TY - JOUR
T1 - Raman spectroscopic study on boron-doped silicon nanoparticles
AU - Momose, Miho
AU - Hirasaka, Masao
AU - Furukawa, Yukio
N1 - Copyright:
Copyright 2014 Elsevier B.V., All rights reserved.
PY - 2014/5
Y1 - 2014/5
N2 - Raman analyses were performed on thin films prepared from B-doped Si nanoparticles with an average diameter of 15 nm using the spin-coating method. The resulting spectrum exhibited a broad band with a peak near 520 cm -1. The band was decomposed into three bands corresponding to the crystalline, grain boundary (GB), and amorphous regions by the least-squares band-fitting method based on the three Voigt bands. The fractions of the crystalline, GB, and amorphous regions were 37%, 35%, and 28%, respectively. A spherical particle exhibited an ordered crystalline core surrounded by a disordered shell in a transmission electron microscope (TEM) image. The crystalline fraction of the 15-nm B-doped Si nanoparticle film was much lower than that of the 19-nm P-doped Si nanoparticle film. This result suggested that the B-doping mechanism was different from that of P-doping. The temperature of the sample was estimated from the ratio of the peak intensities of anti-Stokes to Stokes Raman bands (IAS/IS) observed near 520 cm -1. The temperature of the B-doped Si nanoparticle film upon irradiation at a power density of 4.6 kW/cm2 was 298 C, whereas the temperature of the P-doped Si nanoparticle film was 92 C. The B-doped Si nanoparticle films were capable of producing light-induced heat.
AB - Raman analyses were performed on thin films prepared from B-doped Si nanoparticles with an average diameter of 15 nm using the spin-coating method. The resulting spectrum exhibited a broad band with a peak near 520 cm -1. The band was decomposed into three bands corresponding to the crystalline, grain boundary (GB), and amorphous regions by the least-squares band-fitting method based on the three Voigt bands. The fractions of the crystalline, GB, and amorphous regions were 37%, 35%, and 28%, respectively. A spherical particle exhibited an ordered crystalline core surrounded by a disordered shell in a transmission electron microscope (TEM) image. The crystalline fraction of the 15-nm B-doped Si nanoparticle film was much lower than that of the 19-nm P-doped Si nanoparticle film. This result suggested that the B-doping mechanism was different from that of P-doping. The temperature of the sample was estimated from the ratio of the peak intensities of anti-Stokes to Stokes Raman bands (IAS/IS) observed near 520 cm -1. The temperature of the B-doped Si nanoparticle film upon irradiation at a power density of 4.6 kW/cm2 was 298 C, whereas the temperature of the P-doped Si nanoparticle film was 92 C. The B-doped Si nanoparticle films were capable of producing light-induced heat.
KW - B-doped Si
KW - Nanoparticle
KW - Raman
KW - Silicon
KW - Temperature
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U2 - 10.1016/j.vibspec.2014.02.014
DO - 10.1016/j.vibspec.2014.02.014
M3 - Article
AN - SCOPUS:84896464942
SN - 0924-2031
VL - 72
SP - 62
EP - 65
JO - Vibrational Spectroscopy
JF - Vibrational Spectroscopy
ER -