TY - JOUR
T1 - The optical properties of liquid chalcogens
AU - Ikemoto, Hiroyuki
AU - Yamamoto, Itsuro
AU - Endo, Hirohisa
PY - 1993/5/2
Y1 - 1993/5/2
N2 - The temperature and pressure variations of the optical reflectivity of liquid Te, Se, Se80Te20 and Se80S20 have been measured in the energy range of 0.5-5.4 eV. The optical conductivity, σ(ω), has been derived by using an oscillator fitting analysis. The σ(ω) curve of liquid Te, which has a stacked planar zigzag geometry, has a broad peak around 2.2 eV and a Drude term on the low-energy side. The peak can be mainly ascribed to the transition from the bonding σ band to the antibonding σ* band and from the filled σ* band to the unfilled σ* band. On the other hand, the σ(ω) curve of liquid Se at 500°C has a broad peak around 3.5 eV, maintaining a semiconducting character. The peak is assigned to the transition from the lone-pair band to the σ* band. With increasing temperature, the peak shifts to the lower energy side. The optical gap closes between 1100 and 1300°C and a Drude term appears. This implies that the structure of liquid Se changes from the spiral chain geometry to the geometry of the metallic liquid Te. The temperature of the semiconductor-metal transition is lowered by replacing Se with Te.
AB - The temperature and pressure variations of the optical reflectivity of liquid Te, Se, Se80Te20 and Se80S20 have been measured in the energy range of 0.5-5.4 eV. The optical conductivity, σ(ω), has been derived by using an oscillator fitting analysis. The σ(ω) curve of liquid Te, which has a stacked planar zigzag geometry, has a broad peak around 2.2 eV and a Drude term on the low-energy side. The peak can be mainly ascribed to the transition from the bonding σ band to the antibonding σ* band and from the filled σ* band to the unfilled σ* band. On the other hand, the σ(ω) curve of liquid Se at 500°C has a broad peak around 3.5 eV, maintaining a semiconducting character. The peak is assigned to the transition from the lone-pair band to the σ* band. With increasing temperature, the peak shifts to the lower energy side. The optical gap closes between 1100 and 1300°C and a Drude term appears. This implies that the structure of liquid Se changes from the spiral chain geometry to the geometry of the metallic liquid Te. The temperature of the semiconductor-metal transition is lowered by replacing Se with Te.
UR - http://www.scopus.com/inward/record.url?scp=0027905615&partnerID=8YFLogxK
U2 - 10.1016/0022-3093(93)90057-5
DO - 10.1016/0022-3093(93)90057-5
M3 - 学術論文
AN - SCOPUS:0027905615
SN - 0022-3093
VL - 156-158
SP - 732
EP - 735
JO - Journal of Non-Crystalline Solids
JF - Journal of Non-Crystalline Solids
IS - PART 2
ER -