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arXiv:0906.0586 · Physical Review A

Measurement of the lifetime of the 6p P21/2o level of Yb+

Steven Olmschenk, David Hayes, Dzmitry Matsukevich, Peter Maunz, David L. Moehring, Kelly Cooper Younge, Christopher R. Monroe

Published Aug 10, 2009• 57 citations
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Abstract

We present a precise measurement of the lifetime of the $6p\text{ }{^{2}P}_{1/2}^{o}$ excited state of a single trapped ytterbium ion $({\text{Yb}}^{+})$. A time-correlated single-photon counting technique is used, where ultrafast pulses excite the ion and the emitted photons are coupled into a single-mode optical fiber. By performing the measurement on a single atom with fast excitation and excellent spatial filtering, we are able to eliminate common systematics. The lifetime of the $6p\text{ }{^{2}P}_{1/2}^{o}$ state is measured to be $8.12\ifmmode\pm\else\textpm\fi{}0.02\text{ }\text{ns}$, in good agreement with previous experimental measurements and some theoretical values.

DOI
10.1103/physreva.80.022502

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We present a precise measurement of the lifetime of the 6p 2P1/2o6p\text{ }{^{2}P}_{1/2}^{o}6p 2P1/2o​ excited state of a single trapped ytterbium ion (Yb+)({\text{Yb}}^{+})(Yb+). A time-correlated single-photon counting technique is used, where ultrafast pulses excite the ion and the emitted photons are coupled into a single-mode optical fiber. By performing the measurement on a single atom with fast excitation and excellent spatial filtering, we are able to eliminate common systematics. The lifetime of the 6p 2P1/2o6p\text{ }{^{2}P}_{1/2}^{o}6p 2P1/2o​ state is measured to be 8.12\ifmmode±\else\textpm\fi0.02 ns8.12\ifmmode\pm\else\textpm\fi{}0.02\text{ }\text{ns}8.12\ifmmode±\else\textpm\fi0.02 ns, in good agreement with previous experimental measurements and some theoretical values.
We present a method to precisely determine the 2D3/2^{2}D_{3/2}2D3/2​ state lifetime of a single trapped 174Yb+^{174}\mathrm{Yb}^{+}174Yb+ ion. This method is based on the detection of photons emitted from excited states, where a highly synchronized measurement sequence for laser control and an intensity-alternating sequence for atomic excitation and photon counting are used to minimize systematic errors. This method is easy to implement and is immune to fluctuations of magnetic field, laser intensity, and frequency detuning. Combined with the real-time approach of background photon correction, the radiative lifetime of the 2D3/2^{2}D_{3/2}2D3/2​ state is determined to be $54.83\ifmmode\pm\else\textpm\fi{}0.18$ ms, which represents an order of magnitude improvement in measurement precision. The accurately determined lifetime sets a benchmark for many-body atomic theories and is particularly useful to determine the coherence time limit of the optical clock.
The ytterbium ion has a rich level structure of low-lying states, and is one of the most widely used in experiments with trapped ions. We have measured the radiative lifetimes for the two 4f145d{4f}^{14}5d4f145d metastable states using single ytterbium ions confined in a rf trap. The obtained lifetimes for D3/2{D}_{3/2}D3/2​ and D5/2{D}_{5/2}D5/2​ states are 52.7(2.4) and 7.0(0.4) ms, respectively. The results are in good agreement with previously measured values, but differ significantly from theoretical estimates. The P1/2{P}_{1/2}P1/2​ branching ratio into D3/2{D}_{3/2}D3/2​ has also been obtained from the experiment to be 0.0483 with a 9% uncertainty.
We present lifetime measurements of the 7p2P3/2{7p}^{2}{P}_{3/2}7p2P3/2​ and 7p2P1/2{7p}^{2}{P}_{1/2}7p2P1/2​ levels of Fr. We use a time-correlated single-photon counting technique on a cold sample of 210Fr{}^{210}\mathrm{Fr}210Fr 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 7p2P3/2{7p}^{2}{P}_{3/2}7p2P3/2​ and 7p2P1/2{7p}^{2}{P}_{1/2}7p2P1/2​ levels, respectively. This gives a line strength ratio S1/2{\mathcal{S}}_{1/2}S1/2​/S3/2{\mathcal{S}}_{3/2}S3/2​ of 0.526(3) for these levels in Fr. To study sources of systematic errors we measure the lifetimes of 5p2P3/2{5p}^{2}{P}_{3/2}5p2P3/2​ and 5p2P1/2{5p}^{2}{P}_{1/2}5p2P1/2​ in stable 87Rb{}^{87}\mathrm{Rb}87Rb and obtain 26.20(9) ns and 27.64(4) ns, respectively.
We present a lifetime measurement of the 6s6s6s 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 5P1∕25{P}_{1∕2}5P1∕2​ level serves as the resonant intermediate step for the two-step excitation to the 6s6s6s level. We detect the decay of the 6s6s6s level through the cascade fluorescence of the 5P3∕25{P}_{3∕2}5P3∕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 the first measurement of an atomic radiative lifetime in Fr. We use a time-correlated single photon counting technique with a cold sample of 210Fr{}^{210}\mathrm{Fr}210Fr 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 7p2P3/27p{}^{2}{P}_{3/2}7p2P3/2​ level of 21.02(16)21.02(16)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.