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Quantum device designing (QDD) for future semiconductor engineering.
John, J D; Nishimoto, S; Kadowaki, N; Saito, I; Okano, K; Okano, S; Zahn, D R T; Masuzawa, T; Yamada, T; Chua, D H C; Ito, T.
Affiliation
  • John JD; Department of Physics, International Christian University, 3-10-2 Osawa, Mitaka, Tokyo 181-8585, Japan.
  • Nishimoto S; Department of Physics, International Christian University, 3-10-2 Osawa, Mitaka, Tokyo 181-8585, Japan.
  • Kadowaki N; Department of Physics, International Christian University, 3-10-2 Osawa, Mitaka, Tokyo 181-8585, Japan.
  • Saito I; Department of Physics, International Christian University, 3-10-2 Osawa, Mitaka, Tokyo 181-8585, Japan.
  • Okano K; Department of Physics, International Christian University, 3-10-2 Osawa, Mitaka, Tokyo 181-8585, Japan.
  • Okano S; Semiconductor Physics, Chemnitz University of Technology, D-09107 Chemnitz, Germany.
  • Zahn DRT; Semiconductor Physics, Chemnitz University of Technology, D-09107 Chemnitz, Germany.
  • Masuzawa T; Research Institute of Electronics, Shizuoka University, 3-5-1 Johoku, Naka-ku, Hamamatsu 432-8011, Japan.
  • Yamada T; Nanomaterials Research Institute, National Institute of Advanced Industrial Science and Technology, 1-1-1 Higashi, Tsukuba 305-8565, Japan.
  • Chua DHC; Department of Material Science and Engineering, National University of Singapore, 9 Engineering Drive, Singapore 119077.
  • Ito T; Eiwa Bussan Company Limited, 2-9-14 Uchikanda, Chiyoda-ku, Tokyo, Japan.
Rev Sci Instrum ; 93(3): 034703, 2022 Mar 01.
Article in En | MEDLINE | ID: mdl-35365006
ABSTRACT
In semiconductor device history, a trend is observed where narrowing and increasing the number of material layers improve device functionality, with diodes, transistors, thyristors, and superlattices following this trend. While superlattices promise unique functionality, they are not widely adopted due to a technology barrier, requiring advanced fabrication, such as molecular beam epitaxy and lattice-matched materials. Here, a method to design quantum devices using amorphous materials and physical vapor deposition is presented. It is shown that the multiplication gain M depends on the number of layers of the superlattice, N, as M = kN, with k as a factor indicating the efficiency of multiplication. This M is, however, a trade-off with transit time, which also depends on N. To demonstrate, photodetector devices are fabricated on Si, with the superlattice of Se and As2Se3, and characterized using current-voltage (I-V) and current-time (I-T) measurements. For superlattices with the total layer thicknesses of 200 nm and 2 µm, the results show that k200nm = 0.916 and k2µm = 0.384, respectively. The results confirm that the multiplication factor is related to the number of superlattice layers, showing the effectiveness of the design approach.

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Rev Sci Instrum Year: 2022 Document type: Article Affiliation country: Japón

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Rev Sci Instrum Year: 2022 Document type: Article Affiliation country: Japón
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