2000
DOI: 10.1116/1.1305921
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ZnSe/CdTe/ZnSe heterostructures

Abstract: Molecular-beam epitaxy growth and nitrogen doping of hexagonal ZnSe and ZnCdSe/ZnSe quantum well structures on hexagonal ZnMgSSe bulk substrates

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Cited by 7 publications
(3 citation statements)
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“…In many studies, the interpretation is based on the mosaic block model. [6][7][8][9] Determination of the dislocation densities from peak widths [9][10][11][12] is based on different variants of the formulas proposed for the classical models in powder diffraction. [13][14][15] A direct Monte Carlo calculation of the diffraction peak profile due to parallel straight dislocations demonstrates that the peak width depends not only on the dislocation density but also on the spatial correlations in dislocation positions.…”
Section: Introductionmentioning
confidence: 99%
“…In many studies, the interpretation is based on the mosaic block model. [6][7][8][9] Determination of the dislocation densities from peak widths [9][10][11][12] is based on different variants of the formulas proposed for the classical models in powder diffraction. [13][14][15] A direct Monte Carlo calculation of the diffraction peak profile due to parallel straight dislocations demonstrates that the peak width depends not only on the dislocation density but also on the spatial correlations in dislocation positions.…”
Section: Introductionmentioning
confidence: 99%
“…It should be easier in the case of epitaxially grown structures, which offer also a feasibility of p-and n-type doping. On the other hand, strain resulting from a very large lattice mismatch [26][27][28][29][30] between CdTe (a CdTe = 0.648 nm) and ZnSe (a ZnSe = 0.567 nm) (above 14%) leads to a high spatial density of QDs combining these two compounds. This has precluded spectroscopy of individual QDs in such mixed type systems so far.…”
Section: Cd(sete)/znse Quantum Dots Produced By a Mn-assisted Epitaxi...mentioning
confidence: 99%
“…X-ray reciprocal space maps allow for the determination of both the position and the broadening of a selected reflection in reciprocal space, and are thus often employed to study the structural properties of epitaxial group III nitride films (Holý et al, 1993;Heinke et al, 1994;Metzger et al, 1998;Chierchia et al, 2001Chierchia et al, , 2003Paduano et al, 2003;Kirste et al, 2005;Vickers et al, 2005;Kyutt et al, 2009;Barchuk et al, 2010Barchuk et al, , 2011Lazarev et al, 2013). The interpretation of these maps is frequently based on the assumption that the film constitutes a mosaic crystal (Holý et al, 1993;Rubini et al, 2000;Chierchia et al, 2001Chierchia et al, , 2003, picturing the film as consisting of finite-sized crystal blocks rigidly rotated with respect to each other. The broadening of reciprocal lattice points as observed in reciprocal space maps is interpreted in terms of the out-of-plane misorientation (the 'tilt') of the blocks with respect to each other and the average block size defining the lateral coherence length for the X-ray wavefield.…”
Section: Introductionmentioning
confidence: 99%