TY - JOUR
T1 - Impact of Co or Cu Substitution for Ni on the Electronic Structure of Ta2NiSe5Studied by Band Structure Calculations
AU - Takahashi, Yu
AU - Mizokawa, Takashi
N1 - Funding Information:
Acknowledgements This work was partially supported by Grants-in-Aid from the Japan Society of the Promotion of Science (JSPS) (No. JP19H00659).
Publisher Copyright:
© 2022 The Physical Society of Japan.
PY - 2022/7
Y1 - 2022/7
N2 - We have investigated the electronic structure of Ta2Ni1-xCoxSe5 and Ta2Ni1-xCuxSe5 by means of band structure calculations. Ta2NiSe5 is one of the excitonic insulator candidates, and its electronic properties can be controlled by chemical substitution for Ni. In the Co doped systems with x ≤ 0.125, since a narrow Co 3d band is formed around the Fermi level, energy shift of the Ta 5d conduction and Ni 3d valence bands by the Co doping is considerably small. This is consistent with the photoemission result reported by Mitsuoka et al. [J. Phys. Soc. Jpn. 89, 124703 (2020)]. For x ≥ 0.25, the Co 3d band becomes wider, and the valence and conduction bands move to the higher energy side with increasing x. In Ta2CoSe5, Ta valence and Co valence are close to +5 (d0) and 0 (d9) respectively. In the Cu doped systems, the Cu 3d band is located well below the Fermi level and is almost fully occupied by electrons. The Cu substitution partially suppresses the Ni-Ta hybridization and causes band shift to the lower energy side by electron doping to the Ta 5d band. In Ta2CuSe5, Ta valence and Cu valence are close to +4.5 (d0.5) and +1 (d10) respectively.
AB - We have investigated the electronic structure of Ta2Ni1-xCoxSe5 and Ta2Ni1-xCuxSe5 by means of band structure calculations. Ta2NiSe5 is one of the excitonic insulator candidates, and its electronic properties can be controlled by chemical substitution for Ni. In the Co doped systems with x ≤ 0.125, since a narrow Co 3d band is formed around the Fermi level, energy shift of the Ta 5d conduction and Ni 3d valence bands by the Co doping is considerably small. This is consistent with the photoemission result reported by Mitsuoka et al. [J. Phys. Soc. Jpn. 89, 124703 (2020)]. For x ≥ 0.25, the Co 3d band becomes wider, and the valence and conduction bands move to the higher energy side with increasing x. In Ta2CoSe5, Ta valence and Co valence are close to +5 (d0) and 0 (d9) respectively. In the Cu doped systems, the Cu 3d band is located well below the Fermi level and is almost fully occupied by electrons. The Cu substitution partially suppresses the Ni-Ta hybridization and causes band shift to the lower energy side by electron doping to the Ta 5d band. In Ta2CuSe5, Ta valence and Cu valence are close to +4.5 (d0.5) and +1 (d10) respectively.
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U2 - 10.7566/JPSJ.91.074714
DO - 10.7566/JPSJ.91.074714
M3 - Article
AN - SCOPUS:85135275516
SN - 0031-9015
VL - 91
JO - journal of the physical society of japan
JF - journal of the physical society of japan
IS - 7
M1 - 074714
ER -