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Canadian Journal of Physics

The Lifetimes of the 72P1/2 and 72P3/2 States of Cesium

Paul W. Pace, J. B. Atkinson

Published May 15, 1975• 17 citations
Publisher

Abstract

The lifetimes of the 72P3/2 and 72P1/2 states of atomic cesium have been determined using delayed coincidence techniques. A nitrogen laser pumped tunable dye laser was used to excite the cesium vapor and direct measurements of the fluorescence decay yielded the following lifetimes: τ3/2(72P3/2) = 136 ± 4 ns and τ1/2(72P1/2) = 158 ± 5 ns. These values are in good agreement with recent measurements and calculations.

DOI
10.1139/p75-117

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The lifetimes of the 72P3/2 and 72P1/2 states of atomic cesium have been determined using delayed coincidence techniques. A nitrogen laser pumped tunable dye laser was used to excite the cesium vapor and direct measurements of the fluorescence decay yielded the following lifetimes: τ3/2(72P3/2) = 136 ± 4 ns and τ1/2(72P1/2) = 158 ± 5 ns. These values are in good agreement with recent measurements and calculations.
We measure the lifetime of the cesium 52D5/25^{2}D_{5/2}52D5/2​ state using a time-resolved single-photon-counting method. We excite atoms in a hot vapor cell via an electric quadrupole transition at a wavelength of 685 nm and record the fluorescence of a cascade decay at a wavelength of 852 nm. We extract a lifetime of 1353(5)1353(5)1353(5) ns for the 52D5/25{\phantom{\rule{0.16em}{0ex}}}^{2}{D}_{5/2}52D5/2​ state, in agreement with a recent theoretical prediction. In particular, the observed lifetime is consistent with the literature values of the polarizabilities of the cesium 6P6P6P states. Our measurement contributes to resolving a long-standing disagreement between a number of experimental and theoretical results.
The method of sensitized fluorescence has been employed to investigate the [Formula: see text] excitation transfer processes in cesium induced in collisions with ground state cesium atoms. The cesium vapor density was kept sufficiently low to enable the cross sections for the mixing process to be determined under single collision conditions and to ensure that radiation trapping and quenching were negligible. A nitrogen laser pumped dye laser was used to excite the cesium atoms to each of the 72P levels in turn and measurements of the relative intensities of fluorescence yielded the following cross sections: [Formula: see text] These results are consistent with the empirical relationship between the magnitude of the cross sections and the fine structure splitting that has previously been determined for the alkalis.
We report measurements of the 5d2D5/2,5d{}^{2}{D}_{5/2},5d2D5/2​, 5d2D3/2,5d{}^{2}{D}_{3/2},5d2D3/2​, and 11s2S1/211s{}^{2}{S}_{1/2}11s2S1/2​ state lifetimes in the 133{}^{133}133Cs atom to be 1281(9), 909(15), and 351(4) ns, respectively. A pulsed-dye laser selectively excites atomic Cs from the ground state, via a single-photon quadrupole transition, to the 5d5d5d states and, via a two-photon electric dipole transition, to the 11s11s11s state. A spectrometer-photomultiplier system detects the fluorescence from the decay of interest and a digitizing oscilloscope records the direct output of the photomultiplier. The data are fit to an exponential function to yield a value for the mean lifetime of the selected state.
The lifetimes of the 7 2{\mathrm{}}^{2}2P1/2o{P}_{1/2}^{o}P1/2o​ and 7 2{\mathrm{}}^{2}2P3/2o{P}_{3/2}^{o}P3/2o​ states of thallium have been measured for the first time by observing the fluorescence decay following two-photon resonant excitation in an atomic beam. The values obtained for these states are 61.9 and 48.4 ns, respectively, with an uncertainty of 2%. These results are in good quantitative agreement with the calculations of Bardsley and Norcross, which include the effect of core polarizability.