318 research outputs found

    Implementation of a double-scanning technique for studies of the Hanle effect in Rubidium vapor

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    We have studied the resonance fluorescence of a room-temperature rubidium vapor exited to the atomic 5P3/2 state (D2 line) by powerful single-frequency cw laser radiation (1.25 W/cm^2) in the presence of a magnetic field. In these studies, the slow, linear scanning of the laser frequency across the hyperfine transitions of the D2 line is combined with a fast linear scanning of the applied magnetic field, which allows us to record frequency-dependent Hanle resonances from all the groups of hyperfine transitions including V- and Lambda - type systems. Rate equations were used to simulate fluorescence signals for 85Rb due to circularly polarized exciting laser radiation with different mean frequency values and laser intensity values. The simulation show a dependance of the fluorescence on the magnetic field. The Doppler effect was taken into account by averaging the calculated signals over different velocity groups. Theoretical calculations give a width of the signal peak in good agreement with experiment

    Magnetic field--induced modification of selection rules for Rb D2_2 line monitored by selective reflection from a vapor nanocell

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    Magnetic field-induced giant modification of the probabilities of five transitions of 5S1/2,Fg=2→5P3/2,Fe=45S_{1/2}, F_g=2 \rightarrow 5P_{3/2}, F_e=4 of 85^{85}Rb and three transitions of 5S1/2,Fg=1→5P3/2,Fe=35S_{1/2}, F_g=1 \rightarrow 5P_{3/2}, F_e=3 of 87^{87}Rb forbidden by selection rules for zero magnetic field has been observed experimentally and described theoretically for the first time. For the case of excitation with circularly-polarized (σ+\sigma^+) laser radiation, the probability of Fg=2, mF=−2→Fe=4, mF=−1F_g=2, ~m_F=-2 \rightarrow F_e=4, ~m_F=-1 transition becomes the largest among the seventeen transitions of 85^{85}Rb Fg=2→Fe=1,2,3,4F_g=2 \rightarrow F_e=1,2,3,4 group, and the probability of Fg=1, mF=−1→Fe=3, mF=0F_g=1,~m_F=-1 \rightarrow F_e=3,~m_F=0 transition becomes the largest among the nine transitions of 87^{87}Rb Fg=1→Fe=0,1,2,3F_g=1 \rightarrow F_e=0,1,2,3 group, in a wide range of magnetic field 200 -- 1000 G. Complete frequency separation of individual Zeeman components was obtained by implementation of derivative selective reflection technique with a 300 nm-thick nanocell filled with Rb, allowing formation of narrow optical resonances. Possible applications are addressed. The theoretical model is perfectly consistent with the experimental results.Comment: 6 pages, 5 figure
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