Hybrid InGaN/CdZnO quantum well structures for optoelectronic applications in the short wavelength spectral region

被引:3
作者
Park, Seoung-Hwan [1 ]
Ahn, Doyeol [2 ]
机构
[1] Catholic Univ Daegu, Dept Elect Engn, Kyeongsan 712702, Kyeongbuk, South Korea
[2] Univ Seoul, Dept Elect & Comp Engn, Seoul 130743, South Korea
来源
PHYSICA STATUS SOLIDI B-BASIC SOLID STATE PHYSICS | 2013年 / 250卷 / 02期
基金
新加坡国家研究基金会;
关键词
CdZnO; GaN; InGaN; quantum wells; spontaneous emission; ZnO; BAND-GAP; ZNO; MGXZN1-XO; EXCITONS; GAIN;
D O I
10.1002/pssb.201248469
中图分类号
O469 [凝聚态物理学];
学科分类号
070205 ;
摘要
Spontaneous emission characteristics of hybrid InxGa1xN/Cd0.05Zn0.95O quantum well (QW) structures were theoretically investigated by using multi-band effective mass theory. The transition wavelength of the InGaN/CdZnO QW structure is shown to be changed from 415 to 580nm when the In content x is varied from 0.1 to 0.3. The conventional InGaN/GaN QW structure shows that its peak intensity linearly decreases with increasing peak wavelength. On the other hand, the InGaN/CdZnO QW structure shows that the spontaneous emission coefficient reaches a maximum at around the peak wavelength of 0.484 mu m, which corresponds to x=0.2. This can be explained by the fact that, in a range of the short peak wavelengths, the InGaN/CdZnO QW structure has a very shallow potential well. In a range of the longer peak wavelengths above 0.47 mu m, the InGaN/CdZnO QW structure is expected to have a larger spontaneous emission peak than the InGaN/GaN QW structure. This can be explained by the fact that the former has a reduced internal field compared to the latter.
引用
收藏
页码:378 / 381
页数:4
相关论文
共 25 条
[1]   Theory of non-Markovian optical gain in quantum-well lasers [J].
Ahn, D .
PROGRESS IN QUANTUM ELECTRONICS, 1997, 21 (03) :249-287
[2]  
Ahn D., 2011, ENG QUANTUM MECH
[3]   Simulation of hybrid ZnO/AlGaN single-heterostructure light-emitting diode [J].
Bulashevich, KA ;
Evstratov, IY ;
Nabokov, VN ;
Karpov, SY .
APPLIED PHYSICS LETTERS, 2005, 87 (24) :1-3
[4]   STRAIN AND CHARGE-DISTRIBUTION IN GAN-ALN-GAN SEMICONDUCTOR-INSULATOR-SEMICONDUCTOR STRUCTURE FOR ARBITRARY GROWTH ORIENTATION [J].
BYKHOVSKI, A ;
GELMONT, B ;
SHUR, M .
APPLIED PHYSICS LETTERS, 1993, 63 (16) :2243-2245
[5]   Realization of band gap above 5.0 eV in metastable cubic-phase MgxZn1-xO alloy films [J].
Choopun, S ;
Vispute, RD ;
Yang, W ;
Sharma, RP ;
Venkatesan, T ;
Shen, H .
APPLIED PHYSICS LETTERS, 2002, 80 (09) :1529-1531
[6]  
Chow W. W., 1994, SEMICONDUCTOR LASER, P119
[7]   k center dot p method for strained wurtzite semiconductors [J].
Chuang, SL ;
Chang, CS .
PHYSICAL REVIEW B, 1996, 54 (04) :2491-2504
[8]   Tunable electroluminescence from n-ZnCdO/p-GaN heterojunction [J].
Fang, Fang ;
Zhao, Dongxu ;
Fang, Xuan ;
Li, Jinhua ;
Wei, Zhipeng ;
Wang, Shaozhuan ;
Wu, Jilong ;
Shen, Dezhen ;
Wang, Xiaohua .
JOURNAL OF PHYSICS AND CHEMISTRY OF SOLIDS, 2012, 73 (02) :217-220
[9]   Polarization, piezoelectric constants, and elastic constants of ZnO, MgO, and CdO [J].
Gopal, P ;
Spaldin, NA .
JOURNAL OF ELECTRONIC MATERIALS, 2006, 35 (04) :538-542
[10]  
Haug H., 1993, QUANTUM THEORY OPTIC, P195