TY - JOUR
T1 - A study of the electrical properties of HgS under high pressure
AU - Hao, Aimin
AU - Gao, Chunxiao
AU - Li, Ming
AU - He, Chunyuan
AU - Huang, Xiaowei
AU - Zhang, Dongmei
AU - Yu, Cuiling
AU - Liu, Hongwu
AU - Ma, Yanzhang
AU - Tian, Yongjun
AU - Zou, Guangtian
PY - 2007/10/24
Y1 - 2007/10/24
N2 - Using a microcircuit fabricated in a diamond anvil cell, we carried out in situ conductivity measurements on α-HgS and β-HgS under high pressure, and investigated the temperature dependence of the conductivity of the samples under several pressures. For α-HgS, the results show that the conductivity increases rapidly with increasing pressure from 8 to 20GPa. The energy gap was obtained by fitting linearly the plot of the logarithm of conductivity versus the reciprocal of temperature. At 29GPa, the sample becomes metallic, characterized by a negative temperature slope of conductivity and a zero energy gap. For β-HgS, a discontinuity of conductivity was observed at 5GPa, corresponding to a transition from the β phase to the α phase. From 5 to 20GPa, the conductivity rises rapidly with increasing pressure. At 27GPa, the sample becomes metallic. In comparison with HgSe and HgTe, we obtained experimentally the transition pressure of the two samples from the cinnabar structure to the rock-salt structure, respectively.
AB - Using a microcircuit fabricated in a diamond anvil cell, we carried out in situ conductivity measurements on α-HgS and β-HgS under high pressure, and investigated the temperature dependence of the conductivity of the samples under several pressures. For α-HgS, the results show that the conductivity increases rapidly with increasing pressure from 8 to 20GPa. The energy gap was obtained by fitting linearly the plot of the logarithm of conductivity versus the reciprocal of temperature. At 29GPa, the sample becomes metallic, characterized by a negative temperature slope of conductivity and a zero energy gap. For β-HgS, a discontinuity of conductivity was observed at 5GPa, corresponding to a transition from the β phase to the α phase. From 5 to 20GPa, the conductivity rises rapidly with increasing pressure. At 27GPa, the sample becomes metallic. In comparison with HgSe and HgTe, we obtained experimentally the transition pressure of the two samples from the cinnabar structure to the rock-salt structure, respectively.
UR - http://www.scopus.com/inward/record.url?scp=34648823457&partnerID=8YFLogxK
U2 - 10.1088/0953-8984/19/42/425222
DO - 10.1088/0953-8984/19/42/425222
M3 - Article
AN - SCOPUS:34648823457
SN - 0953-8984
VL - 19
JO - Journal of Physics Condensed Matter
JF - Journal of Physics Condensed Matter
IS - 42
M1 - 425222
ER -