2000
DOI: 10.1103/physreva.61.033409
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Interference effects in a two-color laser beam interaction with alkali-metal atoms

Abstract: The interaction of an alkali-metal atom with two different color laser beams is analyzed. The quantum interference effect is studied in weak and strong field limits. Our theoretical results are related to the recent experimental data for the S 1/2 →S 1/2 two-photon transition in Na and Rb atoms. It is shown that the interference profile becomes narrow for moderately strong fields and the destruction of the interference is predicted for very strong ones. The electromagnetically induced interference effects are … Show more

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Cited by 4 publications
(5 citation statements)
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“…The excitation spectrum for generating 4-5 emission can be obtained by fixing the emission frequency ω = ω 45 and tuning the frequencies of the laser fields (I) and (II), respectively, near the 3S-3P and 3P-5S resonant transitions while the two-photon resonance condition be satisfied, that is, S( ) = Re (z, )| z=i ω 45 . In [16], the authors calculated the population in level 4 by perturbation expansion of the density matrix element ρ 44 up to the fourth order. In this paper, we do not calculate the population ρ 44 , but calculate the excitation spectrum for generating 5S-4P emission.…”
Section: Motion Equation Of the Density Matrixmentioning
confidence: 99%
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“…The excitation spectrum for generating 4-5 emission can be obtained by fixing the emission frequency ω = ω 45 and tuning the frequencies of the laser fields (I) and (II), respectively, near the 3S-3P and 3P-5S resonant transitions while the two-photon resonance condition be satisfied, that is, S( ) = Re (z, )| z=i ω 45 . In [16], the authors calculated the population in level 4 by perturbation expansion of the density matrix element ρ 44 up to the fourth order. In this paper, we do not calculate the population ρ 44 , but calculate the excitation spectrum for generating 5S-4P emission.…”
Section: Motion Equation Of the Density Matrixmentioning
confidence: 99%
“…In this paper, we do not calculate the population ρ 44 , but calculate the excitation spectrum for generating 5S-4P emission. As analysed in [12,19], the population ρ 44 in [16] includes collision-free population (related to Raman scattering (3P 1/2,3/2 -4P)) and collisionaided population (related to the resonant emission (5S-4P)). Since we study the interference between the two collision-assisted two-step two-photon transition pathways 1-2-4 and 1-3-4, which results in the real population of level 4, and the intensity of 4-5 emission is the direct measure of the real population in level 4, the excitation spectrum for generating 4-5 emission can be used to examine the collision-induced quantum interference.…”
Section: Motion Equation Of the Density Matrixmentioning
confidence: 99%
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“…The first attempt at a theoretical analysis of this system was presented by Czub et al (1986). However, in this work they did not include the propagation effects and the growth of the Raman beam through the stimulated emission (one-photon process) on the collisionbroadened 2 P 1/2 → 2 S 1/2 transition.…”
Section: Introductionmentioning
confidence: 99%