Long Wave Polar Modes in Semiconductor Heterostructures 1998
DOI: 10.1016/b978-008042694-5/50004-9
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Polar optical modes in heterostructures

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Cited by 13 publications
(33 citation statements)
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“…We follow the approach to COP described in [23][24][25], where a system of coupled differential equations for the relative ion displacement u and the electric potential ϕ should be solved within each nanolayer of the considered nanostructure. The solutions obtained for each nanolayer must be matched at the corresponding interfaces, involving both mechanical and electric boundary conditions.…”
Section: Analytical Resultsmentioning
confidence: 99%
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“…We follow the approach to COP described in [23][24][25], where a system of coupled differential equations for the relative ion displacement u and the electric potential ϕ should be solved within each nanolayer of the considered nanostructure. The solutions obtained for each nanolayer must be matched at the corresponding interfaces, involving both mechanical and electric boundary conditions.…”
Section: Analytical Resultsmentioning
confidence: 99%
“…Within the long-wave limit, and also applying a continuum approach, a theoretically more reliable treatment was reported in Refs. [22][23][24][25]. The present work focuses on the application of this theory to the spherical QD/QW nanostructure, but we shall limit ourselves to the analysis of the so-called uncoupled modes representing polar optical oscillations of strict transversal character and mechanical nature.…”
Section: Introductionmentioning
confidence: 99%
“…For both equations eigenvalues are ±k; k = ω c (n 0 + iξ 0 ) 2 − (n a sin θ) 2 for Equation (44) and…”
Section: The Anisotropic Layered Systemmentioning
confidence: 99%
“…(n e + iξ e ) 2 − (n a sin θ) 2 for Equation (45). Therefore in this case both components E 1 (z) and E 2 (z) can be calculated using a 2 × 2 associated transfer matrix as in the isotropic case.…”
Section: The Anisotropic Layered Systemmentioning
confidence: 99%
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