TY - JOUR
T1 - Native defects at the Si/SiO2 interface-amorphous silicon revisited
AU - Biegelsen, D. K.
AU - Johnson, N. M.
AU - Stutzmann, M.
AU - Poindexter, E. H.
AU - Caplan, P. J.
N1 - Funding Information:
We wish to thank M.D. Moyer for state of the art samplep reparation. We also thank K.L. Brower for sharingw ith us his results( ref. \[8\]b) efore publicationW. ork reportedh ere was supportedin part by the US Army ERADCOM.
PY - 1985/5
Y1 - 1985/5
N2 - We review here work which demonstrates that silicon dangling bonds, Si3, are the predominant, electrically active deep states associated with the clean crystalline silicon/amorphous SiO2 interface. Si3 exists in three charge states in the silicon band gap with E+,0 {reversed tilde equals} Ev + 0.3 eV and E0,- {reversed tilde equals} Ev + 0.9 eV, where E represents a demarcation level between charge states. We discuss the structural and electronic characteristics of Si3 at the Si/SiO2 interface, including degree of charge localization, effective correlation energies, role of hydrogen passivation, etc. We argue, from the strongly analogous behavior in amorphous silicon, that the electronic density of states in the gap is dominated by the characteristic effects of disorder in covalently bonded semiconductors. The states consist of two topologically distinct entities: distorted, fully-bonded network configurations giving rise to shallow silicon band tails, and three-fold coordinated, amphoteric silicon defects.
AB - We review here work which demonstrates that silicon dangling bonds, Si3, are the predominant, electrically active deep states associated with the clean crystalline silicon/amorphous SiO2 interface. Si3 exists in three charge states in the silicon band gap with E+,0 {reversed tilde equals} Ev + 0.3 eV and E0,- {reversed tilde equals} Ev + 0.9 eV, where E represents a demarcation level between charge states. We discuss the structural and electronic characteristics of Si3 at the Si/SiO2 interface, including degree of charge localization, effective correlation energies, role of hydrogen passivation, etc. We argue, from the strongly analogous behavior in amorphous silicon, that the electronic density of states in the gap is dominated by the characteristic effects of disorder in covalently bonded semiconductors. The states consist of two topologically distinct entities: distorted, fully-bonded network configurations giving rise to shallow silicon band tails, and three-fold coordinated, amphoteric silicon defects.
UR - http://www.scopus.com/inward/record.url?scp=0021420292&partnerID=8YFLogxK
U2 - 10.1016/0378-5963(85)90220-X
DO - 10.1016/0378-5963(85)90220-X
M3 - Article
AN - SCOPUS:0021420292
SN - 0378-5963
VL - 22-23
SP - 879
EP - 890
JO - Applications of Surface Science
JF - Applications of Surface Science
IS - PART 2
ER -