HgTe/Cdte superlattices grown on CdZnTe(211)B by MBE

  • Kang, T.W. (Department of Physics, Dongguk University) ;
  • Jeong, C.S. (Department of physics & biophysics, Catholic University Medical College) ;
  • Leem, J.H. (Department of Physics, Dongguk University) ;
  • Ryu, Y.S. (Department of Physics, Dongguk University) ;
  • Hyun, J.K. (Department of Physics, Dongguk University) ;
  • Jeon, H.C. (Department of Physics, Dongguk University) ;
  • Lee, H.Y. (Department of Physics, Dongguk University) ;
  • Han, M.S. (Department of Physics, Dongguk University)
  • Published : 1997.10.01

Abstract

Hg-Te-CdTe superlattices have received much interests over the last several years as a potential material for its applications for detecting devices and optoelectronics. We have grown the HgTe-CdTe superlattice using MBE. in our lab. We have carried out DCRC spectroscopy after growth of HgTe-CdTe superlattice with varying the superlattice periods and controlling the barrier thickness and we have that the presence of the main peak and the satellite peaks. We obtained 20 arcsec of FWHM over 100 periods of superlattice. We also note that high peak intensity shows the high quality of the sample and each layer of superlattice has abrupt interfaces. The angular separation between the main peak(m=0) and the first satellite peak(m=$\pm$1) is increased when the barrier layer thickness in superlatice layers are decreased. The separation between the first setellite peak(m=$\pm$1) and the second satellite peak(m$\pm$2) is increased similarly. The number of the satellite peak is a qualitative measure of the interfacial abruptness of the superlattice.

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