Exciton localization behaviour in different well width undoped GaN/Al0.07Ga0.93N nanostructures

被引:6
|
作者
Sabooni, M. [1 ]
Esmaeili, M.
Haratizadeh, H.
Monemar, B.
Paskov, P.
Kamiyama, S.
Iwaya, M.
Amano, H.
Akasaki, I.
机构
[1] Islamic Azad Univ, Dept Phys, Shahrood Branch, Shahrood, Iran
[2] Shahrood Univ Technol, Dept Phys, Shahrood, Iran
[3] Linkoping Univ, Dept Phys, S-58183 Linkoping, Sweden
[4] Linkoping Univ, Dept Measurements Technol, S-58183 Linkoping, Sweden
[5] Meijo Univ, Dept Mat Sci & Engn, Tempaku Ku, Nagoya, Aichi 468, Japan
[6] Meijo Univ, Hi Tech Res Ctr, Tempaku Ku, Nagoya, Aichi 468, Japan
关键词
photoluminescence; time-resolved photoluminescence; quantum well; exciton localization; GaN/AlGaN;
D O I
10.2478/s11772-007-0017-5
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
We report results from optical spectroscopy such as photoluminescence (PL) and time resolved photo-luminescence (TRPL) techniques from different well width MOCVD grown GaNlAl(0.07)Ga(0.93)N MQW samples. There is evidence of localization at low temperature in all samples. The decay time of all samples becomes non-exponential when the detection energy is increased with respect to the peak of the emission. Localization of carriers (excitons) is demonstrated by the "S-shape" dependences of the PE peak energies on the temperature. The time-resolved PL spectra of the 3-nm well multi quantum wells reveal that the spectral peak position shifts toward lower energies as the decay time increases and becomes red-shifted at longer decay times. Their is a gradient in the PL decay time across the emission peak profile, so that the PL process at low temperatures is a free e election-localized hole transition.
引用
收藏
页码:163 / 167
页数:5
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