Bulletin of the American Physical Society

Two-Photon Polarization Spectroscopy of atomic Cs over the $6s^{2}S_{1/2}\rightarrow6p^{2}P_{3/2}\rightarrow9d^{2}D_{5/2}$ transition

M. J. Welsh, Seda Kin, Jacob D Hinkle, Servet Bayram

Published Apr 9, 2005• 0 citations

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Bulletin of the American Physical Society

Two-Photon Polarization Spectroscopy of atomic Cs over the $6s^{2}S_{1/2}\rightarrow6p^{2}P_{3/2}\rightarrow9d^{2}D_{5/2}$ transitionTwo-Photon Polarization Spectroscopy of atomic Cs over the $6s^{2}S_{1/2}\rightarrow6p^{2}P_{3/2}\rightarrow9d^{2}D_{5/2}$ transition

M. J. Welsh, Seda Kin, Jacob D Hinkle, Servet Bayram

Published Apr 9, 2005• 0 citations

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Polarization dependence of double-resonance optical pumping and electromagnetically induced transparency in the 5S1/2−5P3/2−5D5/2 transition of 87 Rb atoms

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The polarization dependence of double-resonance optical pumping (DROP) in the ladder-type electromagnetically induced transparency (EIT) of the $5{S}_{1/2}\ensuremath{-}5{P}_{3/2}\ensuremath{-}5{D}_{5/2}$ transition of ${}^{87}$ Rb atoms is studied. The transmittance spectra in the $5{S}_{1/2}(F=2)\ensuremath{-}5{P}_{3/2}({F}^{\ensuremath{'}}=3)\ensuremath{-}5{D}_{5/2}({F}^{\ensuremath{'}\ensuremath{'}}=2,3,4)$ transition were observed as caused by EIT, DROP, and saturation effects in the various polarization combinations between the probe and coupling lasers. The features of the double-structure transmittance spectra in the $5{S}_{1/2}(F=2)\ensuremath{-}5{P}_{3/2}({F}^{\ensuremath{'}}=3)\ensuremath{-}5{D}_{5/2}({F}^{\ensuremath{'}\ensuremath{'}}=4)$ cycling transition were attributed to the difference in saturation effect according to the transition routes between the Zeeman sublevels and the EIT according to the two-photon transition probability.The polarization dependence of double-resonance optical pumping (DROP) in the ladder-type electromagnetically induced transparency (EIT) of the $5{S}_{1/2}\ensuremath{-}5{P}_{3/2}\ensuremath{-}5{D}_{5/2}$ transition of ${}^{87}$Rb atoms is studied. The transmittance spectra in the $5{S}_{1/2}(F=2)\ensuremath{-}5{P}_{3/2}({F}^{\ensuremath{'}}=3)\ensuremath{-}5{D}_{5/2}({F}^{\ensuremath{'}\ensuremath{'}}=2,3,4)$ transition were observed as caused by EIT, DROP, and saturation effects in the various polarization combinations between the probe and coupling lasers. The features of the double-structure transmittance spectra in the $5{S}_{1/2}(F=2)\ensuremath{-}5{P}_{3/2}({F}^{\ensuremath{'}}=3)\ensuremath{-}5{D}_{5/2}({F}^{\ensuremath{'}\ensuremath{'}}=4)$ cycling transition were attributed to the difference in saturation effect according to the transition routes between the Zeeman sublevels and the EIT according to the two-photon transition probability.

