欢迎登录材料期刊网

材料期刊网

高级检索

摘要 本文介绍利用界面混合技术对GaAs/AlGaAs量子阱结构进 行微调,通过荧光光谱和光响应电流谱给出了质子注入和快速退火对 禁带宽度及导带内子带位置的影响,荧光光谱峰位随注入剂量(5× 1014~5×1015~cm-2)的增加从766~nm持续蓝移至753~nm,光响 应峰值波长从8.2~μm移至10.3~μm。

In this paper we shall demonstrate the use of intermixing in modify of GaAs/AlGaAs quantum-well. The paper shows that proton implantation can achieve large energy shifts after standard annealing procedures. The PL and photoresponse spectrum were measured as a function of ion dose in the range 5×1014~cm-2 to 2.5×1015~cm-2, the peak photoresponse wavelength was tunable between 8.4~μm to 10.2~μm and PL peak from 780~nm to 850~nm.

参考文献

[1] Levine B F. Quantum-well infrared photodetectors. J. Appl. Phys., 1993, 74
[2] Gunapala S D, Liu J K, Park J S et al. 9~μm cutoff 256× 256 GaAs/AlGaAs quantum well infrared photodetector hand-held camera, IEEE Trans. Electron Devices, 1997, 44(1): 51
[3] Gunapala S D, Park J S, Sarusi G et al. 128× 128 GaAs/AlGaAs quantum well infrared photodetector focal plane array for imaging at 15~μm. IEEE Trans. Electron Devices, 1997, 44(1): 45
[4] Chen C J, Choi K K, Chang W H et al. Two-color corrugated quantum-well infrared photodetector for remote temperature sensing. Appl. Phys. Lett., 1998, 72(1): 7
[5] Elman B, Koteles E S, Melman P et al. Effect of heat treatment on InGaAs/GaAs quantum wells. J. Appl. Phys., 1989, 66(2): 2104
[6] Tan H H, Williams J S, Jagadish C et al. Large energy shifts in GaAs-AlGaAs quantum wells by proton irradiation-induced intermixing. Appl. Phys. Lett., 1996, 68: 1996
[7] Steele A G, Buchanan M, Liu H C et al. Postgrowth tuning of quantum-well infrared detectors by rapid thermal annealing. J. Appl. Phys., 1994, 75(12): 8234
[8] Li E H, Weiss B L, Chan K S. Effect of interdiffusion on the subbands in an AlxGa1-xAs single-quantum-well structure. Phys. Rev. B, 1992, 46(23): 1518
[9] Lee Alex S W, Li E H. Effect of interdiffusion of quantum well infrared photodetector. Appl. Phys. Lett., 1996, 69(23): 518
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%