2008
DOI: 10.1134/s0030400x08080195
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Two-level atoms moving in strong biharmonic and monochromatic counterpropagating fields

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Cited by 8 publications
(8 citation statements)
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“…It was shown that in the polarization spectrum the additional narrow resonances arise on the frequencies that satisfy of the conditions of multi -photon resonances. We can explain the result of present researches using results of papers [6,7]. The possibility of Doppler shift compensation is common feature for previous work [7] and present researches.…”
Section: Introductionmentioning
confidence: 61%
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“…It was shown that in the polarization spectrum the additional narrow resonances arise on the frequencies that satisfy of the conditions of multi -photon resonances. We can explain the result of present researches using results of papers [6,7]. The possibility of Doppler shift compensation is common feature for previous work [7] and present researches.…”
Section: Introductionmentioning
confidence: 61%
“…Two manifolds shifted on frequency 2kv arise for the case of moving atoms with velocity v. The narrow coherent peaks in the polarization and susceptibility spectrum arise additionally to known dopplerons when all fields are phased (combspectrum and phase control). This work is a prolongation of our previous work [7], where we considered the interaction of two counter propagating waves with two -level system -bi-harmonic (strong modulated) and weak counterpropagated monochromatic field. It was shown that in the polarization spectrum the additional narrow resonances arise on the frequencies that satisfy of the conditions of multi -photon resonances.…”
Section: Introductionmentioning
confidence: 96%
“…In order to prove this process we studied a three-level system. The system considered a three-level Λ−type system with a ground state (2). The transition2 ↔ 3 is driven by frequency ω 23 and Rabbi frequency G c .The transition 2 ↔ 1 is driven by frequency ω 21 and Rabbi Frequency g c .…”
Section: Theoretical Frameworkmentioning
confidence: 99%
“…Distance between control pulses for weak degenerate levels b =0.05, c=0.10, a=0.02(Signals polarized differently) As it has been shown in figure.3 intensity of signal is depends on the delay time exponential. This figure has been gotten by using parameter of distance in equation for detuning probe field [2]. the intensity of echo signal depends on the modulation index of process grating which led to a reduction of the echo signal.Based on [7] during delay time T, spectral diffusion cases frequency grating to earase and their magnitude to decay in time.The results of our simulation are shown in figure.2.…”
Section: Numerical Frameworkmentioning
confidence: 99%
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