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Collisional depolarization of Zeeman coherences in the Cs1336pP3∕22 level: Double-resonance two-photon polarization spectroscopy

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An experimental investigation of the Cs $6s\phantom{\rule{0.2em}{0ex}}^{2}S_{1∕2}\ensuremath{\rightarrow}6p\phantom{\rule{0.2em}{0ex}}^{2}P_{3∕2}\ensuremath{\rightarrow}10s\phantom{\rule{0.2em}{0ex}}^{2}S_{1∕2}$ double-resonance two-photon polarization spectrum has been made. In the investigation, a linear polarization degree was measured to extract the alignment depolarization cross section in the cesium $6p\phantom{\rule{0.2em}{0ex}}^{2}P_{3∕2}$ level due to collisions between ground-level argon and excited $6p\phantom{\rule{0.2em}{0ex}}^{2}P_{3∕2}$ cesium atoms over the Zeeman coherences. The spectra show strong depolarization of the Cs $6p\phantom{\rule{0.2em}{0ex}}^{2}P_{3∕2}$ level. The measured alignment depolarization cross section value of 186 $(58)\phantom{\rule{0.3em}{0ex}}{\mathrm{\AA{}}}^{2}$ is in good agreement with the experiment and theoretical predictions.An experimental investigation of the Cs $6s\phantom{\rule{0.2em}{0ex}}^{2}S_{1∕2}\ensuremath{\rightarrow}6p\phantom{\rule{0.2em}{0ex}}^{2}P_{3∕2}\ensuremath{\rightarrow}10s\phantom{\rule{0.2em}{0ex}}^{2}S_{1∕2}$ double-resonance two-photon polarization spectrum has been made. In the investigation, a linear polarization degree was measured to extract the alignment depolarization cross section in the cesium $6p\phantom{\rule{0.2em}{0ex}}^{2}P_{3∕2}$ level due to collisions between ground-level argon and excited $6p\phantom{\rule{0.2em}{0ex}}^{2}P_{3∕2}$ cesium atoms over the Zeeman coherences. The spectra show strong depolarization of the Cs $6p\phantom{\rule{0.2em}{0ex}}^{2}P_{3∕2}$ level. The measured alignment depolarization cross section value of 186 $(58)\phantom{\rule{0.3em}{0ex}}{\mathrm{\AA{}}}^{2}$ is in good agreement with the experiment and theoretical predictions.

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May 8, 19940 citations

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Ramiz Hamid, Mustafa Çetintaş, Mehmet Çelik

Optics CommunicationsSep 1, 200311 citations

Two-Photon Polarization Spectroscopy of atomic Cs over the

6s^{2}S_{1/2}\rightarrow6p^{2}P_{3/2}\rightarrow9d^{2}D_{5/2}

transition

Doppler-free two-photon spectroscopy of Cs

6S_{1/2}

7D_{3/2,\,5/2}

transition

Power dependence of multi-photon processes in the

5S_{1/2}-5P_{3/2}-5D_{5/2}

transition of

^{87}

Rb atoms

{}^{87}

Rb atoms is studied. The transmittance spectra in the $5{S}_{1/2}(F=2)\ensuremath{-}5{P}_{3/2}({F}^{\ensuremath{'}}=3)\ensuremath{-}5{D}_{5/2}({F}^{\ensuremath{'}\ensuremath{'}}=2,3,4)$ transition were observed as caused by EIT, DROP, and saturation effects in the various polarization combinations between the probe and coupling lasers. The features of the double-structure transmittance spectra in the $5{S}_{1/2}(F=2)\ensuremath{-}5{P}_{3/2}({F}^{\ensuremath{'}}=3)\ensuremath{-}5{D}_{5/2}({F}^{\ensuremath{'}\ensuremath{'}}=4)$ cycling transition were attributed to the difference in saturation effect according to the transition routes between the Zeeman sublevels and the EIT according to the two-photon transition probability.

6p\phantom{\rule{0.2em}{0ex}}^{2}P_{3∕2}

level due to collisions between ground-level argon and excited

6p\phantom{\rule{0.2em}{0ex}}^{2}P_{3∕2}

cesium atoms over the Zeeman coherences. The spectra show strong depolarization of the Cs

6p\phantom{\rule{0.2em}{0ex}}^{2}P_{3∕2}

level. The measured alignment depolarization cross section value of 186

(58)\phantom{\rule{0.3em}{0ex}}{\mathrm{\AA{}}}^{2}

is in good agreement with the experiment and theoretical predictions.