2013
DOI: 10.1070/qe2013v043n09abeh014772
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Laser spectroscopy of sub-micrometre- and micrometre-thick caesium-vapour layers

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Cited by 11 publications
(8 citation statements)
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“…With a small pump frequency detuning from the resonance (figure 5), the EIT resonance is slightly broadened and its contrast does not change significantly. As the EIT resonance is shifted from the F g = 4 → F e = 4 transition centre by Δ = 43 MHz, which is larger than the width of the VSOP resonances observed in the MM cell by single beam spectrosocopy [20], it is accompanied by the VSOP (4-4) resonance. The last resonance is observed as a dip in absorption (fluorescence) that is centered at the F g = 4 → F e = 4 transition.…”
Section: Methodsmentioning
confidence: 69%
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“…With a small pump frequency detuning from the resonance (figure 5), the EIT resonance is slightly broadened and its contrast does not change significantly. As the EIT resonance is shifted from the F g = 4 → F e = 4 transition centre by Δ = 43 MHz, which is larger than the width of the VSOP resonances observed in the MM cell by single beam spectrosocopy [20], it is accompanied by the VSOP (4-4) resonance. The last resonance is observed as a dip in absorption (fluorescence) that is centered at the F g = 4 → F e = 4 transition.…”
Section: Methodsmentioning
confidence: 69%
“…The last resonance is observed as a dip in absorption (fluorescence) that is centered at the F g = 4 → F e = 4 transition. Under the conditions of low light intensity and atomic source temperature, at the F g = 4 → F e = 5 transition centre a sharp peak in absorption is observed [20], which is denoted as VSOP 4-5 in figure 5.…”
Section: Methodsmentioning
confidence: 99%
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“…An optical cell with internal longitudinal and transversal dimensions 8 mm contains atomic Cs vapor buffered by 20 Torr of Ne. Part of the probe radiation is directed to another cell with L=6λ thickness, which is used to provide a reference spectrum for calibration of the probe laser detuning (for more details see [15]). The probe and the coupling laser beams are separated using a polarizing BS PBS situated after the 8 mm optical cell.…”
Section: Methodsmentioning
confidence: 99%
“…Some of these early studies also applied the optical Bloch equations to a simplified two-level representation with optical pumping losses [15,18], but only in the linear excitation regime for intensities up to several milliwatts per square centimeter and Rabi frequencies less than 10 MHz. More recently, the cesium D 2 line has been studied experimentally and theoretically at somewhat higher powers up to 40 mW/cm 2 using a model based on the optical Bloch equations [19,20], but these models still were based on an open two-level system rather than including all degenerate sublevels. Furthermore, theoretical results were not compared directly to experimental curves, with the exception of some aggregate parameters, such as peak amplitude.…”
Section: Introductionmentioning
confidence: 99%