scholarly journals Interface relaxation and band gap shift in epitaxial layers

AIP Advances ◽  
2012 ◽  
Vol 2 (4) ◽  
pp. 042185 ◽  
Author(s):  
Ziming Zhu ◽  
Ai Zhang ◽  
Yan He ◽  
Gang Ouyang ◽  
Guowei Yang
Keyword(s):  
Band Gap ◽  
2004 ◽  
Vol 459 (1-2) ◽  
pp. 28-31 ◽  
Author(s):  
A.P Vlasov ◽  
B.S Sokolovskii ◽  
L.S Monastyrskii ◽  
O.Yu Bonchyk ◽  
A Barcz

2000 ◽  
Vol 39 (S1) ◽  
pp. 322 ◽  
Author(s):  
Andreas Bauknecht ◽  
Susanne Siebentritt ◽  
Jürgen Albert ◽  
Yvonne Tomm ◽  
Martha Christina Lux-Steiner

2009 ◽  
Vol 7 (2) ◽  
pp. 175-178 ◽  
Author(s):  
Dimiter Alexandrov

AbstractInvestigation of the magnetic properties of MnGaN epitaxial layers as a function of external electrical field was performed on the basis of field effect structure. The structure included substrate of n-type GaN, epitaxial layer of n-type MnxGa1-xN, dielectric layer and metal layer acting as field effect device gate. Each Mn atom in MnxGa1-xN contributes 4 net spins due to the electrons occupying energy levels 4F, 4D, 4P and 4G belonging to 3d orbital, and these levels are in the energy band gap and in the top of the valence band of MnxGa1-xN. The position of the Fermi level is determined to be in the energy band gap of the layer of GaN and to be above the level 4F in the layer of MnxGa1-xN. In this way application of external negative voltage on the gate causes change in the number of electrons contributing net spins and the saturation magnetization Msat of MnxGa1-xN changes as well. It was found that Msat changes in the range 1.15 × 10−3–0.7 × 10−3 A μm−1 if the external voltage changes in the interval 0–−5V. The application of this structure for the design of spintronic devices is discussed in this paper.


1998 ◽  
Vol 123-124 ◽  
pp. 513-516 ◽  
Author(s):  
H. Ariza-Calderon ◽  
L. Tirado-Mejia ◽  
J.G. Mendoza-Alvarez ◽  
G. Torres-Delgado

Author(s):  
E.N. Mokhov ◽  
M.V. Chukichev ◽  
A.D. Roenkov ◽  
G.V. Saparin ◽  
S.K. Obyden ◽  
...  

Investigations were undertaken with SiC, a large-bandgap semiconductor material, that is rather promising for designing different optoelectronic devices. The characteristic feature of SiC is the availability of a large number of modifications, i.e. polytypes, strongly differing in the band-gap. The important problems that stand in the way of mastering SiC are the detectable doping of single crystals and epitaxial structures, the transformation of polytypes, and the structure of the intermediate layer. Crystals of SiC and its EL of 3C, 15R, 6H, 4H polytypes doped with N, Al, Ga and B were investigated. Single crystals were grown by the Leli method at T = 2600-2700°C as plates with basis planes {0001} . Epitaxial layers were grown by the sublimation "sandwich method" at T = 1700-2400°C in a vacuum or in an argon atmosphere.An analysis of the luminescence micrographs in the SEM and of the CL spectra shows that the distribution of impurities and polytype inclusions in single crystals considerably differs from that in EL. In the first case there occurs a striated inhomogeneity of CL across the whole width of the crystal which is obviously connected with an inhomogeneous distribution of dopes. Such a distribution of impurities was not observed in EL.


1994 ◽  
Vol 75 (6) ◽  
pp. 3024-3029 ◽  
Author(s):  
A. Bensaada ◽  
A. Chennouf ◽  
R. W. Cochrane ◽  
J. T. Graham ◽  
R. Leonelli ◽  
...  

1989 ◽  
Vol 67 (4) ◽  
pp. 330-338 ◽  
Author(s):  
P. Roth ◽  
M. A. Sacilotti ◽  
R. A. Masut ◽  
D. Morris ◽  
J. Young ◽  
...  

The effect of substrate orientation on the optical properties of nonpseudomorphic InxGa1–xAs epitaxial layers grown by metal organic vapour-phase epitaxy has been investigated in two series of samples. Series (a) samples were grown on GaAs substrates cut 2° off (001) towards [Formula: see text], and those of series (b) were grown on GaAs substrates cut exactly on (001). The low-temperature photoluminescence spectra of the two series of samples differ drastically. Those of the (a) series are characteristic of highly uniform, fully relaxed ternary layers and are used to determine the composition dependence of the alloy band gap and of the carbon acceptor binding energy. In contrast, those of the (b) series are dominated by an intense, low-energy emission, which is attributed to exciton recombinations in small regions of small band gap. The reduction of the band gap is tentatively assigned to the presence of In-rich regions created by the large strain fields present along dislocations. The density of dislocations is much larger in the samples of the (b) series than in those of the (a) series owing to the combination of three-dimensional growth and slow strain relaxation for layers grown on (001) substrates.


1998 ◽  
Vol 83 (7) ◽  
pp. 3678-3689 ◽  
Author(s):  
S. Chichibu ◽  
T. Mizutani ◽  
K. Murakami ◽  
T. Shioda ◽  
T. Kurafuji ◽  
...  
Keyword(s):  
Band Gap ◽  

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