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Bulletin of the American Physical Society

Fine Structure Excitation Transfer in Rb-Buffer Gas Mixtures

Jeremiah Wells, Alina Gearba, Randy Knize, Jerry Sell

Published Oct 21, 2016• 0 citations
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Enhancement of Rb 5P fine-structure collisional transfer rates in dense inert buffer gas mixtures

Alina Gearba, Jeremiah Wells, Randy Knize +1 more

Bulletin of the American Physical Society•Jun 8, 2017•0 citations

Collisional excitation transfer and quenching in Rb(5P) -methane mixtures

M. A. Gearba, Jeremiah Wells, Philip H. Rich +5 more

We have examined fine-structure mixing between the rubidium $5\phantom{\rule{0.16em}{0ex}}^{2}P_{3/2}$ and $5\phantom{\rule{0.16em}{0ex}}^{2}P_{1/2}$ states along with quenching of these states due to collisions with methane gas. Measurements are carried out using ultrafast laser-pulse excitation to populate one of the Rb $5{\phantom{\rule{0.16em}{0ex}}}^{2}P$ states, with the fluorescence produced through collisional excitation transfer observed using time-correlated single-photon counting. Fine-structure mixing rates and quenching rates are determined by the time dependence of this fluorescence. As $\mathrm{Rb}(5\phantom{\rule{0.16em}{0ex}}^{2}P$) collisional excitation transfer is relatively fast in methane gas, measurements were performed at methane pressures of $2.5--25$ Torr, resulting in a collisional transfer cross section ($5\phantom{\rule{0.16em}{0ex}}^{2}P_{3/2}\ensuremath{\rightarrow}5\phantom{\rule{0.16em}{0ex}}^{2}P_{1/2}$) of $(4.23\ifmmode\pm\else\textpm\fi{}0.13)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}15}\phantom{\rule{4pt}{0ex}}{\mathrm{cm}}^{2}$. Quenching rates were found to be much slower and were performed over methane pressures of $50--4000$ Torr, resulting in a quenching cross section of $(7.52\ifmmode\pm\else\textpm\fi{}0.10)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}19}\phantom{\rule{4pt}{0ex}}{\mathrm{cm}}^{2}$. These results represent a significant increase in precision compared to previous work, and also resolve a discrepancy in previous quenching measurements.

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M. A. Gearba, J. F. Sell, Brian M. Patterson +3 more

Employing ultrafast laser excitation and time-correlated single-photon counting, we have measured the fine-structure transfer between Rb 5P states induced by collisions with 4He buffer gas at temperatures up to 150 °C. The temperature dependence of the binary cross section agrees with earlier measurements. Our data show that the temperature dependence of the three-body rate is about the same as that of the binary rate. The three-body rate can be described as arising from the reduction of the rubidium fine-structure splitting due to nearby helium atoms.

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Three—body collisions involving Na(3P),Rb(5S) and buffer gas atoms

沈异凡, 李万兴

Energy pooling in the Na-Rb vapor mixture has been investigated.While some kind of buffer gas is introduced into the cell the peculiar features appear.The buffer gas enhances the energy transfer betwwen Na(3P) and Rb(5S),which can be detected through the effects induced on the highly excited states populated by the Na(3P)/Rb(5P) and Rb(5P)/Rb(5P) collisions.

Nuclear Science and Techniques•Jan 1, 1996•0 citations
We have examined fine-structure mixing between the rubidium 52P3/25\phantom{\rule{0.16em}{0ex}}^{2}P_{3/2}52P3/2​ and 52P1/25\phantom{\rule{0.16em}{0ex}}^{2}P_{1/2}52P1/2​ states along with quenching of these states due to collisions with methane gas. Measurements are carried out using ultrafast laser-pulse excitation to populate one of the Rb 52P5{\phantom{\rule{0.16em}{0ex}}}^{2}P52P states, with the fluorescence produced through collisional excitation transfer observed using time-correlated single-photon counting. Fine-structure mixing rates and quenching rates are determined by the time dependence of this fluorescence. As Rb(52P\mathrm{Rb}(5\phantom{\rule{0.16em}{0ex}}^{2}PRb(52P) collisional excitation transfer is relatively fast in methane gas, measurements were performed at methane pressures of 2.5−−252.5--252.5−−25 Torr, resulting in a collisional transfer cross section ($5\phantom{\rule{0.16em}{0ex}}^{2}P_{3/2}\ensuremath{\rightarrow}5\phantom{\rule{0.16em}{0ex}}^{2}P_{1/2}$) of $(4.23\ifmmode\pm\else\textpm\fi{}0.13)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}15}\phantom{\rule{4pt}{0ex}}{\mathrm{cm}}^{2}$. Quenching rates were found to be much slower and were performed over methane pressures of 50−−400050--400050−−4000 Torr, resulting in a quenching cross section of $(7.52\ifmmode\pm\else\textpm\fi{}0.10)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}19}\phantom{\rule{4pt}{0ex}}{\mathrm{cm}}^{2}$. These results represent a significant increase in precision compared to previous work, and also resolve a discrepancy in previous quenching measurements.
Employing ultrafast laser excitation and time-correlated single-photon counting, we have measured the fine-structure transfer between Rb 5P states induced by collisions with 4He buffer gas at temperatures up to 150 °C. The temperature dependence of the binary cross section agrees with earlier measurements. Our data show that the temperature dependence of the three-body rate is about the same as that of the binary rate. The three-body rate can be described as arising from the reduction of the rubidium fine-structure splitting due to nearby helium atoms.