共查询到5条相似文献,搜索用时 0 毫秒
1.
P. V. Seredin A. S. Lenshin A. V. Glotov I. N. Arsentyev D. A. Vinokurov I. S. Tarasov T. Prutskij H. Leiste M. Rinke 《Semiconductors》2014,48(8):1094-1102
The high-resolution X-ray diffraction technique, Raman spectroscopy, and photoluminescence spectroscopy are used to study the structural, optical, and electron energy properties of epitaxial Al x Ga1 ? x As1 ? y P y :Mg alloy films grown by metal-organic chemical vapor deposition (MOCVD). It is shown that the introduction of a Mg impurity into the quaternary alloy provides high charge-carrier concentrations. A decrease in the growth temperature yields a decrease in the charge-carrier concentration in films doped with magnesium at a small gas-carrier flux of the acceptor impurity, whereas an increase in the flux results in an increase in the acceptor-impurity concentration, which is reflected in the character of the photoluminescence spectra. 相似文献
2.
A. Aissat S. Nacer F. Ykhlef J.P. Vilcot 《Materials Science in Semiconductor Processing》2013,16(6):1936-1942
The aim of this work is to model the properties of GaInAsNSb/GaAs compressively strained structures. Indeed, Ga1?xInxAs1?y?zNySbz has been found to be a potentially superior material to GaInAsN for long wavelength laser dedicated to optical fiber communications. Furthermore, this material can be grown on GaAs substrate while having a bandgap smaller than that of GaInNAs. The influence of nitrogen and antimony on the bandgap and the transition energy is explored. Also, the effect of these two elements on the optical gain and threshold current density is investigated. For example, a structure composed of one 7.5 nm thick quantum well of material with In=30%, N=3.5%, Sb=1% composition exhibits a threshold current density of 339.8 A/cm2 and an emission wavelength of 1.5365 μm (at T=300 K). It can be shown that increasing the concentration of indium to 35% with a concentration of nitrogen and antimony, of 2.5% and 1%, respectively, results in a decrease of the threshold current density down to 253.7 A/cm2 for a two well structure. Same structure incorporating five wells shows a threshold current density as low as 221.4 A/cm2 for T=300 K, which agrees well with the reported experimental results. 相似文献
3.
F. Dimroth R. Beckert M. Meusel U. Schubert A. W. Bett 《Progress in Photovoltaics: Research and Applications》2001,9(3):165-178
The use of Ga1−xInxAs instead of GaAs as a bottom solar cell in a GayIn1−yP/Ga1−xInxAs tandem structure increases the flexibility of choosing the optimum bandgap combination of materials for a multijunction solar cell. Higher theoretical efficiencies are calculated and different cell concepts are suggested for space and terrestrial concentrator applications. Various GayIn1−yP/Ga1−xInxAs material combinations have been investigated for the first time and efficiencies up to 24·1% (AM0) and 27·0% (AM1·5 direct) have been reached under one-sun conditions. An efficiency of 30·0–31·3% was measured for a Ga0·35In0·65P/Ga0·83In0·17As tandem concentrator cell with prismatic cover at 300 suns. The top and bottom cell layers of this structure are grown lattice-matched to each other, but a large mismatch is introduced at the interface to the GaAs substrate. This cell structure is well suited for the use in next-generation terrestrial concentrators working at high concentration ratios. For the first time a cell efficiency up to 29–30% has been measured at concentration levels up to 1300 suns. A small prototype concentrator with Fresnel lenses and four tandem solar cells working at C = 120 has been constructed, with an outdoor efficiency of 23%. Copyright © 2001 John Wiley & Sons, Ltd. 相似文献
4.
Formulas are derived for, and a numerical analysis made of, the dependence of the transverse phase relaxation time on electron
energy for resonant current flow through GaAs/AlxGa1−x
As superlattices with doped quantum wells. The parameters are chosen to be close to those of superlattices used for creating
photodiodes for operation at λ⋍10 μm. The analysis is limited to the interactions of electrons with neutral atoms and impurity
ions at low temperatures. Resonant current flow is ensured by an electric field that brings the ground state and the first
excited state of the “Stark ladder” into resonance with neighboring, weakly interacting quantum wells.
Fiz. Tekh. Poluprovodn. 33, 438–444 (April 1999) 相似文献
5.
A. Yildiz P. Tasli B. Sarikavak S. B. Lisesivdin M. K. Ozturk M. Kasap S. Ozcelik E. Ozbay 《Semiconductors》2011,45(1):33-36
Electrical transport data for Al-rich AlGaN layers grown by metal-organic chemical vapor deposition (MOCVD) are presented
and analyzed in the temperature range 135–300 K. The temperature dependence of electrical conductivity indicated that conductivity
in the films was controlled by potential barriers caused by carrier depletion at grain boundaries in the material. The Seto’s
grain boundary model provided a complete framework for understanding of the conductivity behavior. Various electrical parameters
of the present samples such as grain boundary potential, donor concentration, surface trap density, and Debye screening length
were extracted. 相似文献