arXiv:physics/0412073 · Physical Review A

Lifetime measurement of the 8s level in francium

E. Gómez, Luis A. Orozco, A. Pérez Galván, Gene D. Sprouse

Published Jun 22, 2005• 18 citations

Abstract

We measure the lifetime of the $8s$ level of $^{210}\mathrm{Fr}$ atoms on a magneto-optically trapped sample with time-correlated single-photon counting. The $7{P}_{1∕2}$ state serves as the resonant intermediate level for two-step excitation of the $8s$ level completed with a $1.3\text{\ensuremath{-}}\ensuremath{\mu}\mathrm{m}$ laser. Analysis of the fluorescence decay through the $7{P}_{3∕2}$ level gives $53.30\ifmmode\pm\else\textpm\fi{}0.44\phantom{\rule{0.3em}{0ex}}\mathrm{ns}$ for the $8s$ level lifetime.

DOI: 10.1103/physreva.71.062504

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Lifetimes of the 9s and 8p levels of atomic francium

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Lifetime measurement of the 9s level of atomic francium

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arXiv:physics/0412073 · Physical Review A

Lifetime measurement of the 8s level in francium

E. Gómez, Luis A. Orozco, A. Pérez Galván, Gene D. Sprouse

Published Jun 22, 2005• 18 citations

arXiv HTML PDF

Abstract

We measure the lifetime of the

8s

level of

^{210}\mathrm{Fr}

atoms on a magneto-optically trapped sample with time-correlated single-photon counting. The

7{P}_{1∕2}

state serves as the resonant intermediate level for two-step excitation of the

8s

level completed with a

1.3\text{\ensuremath{-}}\ensuremath{\mu}\mathrm{m}

laser. Analysis of the fluorescence decay through the

7{P}_{3∕2}

level gives

53.30\ifmmode\pm\else\textpm\fi{}0.44\phantom{\rule{0.3em}{0ex}}\mathrm{ns}

for the

8s

level lifetime.

DOI: 10.1103/physreva.71.062504

Related papers

Lifetimes of the 9s and 8p levels of atomic francium

S. Aubin, E. Gómez, Luis A. Orozco +1 more

We use time-correlated single-photon counting techniques on a sample of $^{210}\mathrm{Fr}$ atoms confined and cooled in a magneto-optical trap to measure the lifetimes of the $9{S}_{1∕2},\phantom{\rule{0.3em}{0ex}}8{P}_{3∕2}$ , and $8{P}_{1∕2}$ excited levels. We populate the $9{S}_{1∕2}$ level by two-photon resonant excitation through the $7{P}_{1∕2}$ level. The direct measurement of the $9{S}_{1∕2}$ decay through the $7{P}_{3∕2}$ level at 851 nm gives a lifetime of $107.53\ifmmode\pm\else\textpm\fi{}0.90\phantom{\rule{0.3em}{0ex}}\mathrm{ns}$. We observe the decay of the $9{S}_{1∕2}$ level through the $8{P}_{3∕2}$ level at 423 nm and the $8{P}_{1∕2}$ level at 433 nm down to the $7{S}_{1∕2}$ ground level, and indirectly determine the lifetimes of these to be $83.5\ifmmode\pm\else\textpm\fi{}1.5\phantom{\rule{0.3em}{0ex}}\mathrm{ns}$ and $149.3\ifmmode\pm\else\textpm\fi{}3.5\phantom{\rule{0.3em}{0ex}}\mathrm{ns}$, respectively.We use time-correlated single-photon counting techniques on a sample of $^{210}\mathrm{Fr}$ atoms confined and cooled in a magneto-optical trap to measure the lifetimes of the $9{S}_{1∕2},\phantom{\rule{0.3em}{0ex}}8{P}_{3∕2}$, and $8{P}_{1∕2}$ excited levels. We populate the $9{S}_{1∕2}$ level by two-photon resonant excitation through the $7{P}_{1∕2}$ level. The direct measurement of the $9{S}_{1∕2}$ decay through the $7{P}_{3∕2}$ level at 851 nm gives a lifetime of $107.53\ifmmode\pm\else\textpm\fi{}0.90\phantom{\rule{0.3em}{0ex}}\mathrm{ns}$. We observe the decay of the $9{S}_{1∕2}$ level through the $8{P}_{3∕2}$ level at 423 nm and the $8{P}_{1∕2}$ level at 433 nm down to the $7{S}_{1∕2}$ ground level, and indirectly determine the lifetimes of these to be $83.5\ifmmode\pm\else\textpm\fi{}1.5\phantom{\rule{0.3em}{0ex}}\mathrm{ns}$ and $149.3\ifmmode\pm\else\textpm\fi{}3.5\phantom{\rule{0.3em}{0ex}}\mathrm{ns}$, respectively.

