2018
DOI: 10.1016/j.optmat.2017.11.047
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Effects of electric field and light polarization on the electromagnetically induced transparency in an impurity doped quantum ring

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Cited by 22 publications
(9 citation statements)
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“…where If, however, γ 31 = γ 21 as they were taken in many theoretical papers [30][31][32][33][34][35][36][37][38][39][40], we obtain Γ = γ 21 , Ω ref = 0. Therefore ∆ ± p = iγ 21 ± Ω c and equation ( 17) can be written as:…”
Section: Transparency Induced Through Autler-townes Splittingmentioning
confidence: 99%
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“…where If, however, γ 31 = γ 21 as they were taken in many theoretical papers [30][31][32][33][34][35][36][37][38][39][40], we obtain Γ = γ 21 , Ω ref = 0. Therefore ∆ ± p = iγ 21 ± Ω c and equation ( 17) can be written as:…”
Section: Transparency Induced Through Autler-townes Splittingmentioning
confidence: 99%
“…The relevant master equations are given in Appendix A. The susceptibility of the three-level system, related to the probe field, is given through the matrix element ρ 21 = ρ * 12 for the Ξ-system and ρ 31 = ρ * 13 for Λ and V systems, and can be written in a compact form as [40]:…”
Section: Theorymentioning
confidence: 99%
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“…The resultant effective confinement potential manifestly alters a number of physical properties of LDSS with respect to a dopant-free condition and the said alteration possesses enormous technological relevance. Naturally, studies on LDSS Physics, taking into account the dopant contributions, has now become ubiquitous with some special emphasis on the optical properties of LDSS under external electric and magnetic fields [26][27][28][29][30][31].…”
Section: Introductionmentioning
confidence: 99%