TY - JOUR
T1 - Pressure Induced Spectral Redistribution due to Te2 Dimer Breaking in AuTe2
AU - Ootsuki, Daiki
AU - Okamura, Hidekazu
AU - Mitsumoto, Shogo
AU - Ikemoto, Yuka
AU - Moriwaki, Taro
AU - Arita, Masashi
AU - Yoshida, Teppei
AU - Kudo, Kazutaka
AU - Ishii, Hiroyuki
AU - Nohara, Minoru
AU - Mizokawa, Takashi
N1 - Funding Information:
The authors thank Dr. Naoki Noguchi for technical assistance. The synchrotron radiation experiments were performed with the approvals of SPring-8 (Proposal Nos. 2015A1798 and 2016B1687) and HiSOR (Proposal No. 15-A-5). This research is supported by Japan Society for the Promotion of Science (JSPS) Grants-in-Aid for Scientific Research (KAKENHI Nos. JP19K03748, JP19H05823, and JP21K13882) and the Chubei Itoh Foundation.
Funding Information:
Acknowledgment The authors thank Dr. Naoki Noguchi for technical assistance. The synchrotron radiation experiments were performed with the approvals of SPring-8 (Proposal Nos. 2015A1798 and 2016B1687) and HiSOR (Proposal No. 15-A-5). This research is supported by Japan Society for the Promotion of Science (JSPS) Grants-in-Aid for Scientific Research (KAKENHI Nos. JP19K03748, JP19H05823, and JP21K13882) and the Chubei Itoh Foundation.
Publisher Copyright:
©2021 The Physical Society of Japan.
PY - 2021/11/15
Y1 - 2021/11/15
N2 - We report the electronic structure of a natural mineral calaverite AuTe2 under high pressure by means of the infrared spectroscopy. The optical conductivity at ambient pressure shows a Drude response and a hump structure around 0.2 eV. These characteristic results are more prominent in going from high temperature to low temperature. The Drude response increases with pressure, which corresponds to the reduction of the electrical resistivity. Meanwhile, the hump structure is suppressed and merged into the Drude response with increasing pressure. Further applying pressure up to 3 GPa, the hump structure almost disappears. We have fitted the optical conductivity by using the Drude–Lorentz model and obtained the plasma frequency ωp and the scattering rate γ. The squared plasma frequency !2p increases and the scattering rate γ decreases with pressure. Our results suggest that the suppression of the electrical resistivity under pressure is mainly due to the increase of the carrier density n and the reduction of the scattering rate γ. By comparing the optical conductivity with the band structure calculation and the photoemission spectroscopy, we discuss the low-energy excitation corresponding to the hump structure and the variation of the Drude component in the optical conductivity.
AB - We report the electronic structure of a natural mineral calaverite AuTe2 under high pressure by means of the infrared spectroscopy. The optical conductivity at ambient pressure shows a Drude response and a hump structure around 0.2 eV. These characteristic results are more prominent in going from high temperature to low temperature. The Drude response increases with pressure, which corresponds to the reduction of the electrical resistivity. Meanwhile, the hump structure is suppressed and merged into the Drude response with increasing pressure. Further applying pressure up to 3 GPa, the hump structure almost disappears. We have fitted the optical conductivity by using the Drude–Lorentz model and obtained the plasma frequency ωp and the scattering rate γ. The squared plasma frequency !2p increases and the scattering rate γ decreases with pressure. Our results suggest that the suppression of the electrical resistivity under pressure is mainly due to the increase of the carrier density n and the reduction of the scattering rate γ. By comparing the optical conductivity with the band structure calculation and the photoemission spectroscopy, we discuss the low-energy excitation corresponding to the hump structure and the variation of the Drude component in the optical conductivity.
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U2 - 10.7566/JPSJ.90.114705
DO - 10.7566/JPSJ.90.114705
M3 - Article
AN - SCOPUS:85149021842
SN - 0031-9015
VL - 90
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 11
M1 - 114705
ER -