TY - JOUR
T1 - Si atomic layer-by-layer epitaxial growth process using alternate exposure of Si(1 0 0) to SiH 4 and to Ar plasma
AU - Sakuraba, Masao
AU - Muto, Daisuke
AU - Seino, Takuya
AU - Murota, Junichi
N1 - Funding Information:
This study was partially supported by the Public Participation Program for the Promotion of Info. Communications Technology R&D from the Telecommunications Advancement Organization of Japan, and a Grant-in-Aid for Priority Area Research B (#11232201) and a Grant-in-Aid for Scientific Research B (#12450001) from the Ministry of Education, Science, Sports and Culture of Japan.
PY - 2003/5/15
Y1 - 2003/5/15
N2 - Si atomic layer-by-layer epitaxial growth without substrate heating has been investigated using alternate exposure of Si(100) to SiH 4 and to Ar plasma. With an Ar plasma generated by electron cyclotron resonance (ECR) at the Ar pressure of 2.1Pa (the measured peak energy and the incident density of the Ar ion are about 3 eV and 3 × 10 15 cm -2 s -1 , respectively), the average deposited Si thickness per cycle increases and saturates with exposure times to SiH 4 and to Ar plasma and also with the SiH 4 partial pressure. The thickness becomes smaller for the longer interruption of SiH 4 introduction until the Ar plasma exposure. In the Si atomic layer-by-layer epitaxial growth processes, their characteristics are qualitatively described in a modified Langmuir-type equation, assuming that the SiH 4 coverage is determined by the equilibrium of adsorption/desorption processes of a SiH 4 molecule on a single site, and the site density is the same as the surface atom density of Si(1 0 0).
AB - Si atomic layer-by-layer epitaxial growth without substrate heating has been investigated using alternate exposure of Si(100) to SiH 4 and to Ar plasma. With an Ar plasma generated by electron cyclotron resonance (ECR) at the Ar pressure of 2.1Pa (the measured peak energy and the incident density of the Ar ion are about 3 eV and 3 × 10 15 cm -2 s -1 , respectively), the average deposited Si thickness per cycle increases and saturates with exposure times to SiH 4 and to Ar plasma and also with the SiH 4 partial pressure. The thickness becomes smaller for the longer interruption of SiH 4 introduction until the Ar plasma exposure. In the Si atomic layer-by-layer epitaxial growth processes, their characteristics are qualitatively described in a modified Langmuir-type equation, assuming that the SiH 4 coverage is determined by the equilibrium of adsorption/desorption processes of a SiH 4 molecule on a single site, and the site density is the same as the surface atom density of Si(1 0 0).
KW - Ar plasma
KW - Chemical vapor deposition
KW - Langmuir type adsorption
KW - Si epitaxial growth
KW - SiH
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U2 - 10.1016/S0169-4332(03)00072-2
DO - 10.1016/S0169-4332(03)00072-2
M3 - Article
AN - SCOPUS:0037904205
SN - 0169-4332
VL - 212-213
SP - 197
EP - 200
JO - Applied Surface Science
JF - Applied Surface Science
IS - SPEC.
ER -