TY - JOUR
T1 - Real-time monitoring of surface passivation of crystalline silicon during growth of amorphous and epitaxial silicon layer
AU - Nunomura, Shota
AU - Sakata, Isao
AU - Sakakita, Hajime
AU - Koga, Kazunori
AU - Shiratani, Masaharu
N1 - Funding Information:
The authors are grateful to Dr. H. Umishio, Dr. T. Matsui, Dr. M. Lozac’h, Dr. K. Matsubara, Dr. T. Maeda, Dr. T. Shimizu, and Dr. H. Takashima (AIST) for fruitful discussions. This work was supported, in part, by JSPS KAKENHI (Grant Nos. 18K03603 and 20H00142) and the New Energy and Industrial Technology Development Organization (NEDO).
Publisher Copyright:
© 2020 Author(s).
PY - 2020/7/21
Y1 - 2020/7/21
N2 - Surface passivation of crystalline silicon (c-Si) is experimentally studied during the growth of a hydrogenated amorphous silicon (a-Si:H) and epitaxial silicon (epi-Si) passivation layer at a subnanometer to nanometer scale. The property of surface passivation is monitored in real time via in situ measurement of a photocurrent in c-Si under plasma-enhanced vapor deposition for the passivation layer growth. The measurement results suggest the following. Passivation is improved by the growth of an a-Si:H layer, where a large band offset is formed at the a-Si:H/c-Si interface, and the carrier recombination is suppressed. On the other hand, passivation is deteriorated with the growth of an ultrathin epi-Si layer (d ≲ 2.5 ± 1.0 nm) because the band offset is not formed at the interface, and plasma-induced defects are created in c-Si. However, passivation is improved with a thick epi-Si layer (d ≳ 2.5 ± 1.0 nm), where the band bending is formed near the epi-Si/c-Si interface, which partially suppresses the carrier recombination. The suppression of the plasma-induced defects as well as the formation of the band offset are important for surface passivation.
AB - Surface passivation of crystalline silicon (c-Si) is experimentally studied during the growth of a hydrogenated amorphous silicon (a-Si:H) and epitaxial silicon (epi-Si) passivation layer at a subnanometer to nanometer scale. The property of surface passivation is monitored in real time via in situ measurement of a photocurrent in c-Si under plasma-enhanced vapor deposition for the passivation layer growth. The measurement results suggest the following. Passivation is improved by the growth of an a-Si:H layer, where a large band offset is formed at the a-Si:H/c-Si interface, and the carrier recombination is suppressed. On the other hand, passivation is deteriorated with the growth of an ultrathin epi-Si layer (d ≲ 2.5 ± 1.0 nm) because the band offset is not formed at the interface, and plasma-induced defects are created in c-Si. However, passivation is improved with a thick epi-Si layer (d ≳ 2.5 ± 1.0 nm), where the band bending is formed near the epi-Si/c-Si interface, which partially suppresses the carrier recombination. The suppression of the plasma-induced defects as well as the formation of the band offset are important for surface passivation.
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U2 - 10.1063/5.0011563
DO - 10.1063/5.0011563
M3 - Article
AN - SCOPUS:85089484968
VL - 128
JO - Journal of Applied Physics
JF - Journal of Applied Physics
SN - 0021-8979
IS - 3
M1 - 033302
ER -