한국전기전자재료학회논문지 (Journal of the Korean Institute of Electrical and Electronic Material Engineers)

  • 제26권6호
  • /
  • Pages.421-424
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  • 2013
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  • 1226-7945(pISSN)
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  • 2288-3258(eISSN)
한국전기전자재료학회 (The Korean Institute of Electrical and Electronic Material Engineers)
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간접천이대를 갖는 양자우물 구조에서의 Hall 상수

Hall Factor in the Quantum Well Structure with Indirect Conduction Minima

  • 투고 : 2013.05.02
  • 심사 : 2013.05.24
  • 발행 : 2013.06.01
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초록

The Hall factor in a quantum well structure with X or L-type indirect conduction valleys is calculated for various strain conditions. The two-dimensional constant energy surfaces of occupied valleys are proven to be identical. As a result, the Hall factor depends on the relative direction of occupied valleys to the growth direction, regardless of the number of occupied valleys. This work is widely applicable to the two-dimensional structure with indirect conduction minima for any growth direction and under different strain conditions.

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참고문헌

  1. X. Zheng, T. K. Carns, K. L. Wang, and B. Wu, Appl. Phys. Lett., 62, 504 (1993). https://doi.org/10.1063/1.108893
  2. H. H. Radamson, M. R. Sardela, Jr., O. Nur, M. Willander, B. E. Sernelius, W. X. Ni, and G. V. Hansson, Appl. Phys. Lett., 64, 1842 (1994). https://doi.org/10.1063/1.111773
  3. S. F. Nelson, K. Ismail, J. O. Chu, and B. S. Meyerson, Appl. Phys. Lett., 63, 367 (1993). https://doi.org/10.1063/1.110045
  4. E. P. De Poortere, Y. P. Shkolnikov, and M. Shayegan, Physica E, 13, 646 (2002). https://doi.org/10.1016/S1386-9477(02)00208-4
  5. K. Sawano, A. Fukumoto, Y. Hoshi, Y. Shiraki, J. Yamanaka, and K. Nakagawa, Appl. Phys. Lett., 90, 202101 (2007). https://doi.org/10.1063/1.2739324
  6. S. K. Chun, J. Korean Phys. Soc., 42, 129 (2003).
  7. I. Park and S. K. Chun, Solid-state Electronics, 49, 31 (2005). https://doi.org/10.1016/j.sse.2004.07.012
  8. S. Takagi, J. L. Hoyt, J. J. Welser, and J. F. Gibbons, J. Appl. Phys., 80, 1567 (1996). https://doi.org/10.1063/1.362953