TY - JOUR
T1 - Temperature Dependence of Desorption in HigMy Photo-Excited CdS
AU - Namiki, Akira
AU - Fukano, Hideki
AU - Kawai, Takaaki
AU - Yasuda, Yukio
AU - Nakamura, Tetsuro
PY - 1985
Y1 - 1985
N2 - Dependence of laser-induced desorption on both substrate temperature and emission angle have been studied in CdS by using the pulse mass counting method. The effective translational temperature (Ttrans) of particles ejected toward the angle of 0° from the surface normal is much higher than that toward 45°. The Ttrans of cach particlc, S, S2 and Cd, is different among them. Ttrans does not exhibit the surface temperature even when the time-of-flight spectra can be fitted with a Maxwellian velocity distribution. Arrhenius plots of desorption yields for the substrate temperature before laser irradiation show rather complicated features. Estimation of the temperature rise at surface by calculating the thermal diffusion equation gives the linear relationship in the Arrhenius plot. The enthalpy for desorption is estimated to be 0.44µ0.1 eV. This value is considerably smaller than that (2.2 eV) obtained in the free vacuum vaporization (ref. 13), suggesting the contribution of the electronic excitation effect.
AB - Dependence of laser-induced desorption on both substrate temperature and emission angle have been studied in CdS by using the pulse mass counting method. The effective translational temperature (Ttrans) of particles ejected toward the angle of 0° from the surface normal is much higher than that toward 45°. The Ttrans of cach particlc, S, S2 and Cd, is different among them. Ttrans does not exhibit the surface temperature even when the time-of-flight spectra can be fitted with a Maxwellian velocity distribution. Arrhenius plots of desorption yields for the substrate temperature before laser irradiation show rather complicated features. Estimation of the temperature rise at surface by calculating the thermal diffusion equation gives the linear relationship in the Arrhenius plot. The enthalpy for desorption is estimated to be 0.44µ0.1 eV. This value is considerably smaller than that (2.2 eV) obtained in the free vacuum vaporization (ref. 13), suggesting the contribution of the electronic excitation effect.
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U2 - 10.1143/JPSJ.54.3162
DO - 10.1143/JPSJ.54.3162
M3 - Article
AN - SCOPUS:0022112043
SN - 0031-9015
VL - 54
SP - 3162
EP - 3167
JO - journal of the physical society of japan
JF - journal of the physical society of japan
IS - 8
ER -