TY - JOUR
T1 - Combined optical, surface and nuclear microscopic assessment of porous silicon formed in HF-acetonitrile
AU - Feng, Z. C.
AU - Chen, Z.
AU - Padmanabhan, K. R.
AU - Li, K.
AU - Wee, A. T.S.
AU - Lin, J.
AU - Tan, K. L.
AU - Yue, K. T.
AU - Bhat, A.
AU - Rohatgi, A.
N1 - Funding Information:
We acknowledge the help and support from Drs. Z. Chen, A. Rohatgi, A. T. S. Wee, J. Lin, K. T. Yu and S. Perkowitz. The work at National Taiwan University was supported by funds from National Science Council of Republic of China, NSC 93-2218-E-002-011 and 93-2215-E-002-035.
PY - 1995
Y1 - 1995
N2 - A new type of HF solution, HF-acetonitrile (MeCN), has been employed to produce 10-30 μm thick porous silicon (P-Si) layers by photoelectrochemical etching of different types of Si wafers, Si(100), Si(111) and polycrystalline Si, with different resistivities. A combined optical, surface and nuclear microscopic assessment of these P-Si layers was performed using photoluminescence (PL), Raman scattering, X-ray photoelectron spectroscopy (XPS) and Rutherford backscattering spectroscopy (RBS). The PL emission intensities, Raman line shapes and structural features are strongly dependent on the properties of the substrates such as the crystallinity and resistivity of the Si wafers used for forming P-Si. With increasing resisitivity of the Si(100) wafers, the resulting P-Si layers show a slight blue-shift of their visible light emission peak energy, an up-shift of the peak position and a narrowing of the band width of the dominant Raman band, and a decrease in the amount of residual elemental Si on the surface. Those Si(111) wafers, etched in HF-MeCN, showed no porous structures and no visible light emission.
AB - A new type of HF solution, HF-acetonitrile (MeCN), has been employed to produce 10-30 μm thick porous silicon (P-Si) layers by photoelectrochemical etching of different types of Si wafers, Si(100), Si(111) and polycrystalline Si, with different resistivities. A combined optical, surface and nuclear microscopic assessment of these P-Si layers was performed using photoluminescence (PL), Raman scattering, X-ray photoelectron spectroscopy (XPS) and Rutherford backscattering spectroscopy (RBS). The PL emission intensities, Raman line shapes and structural features are strongly dependent on the properties of the substrates such as the crystallinity and resistivity of the Si wafers used for forming P-Si. With increasing resisitivity of the Si(100) wafers, the resulting P-Si layers show a slight blue-shift of their visible light emission peak energy, an up-shift of the peak position and a narrowing of the band width of the dominant Raman band, and a decrease in the amount of residual elemental Si on the surface. Those Si(111) wafers, etched in HF-MeCN, showed no porous structures and no visible light emission.
UR - http://www.scopus.com/inward/record.url?scp=0029229241&partnerID=8YFLogxK
M3 - Conference article
AN - SCOPUS:0029229241
SN - 0272-9172
VL - 358
SP - 345
EP - 350
JO - Materials Research Society Symposium - Proceedings
JF - Materials Research Society Symposium - Proceedings
T2 - Proceedings of the 1994 MRS Fall Meeting
Y2 - 28 November 1994 through 30 November 1994
ER -