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Lifetime measurements of the 7D levels of atomic francium

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Lifetime measurement of the 9s level of atomic francium

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Lifetime measurement of the 6s level of rubidium

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Physical Review AApr 1, 199895 citations

Measurement of the 7p2P3/2 Level Lifetime in Atomic Francium

W. Z. Zhao, J. E. Simsarian, Luis A. Orozco +2 more

We present the first measurement of an atomic radiative lifetime in Fr. We use a time-correlated single photon counting technique with a cold sample of ${}^{210}\mathrm{Fr}$ atoms in a magneto-optic trap. The results are a precision experimental test of the atomic many-body perturbation theory applied to the heaviest alkali. The lifetime for the $7p{}^{2}{P}_{3/2}$ level of $21.02(16)$ ns gives a value for the reduced transition matrix element between the levels $7s{}^{2}{S}_{1/2}\ensuremath{\rightarrow}7p{}^{2}{P}_{3/2}$ of $5.898(22){a}_{\ensuremath{\infty}}$ atomic units.We present the first measurement of an atomic radiative lifetime in Fr. We use a time-correlated single photon counting technique with a cold sample of ${}^{210}\mathrm{Fr}$ atoms in a magneto-optic trap. The results are a precision experimental test of the atomic many-body perturbation theory applied to the heaviest alkali. The lifetime for the $7p{}^{2}{P}_{3/2}$ level of $21.02(16)$ ns gives a value for the reduced transition matrix element between the levels $7s{}^{2}{S}_{1/2}\ensuremath{\rightarrow}7p{}^{2}{P}_{3/2}$ of $5.898(22){a}_{\ensuremath{\infty}}$ atomic units.

Physical Review LettersJun 2, 199732 citations

We measure the lifetime of the

8s

level of

^{210}\mathrm{Fr}

atoms on a magneto-optically trapped sample with time-correlated single-photon counting. The

7{P}_{1∕2}

state serves as the resonant intermediate level for two-step excitation of the

8s

level completed with a

1.3\text{\ensuremath{-}}\ensuremath{\mu}\mathrm{m}

laser. Analysis of the fluorescence decay through the

7{P}_{3∕2}

level gives

53.30\ifmmode\pm\else\textpm\fi{}0.44\phantom{\rule{0.3em}{0ex}}\mathrm{ns}

for the

8s

level lifetime.

We use time-correlated single-photon counting techniques on a sample of

^{210}\mathrm{Fr}

atoms confined and cooled in a magneto-optical trap to measure the lifetimes of the

9{S}_{1∕2},\phantom{\rule{0.3em}{0ex}}8{P}_{3∕2}

, and

8{P}_{1∕2}

excited levels. We populate the

9{S}_{1∕2}

level by two-photon resonant excitation through the

7{P}_{1∕2}

level. The direct measurement of the

9{S}_{1∕2}

decay through the

7{P}_{3∕2}

level at 851 nm gives a lifetime of $107.53\ifmmode\pm\else\textpm\fi{}0.90\phantom{\rule{0.3em}{0ex}}\mathrm{ns}$. We observe the decay of the

9{S}_{1∕2}

level through the

8{P}_{3∕2}

level at 423 nm and the

8{P}_{1∕2}

level at 433 nm down to the

7{S}_{1∕2}

ground level, and indirectly determine the lifetimes of these to be $83.5\ifmmode\pm\else\textpm\fi{}1.5\phantom{\rule{0.3em}{0ex}}\mathrm{ns}$ and $149.3\ifmmode\pm\else\textpm\fi{}3.5\phantom{\rule{0.3em}{0ex}}\mathrm{ns}$, respectively.

We present lifetime measurements of the

{7D}_{3/2}

and

{7D}_{5/2}

levels of Fr. We use a time-correlated single-photon counting technique on a sample of

{}^{210}\mathrm{Fr}

atoms confined and cooled in a magneto-optical trap. The upper state of the

{7P}_{3/2}

trapping transition serves as the resonant intermediate level for two-photon excitation of the

7D

states. A probe laser provides the second step of the excitation, and we detect the decay of the atomic fluorescence. Our measurements help extend the knowledge of this class of atomic wave functions in which correlation effects are very significant. We measure lifetimes of $73.6\ifmmode\pm\else\textpm\fi{}0.3 \mathrm{ns}$ and $67.7\ifmmode\pm\else\textpm\fi{}2.9 \mathrm{ns}$ for the

{7D}_{3/2}

and

{7D}_{5/2}

levels, respectively.

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 $45.57\ifmmode\pm\else\textpm\fi{}0.17\phantom{\rule{0.3em}{0ex}}\mathrm{ns}$.

We present lifetime measurements of the

{7p}^{2}{P}_{3/2}

and

{7p}^{2}{P}_{1/2}

levels of Fr. We use a time-correlated single-photon counting technique on a cold sample of

{}^{210}\mathrm{Fr}

atoms in a magneto-optic trap. We excite the atoms with the trapping and repumping beams of the magneto-optic trap and detect the decay of the atomic fluorescence. The results are a precision experimental test of the atomic many-body perturbation theory applied to the heaviest alkali metal. The lifetime results are 21.02(11) ns and 29.45(11) ns for the

{7p}^{2}{P}_{3/2}

and

{7p}^{2}{P}_{1/2}

levels, respectively. This gives a line strength ratio

{\mathcal{S}}_{1/2}

{\mathcal{S}}_{3/2}

of 0.526(3) for these levels in Fr. To study sources of systematic errors we measure the lifetimes of

{5p}^{2}{P}_{3/2}

and

{5p}^{2}{P}_{1/2}

in stable

{}^{87}\mathrm{Rb}

and obtain 26.20(9) ns and 27.64(4) ns, respectively.

We present the first measurement of an atomic radiative lifetime in Fr. We use a time-correlated single photon counting technique with a cold sample of

{}^{210}\mathrm{Fr}

atoms in a magneto-optic trap. The results are a precision experimental test of the atomic many-body perturbation theory applied to the heaviest alkali. The lifetime for the

7p{}^{2}{P}_{3/2}

level of

21.02(16)

ns gives a value for the reduced transition matrix element between the levels $7s{}^{2}{S}_{1/2}\ensuremath{\rightarrow}7p{}^{2}{P}_{3/2}$ of $5.898(22){a}_{\ensuremath{\infty}}$ atomic units.