arXiv:physics/0612235

Rubidium lifetime in a dark magneto-optical trap

O. I. Permyakova, A. V. Yakovlev, P. L. Chapovsky

Published Dec 24, 2006• 1 citation

Abstract

Measurements of rubidium lifetime in a dark magneto-optical trap (DMOT) was performed at various populations of the bright and dark hyperfine states of the trapped atoms. The rubidium lifetime in the trap appeared to be shorter if the atom spent more time in the bright state. A simple explanation of this effect is based on the increase of the cross-section of rubidium collisions with the surrounding warm atoms upon rubidium electronic excitation.

DOI: 10.48550/arxiv.physics/0612235

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arXiv:physics/0612235

Rubidium lifetime in a dark magneto-optical trap

O. I. Permyakova, A. V. Yakovlev, P. L. Chapovsky

Published Dec 24, 2006• 1 citation

arXiv HTML PDF

Abstract

DOI: 10.48550/arxiv.physics/0612235

Related papers

Measurement of the lifetime of rubidium atoms in a dark magneto-optical trap

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The lifetimes of rubidium atoms in a dark magneto-optical trap are measured at different populations of the 'bright' and 'dark' hyperfine states of captured atoms. It is found that the lifetime of atoms in the trap decreases if they spend more time in the bright state. A simple explanation of this effect is proposed which is based on the increase in the transport cross section for collisions of thermal rubidium atoms surrounding the trap with cold rubidium atoms upon their electronic excitation.The lifetimes of rubidium atoms in a dark magneto-optical trap are measured at different populations of the 'bright' and 'dark' hyperfine states of captured atoms. It is found that the lifetime of atoms in the trap decreases if they spend more time in the bright state. A simple explanation of this effect is proposed which is based on the increase in the transport cross section for collisions of thermal rubidium atoms surrounding the trap with cold rubidium atoms upon their electronic excitation.

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We measure the collision-rate coefficient between laser-cooled rubidium (Rb) atoms in a magneto-optical trap (MOT) and optically dark Rb

{}^{+}

ions in an overlapping Paul trap. In such a mixture, the ions are created from the MOT atoms and allowed to accumulate in the ion trap, which results in a significant reduction in the number of steady-state MOT atoms. A theoretical rate-equation model is developed to describe the evolution of the MOT atom number due to ionization and ion-atom collisions, and we derive an expression for the ion-atom collision-rate coefficient. The loss of MOT atoms is studied systematically by sequentially switching on the various mechanisms in the experiment. Combining the measurements with the model allows the direct determination of the ion-atom collision-rate coefficient. Finally, the scope of the experimental technique developed here is discussed.

We present lifetime measurements of the

5{D}_{3∕2}

and

5{D}_{5∕2}

states of rubidium using the time-correlated single-photon-counting method. We perform the experiment in a magneto-optical trap of

^{87}\mathrm{Rb}

atoms using a two-step excitation with the trap laser at

780\phantom{\rule{0.3em}{0ex}}\mathrm{nm}

as the first step. We record the

761.9\phantom{\rule{0.3em}{0ex}}\mathrm{nm}

fluorescence from the decay of the

5{D}_{3∕2}

state to the

5{P}_{1∕2}

state, and measure the lifetime of the

5{D}_{3∕2}

state $\ensuremath{\tau}=246.3(1.6)\phantom{\rule{0.3em}{0ex}}\mathrm{ns}$. We record the

420.2\phantom{\rule{0.3em}{0ex}}\mathrm{nm}

fluorescence from the cascade decay of the

5{D}_{5∕2}

state to the

5{S}_{1∕2}

state through the

6{P}_{3∕2}

state, and extract the lifetime of the

5{D}_{5∕2}

state $\ensuremath{\tau}=238.5(2.3)\phantom{\rule{0.3em}{0ex}}\mathrm{ns}$.

We present a lifetime measurement of the

6s

level of rubidium. We use a time-correlated single-photon counting technique on two different samples of rubidium atoms, a vapor cell with variable rubidium density, and a sample of atoms confined and cooled in a magneto-optical trap. The

5{P}_{1∕2}

level serves as the resonant intermediate step for the two-step excitation to the

6s

level. We detect the decay of the

6s

level through the cascade fluorescence of the

5{P}_{3∕2}

level at 780 nm. The two samples have different systematic effects, but we obtain consistent results that averaged give a lifetime of $45.57\ifmmode\pm\else\textpm\fi{}0.17\phantom{\rule{0.3em}{0ex}}\mathrm{ns}$.