Codoping method for the fabrication of low-resistivity wide band-gap semiconductors in p-type GaN, p-type AlN and n-type diamond: prediction versus experiment

被引:120
作者
Katayama-Yoshida, H [1 ]
Nishimatsu, T
Yamamoto, T
Orita, N
机构
[1] Osaka Univ, Dept Condensed Matter Phys, Inst Sci & Ind Res, Osaka 5670047, Japan
[2] Tohoku Univ, Inst Mat Res, Sendai, Miyagi 9808577, Japan
[3] Kochi Univ Technol, Dept Elect & Photon Syst Engn, Kochi 7828502, Japan
[4] Natl Inst Adv Ind Sci & Technol, Tsukuba, Ibaraki 3058568, Japan
关键词
D O I
10.1088/0953-8984/13/40/304
中图分类号
O469 [凝聚态物理学];
学科分类号
070205 ;
摘要
We review our new valence control method of a co-doping for the fabrication of low-resistivity p-type GaN, p-type AIN and n-type diamond. The co-doping method is proposed based upon ab initio electronic structure calculation in order to solve the uni-polarity and the compensation problems in the wide bandgap semiconductors. In the co-doping method, we dope both the acceptors and donors at the same time by forming the meta-stable acceptor-donor-acceptor complexes for the p-type. or donor-acceptor-donor complexes for the n-type under thermal non-equilibrium crystal growth conditions. We propose the following co-doping method to fabricate the low-resistivity wide band-gap semiconductors; p-type GaN: [Si + 2Mg (or Be)], [H + 2Mg (or Be)], [O + 2Mg (or Be)], p-type AIN: [O + 2C] and n-type diamond: [B + 2N], [H + S], [H + 2P]. We compare our prediction of the co-doping method with the recent successful experiments to fabricate the low-resistivity p-type GaN, p-type AIN and n-type diamond. We show that the co-doping method is the efficient and universal doping method by which to avoid carrier compensation with an increase of the solubility of the dopant, to increase the activation rate by decreasing the ionization energy of acceptors and donors, and to increase the mobility of the carrier.
引用
收藏
页码:8901 / 8914
页数:14
相关论文
共 37 条
[1]  
AKASAKI I, 1998, COMMUNICATON
[2]   High p-type conductivity in cubic GaN/GaAs(113)A by using Be as the acceptor and O as the codopant [J].
Brandt, O ;
Yang, H ;
Kostial, H ;
Ploog, KH .
APPLIED PHYSICS LETTERS, 1996, 69 (18) :2707-2709
[3]   UNIFIED APPROACH FOR MOLECULAR-DYNAMICS AND DENSITY-FUNCTIONAL THEORY [J].
CAR, R ;
PARRINELLO, M .
PHYSICAL REVIEW LETTERS, 1985, 55 (22) :2471-2474
[4]  
HEDIN L, 1971, J PHYS C SOLID STATE, V4, P3107
[5]  
IWAI S, 2000, INT WORKSH NITR SEM
[6]  
Katayama-Yoshida H, 1999, INST PHYS CONF SER, P747
[7]  
Katayama-Yoshida H, 1998, PHYS STATUS SOLIDI B, V210, P429, DOI 10.1002/(SICI)1521-3951(199812)210:2<429::AID-PSSB429>3.0.CO
[8]  
2-H
[9]  
KatayamaYoshida H, 1997, PHYS STATUS SOLIDI B, V202, P763, DOI 10.1002/1521-3951(199708)202:2<763::AID-PSSB763>3.0.CO
[10]  
2-C