2018
DOI: 10.1016/j.optmat.2018.01.043
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Electromagnetically induced transparency in a multilayered spherical quantum dot with hydrogenic impurity

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Cited by 15 publications
(4 citation statements)
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“…The BOR-FDTD method is one of the most widely used methods in electromagnetic simulation of structures that contain azimuthal symmetry such as modeling wave propagation through optical lenses [53], resonant cavities [54] and the calculation of spontaneous emission lifetime [55]. A large number of low dimensional semiconductors including spherical, cylindrical, cone-like and multilayered spherical QDs present symmetry around an axis of rotation [56][57][58][59][60][61]. The BOR-FDTD method has a great advantage over the 3D FDTD method for a rotationally symmetric problem, since in this approach a 3D problem is reduced to a numerically solvable two dimensional one.…”
Section: Introductionmentioning
confidence: 99%
“…The BOR-FDTD method is one of the most widely used methods in electromagnetic simulation of structures that contain azimuthal symmetry such as modeling wave propagation through optical lenses [53], resonant cavities [54] and the calculation of spontaneous emission lifetime [55]. A large number of low dimensional semiconductors including spherical, cylindrical, cone-like and multilayered spherical QDs present symmetry around an axis of rotation [56][57][58][59][60][61]. The BOR-FDTD method has a great advantage over the 3D FDTD method for a rotationally symmetric problem, since in this approach a 3D problem is reduced to a numerically solvable two dimensional one.…”
Section: Introductionmentioning
confidence: 99%
“…The effect was proposed theoretically in 1989 [1] and experimentally verified in 1991 [2]. Since then, the EIT has attracted much studies in atomic/molecular systems [3][4][5][6][7][8][9][10][11][12][13][14] and quantum well/dot systems [15][16][17][18][19] due to its unusual optical properties and promises for potential applications, such as lasing without inversion [20], high resolution spectroscopy [21], nonlinear optics at low light levels [22], giant Kerr nonlinearity [23][24][25][26], and optical bistability (OB) [27]. In addition to the reduction of the resonant absorption, modification of refractive index of the EIT medium was also studied theoretically [28,29] and experimentally [8,30].…”
Section: Introductionmentioning
confidence: 99%
“…In the early years of EIT study, three-level configurations were the main objects which give single-window EIT signature [3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18][19]. It is worthy to mention here that the linear and nonlinear susceptibilities of such single-window EIT medium have been well understood and promoted significant progress in the EIT related applications .…”
Section: Introductionmentioning
confidence: 99%
“…Here, the polarization of the laser fields is chosen in such a way that they couple to the particular energy levels of the configuration and no other levels are considered, thus forming the closed system. For example, in Pavlović et al, 2018, the laser polarization is such that the probe laser excites the transition , while the control laser excites the transition As determined by the selection rules, level decays to the level only, while level undergoes the spontaneous emission exclusively to the level . However, if the polarization of the laser is chosen in a different way, such that the probe laser excites the transition , while the control laser excites the transition , the highest level then decays to the levels , and , which, due to the spherical symmetry of the problem, all have the same energy.…”
Section: Introductionmentioning
confidence: 99%