of the population decay being made on the nS -+ 5P 1/2 line. The nD states are produced by using light pulses whose wavelengths correspond either, to the 5PI/2 --+ nD3/2 transitions for n 13, or to the 5P3/2 -+ nD3/2,5/2 transitions for n &#x3E; 13; the population decay is observed on these same lines. Such a choice is determined by the fact that we are also interested in the study of some collisional properties of the nD states (results concerning the collisional properties of both the S and D levels will be published elsewhere [8]). Thus our reported lifetimes refer to the nD3/2 states for n 13 and to the nD states, without allowance for fine structure, for n &#x3E; 13. This is of no importance since the lifetimes corresponding to the two fine structure levels are expected to be very close, for a given n value. A high-speed photon counting system allows the determination of the decay of the excited.state population as a function of time for a given rubidium pressure. The extrapolation to zero rubidium pressure yields the natural radiative lifetime. The experimental set-up, shown in figure 1, has been already widely Fig. 1. Experimental set-up. Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphys:01980004102011900
Assessments of lifetimes and photoionization cross-sections at 10.6 μm of nd Rydberg states of Rb measured in a magneto-optical trap
Abstract By using IR laser photoionization in a magneto-optical trap, radiative lifetimes of rubidium Rydberg nd states (n = 16–20) have been measured. The measured lifetimes are: 4.63 μs for the 16d state, 5.39 μs (17d), 6.74 μs (18d), 8.06 μs (19d) and 8.99 μs (20d). The experimental values are in agreement with previous theoretical calculations. The reported method allows also for a measurement of the photoionization cross-sections of the specified Rydberg states at 10.6 μm. In this case the experimental values (ranging from 39 Mb for the 16d state to 30 Mb for the 20d state) look inconsistent with theoretical calculations.
Detection of the Rydberg states of rubidium using a frequency doubled CW dye laser
Abstract A sensitive method of detecting Rydberg atoms of Rb is described. The excitation source is a continuous-wave frequency doubled dye laser and detection is by a spacecharge limited thermionic triode. By applying a small electric field 2 S, 2 P and 2 D series can be excited directly from the ground state. Term value for the 2 S and 2 D series up to 54 2 S and 52 2 D have been measured using the 2 P states as references.