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Physical Review A

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

S. B. Bayram, Seda Kin, M. J. Welsh, Jacob D Hinkle

Published Apr 21, 2006• 10 citations
Publisher

Abstract

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.

DOI
10.1103/physreva.73.042713

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Depolarization of 6P322 cesium atoms, induced in collisions with noble gases

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Physical Review A•Dec 1, 1976•13 citations
An experimental investigation of the Cs 6s2S1∕2\ensuremath→6p2P3∕2\ensuremath→10s2S1∕26s\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}6s2S1∕2​\ensuremath→6p2P3∕2​\ensuremath→10s2S1∕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 6p2P3∕26p\phantom{\rule{0.2em}{0ex}}^{2}P_{3∕2}6p2P3∕2​ level due to collisions between ground-level argon and excited 6p2P3∕26p\phantom{\rule{0.2em}{0ex}}^{2}P_{3∕2}6p2P3∕2​ cesium atoms over the Zeeman coherences. The spectra show strong depolarization of the Cs 6p2P3∕26p\phantom{\rule{0.2em}{0ex}}^{2}P_{3∕2}6p2P3∕2​ level. The measured alignment depolarization cross section value of 186 (58)A˚2(58)\phantom{\rule{0.3em}{0ex}}{\mathrm{\AA{}}}^{2}(58)A˚2 is in good agreement with the experiment and theoretical predictions.
An experimental investigation of the Cs 6s {sup 2}S{sub 1/2}{yields}6p {sup 2}P{sub 3/2}{yields}10s {sup 2}S{sub 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 {sup 2}P{sub 3/2} level due to collisions between ground-level argon and excited 6p {sup 2}P{sub 3/2} cesium atoms over the Zeeman coherences. The spectra show strong depolarization of the Cs 6p {sup 2}P{sub 3/2} level. The measured alignment depolarization cross section value of 186 (58) A{sup 2} is in good agreement with the experiment and theoretical predictions.
An experimental investigation of the Cs 6s 2S1/2→6p 2P3/2→10s 2S1/2 double-resonance two-photon polar-ization spectrum has been made. In the investigation, a linear polarization degree was measured to extract the alignment depolarization cross section in the cesium 6p 2P3/2 level due to collisions between ground-level argon and excited 6p 2P3/2 cesium atoms over the Zeeman coherences. The spectra show strong depolarization of the Cs 6p 2P3/2 level. The measured alignment depolarization cross section value of 186 58 Å2 is in good agreement with the experiment and theoretical predictions. DOI: 10.1103/PhysRevA.73.042713 PACS numbers: 32.80.t, 32.70.n I.
We have experimentally investigated the anisotropy-dependent circular polarization spectra of the 133Cs^{133}\mathrm{Cs}133Cs $6s^{2}S_{1∕2}\ensuremath{\rightarrow}6p^{2}P_{3∕2}\ensuremath{\rightarrow}10s^{2}S_{1∕2}$ double-resonance transition in the presence of Ar. Satisfaction of double-resonance condition, achieved by use of a two-photon two-color pulse laser excitation scheme, was monitored by measurement of the intensity of the $9p^{2}P_{1∕2}\ensuremath{\rightarrow}6s^{2}S_{1∕2}$ cascade fluorescence at 361.73nm361.73\phantom{\rule{0.3em}{0ex}}\mathrm{nm}361.73nm. In the experiment anisotropies, namely, alignment and orientation in the 6p2P3∕26p^{2}P_{3∕2}6p2P3∕2​ level, were produced from circularly polarized light with positive helicity. Then, a circular polarization degree was measured when both lasers were circularly polarized with positive helicities, and alternately positive and negative helicities for the $6p^{2}P_{3∕2}\ensuremath{\rightarrow}10s^{2}S_{1∕2}$ transition. From the measurement, we obtained the orientation-dependent depolarization cross section in the 6p2P3∕26p^{2}P_{3∕2}6p2P3∕2​ level due to collisions with ground-level argon atoms. A disorientation cross section value of 151 (42)A˚2(42)\phantom{\rule{0.3em}{0ex}}{\mathrm{\AA{}}}^{2}(42)A˚2 is reported.
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Measurements of collisional depolarization cross sections play an important role in gaining valuable information about the interaction between inert and rare-gas atoms.A key element in understanding collisional dynamics is the detailed analysis of the polarization of the emitted photons.In order to investigate the collisional cross section of the excited J=1/2 cesium atoms, by collisions with the ground level argon atoms, experimental measurements were made studying circular polarization spectra.Orientation in the J=1/2 level was optically induced by circularly polarized light with a positive helicity.A two-photon double-resonance (6s 2 S 1/2 →6p 2 P 1/2 → 10s 2 S 1/2 ) condition was achieved using nanosecond pulsed dye lasers, and the intensity of the cascade fluorescence was monitored in the presence of argon atoms ranging from 10 -4 torr to 100 torr.
Cross sections for relaxation of circular and linear polarization of 62P326^{2}P_{\frac{3}{2}}62P23​​ cesium atoms, induced in collisions with ground-state He, Ne, Ar, and Xe, have been determined by Zeeman scanning techniques. A fluorescence cell containing low-pressure cesium vapor together with a buffer gas was irradiated with circularly or linearly polarized 8521-\AA{} Cs resonance radiation, producing excited and polarized Cs atoms which became depolarized in subsequent collisions with the buffer-gas atoms. The resulting depolarization of the cesium resonance fluorescence was monitored in relation to buffer-gas pressure (0-10 Torr) and to the strength of the ambient magnetic field (0-10 kG). At low fields at which the nuclear spin $\stackrel{\ensuremath{\rightarrow}}{\mathrm{I}}$ is coupled to the electronic angular momentum $\stackrel{\ensuremath{\rightarrow}}{\mathrm{J}}$, the measurements yielded depolarization cross sections Q(circ.)Q(\mathrm{circ}.)Q(circ.) and Q(lin.)Q(\mathrm{lin}.)Q(lin.), which agree within experimental error with theoretical values calculated for spin-coupled conditions. At kilogauss fields with $\stackrel{\ensuremath{\rightarrow}}{\mathrm{I}}$ and $\stackrel{\ensuremath{\rightarrow}}{\mathrm{J}}$ decoupled, the experiments produced cross sections for disorientation and disalignment, which are also in satisfactory agreement with the appropriate theoretical predictions. The results indicate that the nuclear spin has a more pronounced effect on the collisional relaxation of the atomic dipole than of the quadrupole.