TY - JOUR
T1 - Hydrogen evolution during deposition of microcrystalline silicon by chemical transport
AU - Pham, N.
AU - Roca I Cabarrocas, P.
AU - Hadjadj, A.
AU - Beorchia, A.
AU - Kail, F.
AU - Chahed, L.
PY - 2008/1/1
Y1 - 2008/1/1
N2 - We exposed a freshly deposited boron-doped, hydrogenated amorphous silicon (a-Si:H) layer to hydrogen plasma under conditions of chemical transport. In situ spectroscopic ellipsometry measurements revealed that atomic hydrogen impinging on the film surface behaves differently before and after crystallization. First, the plasma exposure increases hydrogen solubility in the a-Si:H network leading to the formation of a hydrogen-rich subsurface layer. Then, once the crystallization process engages, the excess hydrogen starts to leave the sample. We have attributed this unusual evolution of the excess hydrogen to the grown hydrogenated microcrystalline (c-Si:H) layer, which gradually prevents the atomic hydrogen from the plasma reaching the c-Si:H/a-Si:H interface. Consequently, hydrogen solubility, initially increased by the hydrogen plasma, recovers the initial value of an untreated a-Si:H material. To support the theory that the outdiffusion is a consequence and not the cause of the c-Si:H layer growth, we solved the combined diffusion and trapping equations, which govern hydrogen diffusion into the sample, using appropriate approximations and a specific boundary condition explaining the lack of hydrogen injection during c-Si:H layer growth.
AB - We exposed a freshly deposited boron-doped, hydrogenated amorphous silicon (a-Si:H) layer to hydrogen plasma under conditions of chemical transport. In situ spectroscopic ellipsometry measurements revealed that atomic hydrogen impinging on the film surface behaves differently before and after crystallization. First, the plasma exposure increases hydrogen solubility in the a-Si:H network leading to the formation of a hydrogen-rich subsurface layer. Then, once the crystallization process engages, the excess hydrogen starts to leave the sample. We have attributed this unusual evolution of the excess hydrogen to the grown hydrogenated microcrystalline (c-Si:H) layer, which gradually prevents the atomic hydrogen from the plasma reaching the c-Si:H/a-Si:H interface. Consequently, hydrogen solubility, initially increased by the hydrogen plasma, recovers the initial value of an untreated a-Si:H material. To support the theory that the outdiffusion is a consequence and not the cause of the c-Si:H layer growth, we solved the combined diffusion and trapping equations, which govern hydrogen diffusion into the sample, using appropriate approximations and a specific boundary condition explaining the lack of hydrogen injection during c-Si:H layer growth.
U2 - 10.1080/14786430701823213
DO - 10.1080/14786430701823213
M3 - Article
AN - SCOPUS:39349083166
SN - 1478-6435
VL - 88
SP - 297
EP - 311
JO - Philosophical Magazine
JF - Philosophical Magazine
IS - 3
ER -