1997
DOI: 10.1070/pu1997v040n12abeh000318
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Simple atomic systems in resonant laser fields

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Cited by 34 publications
(13 citation statements)
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“…This line profile represents the dominant term in Im ρ 21 and is separated out in Eq. (7). But in addition the function f (Ω 2 α , Ω 2 β , ∆ α , ∆ β ) in Eq.…”
Section: Numerical Results and Discussionmentioning
confidence: 99%
“…This line profile represents the dominant term in Im ρ 21 and is separated out in Eq. (7). But in addition the function f (Ω 2 α , Ω 2 β , ∆ α , ∆ β ) in Eq.…”
Section: Numerical Results and Discussionmentioning
confidence: 99%
“…For many physical considerations of light‐matter interaction, it is sufficient to take only two energy eigenstates into account, namely, the states |1 and |2 with the energy difference E2E1 close to the incident light photon energy ω. The pair states can be two levels in atoms, spin‐split states in the magnetic resonance, tunneling two‐level systems in dielectric glasses, the ground electron and hole quantum‐confined levels in semiconductor quantum dots, etc. In such systems, the saturation of resonant optical properties is controlled by two characteristic times, longitudinal and transverse relaxation times T1 and T2, respectively (T22T1).…”
Section: Introductionmentioning
confidence: 99%
“…So, for the efficient transfer of population it is necessary to provide the adiabaticity of interaction of the atom with laser pulses. It is known that the adiabaticity for a single atom can be provided under the following conditions [15,29]:…”
Section: Model and Conditions Of Population Transfer In The Mediummentioning
confidence: 99%