TY - JOUR
T1 - Hybridization-gap formation and superconductivity in the pressure-induced semimetallic phase of the excitonic insulator Ta2NiSe5
AU - Matsubayashi, Kazuyuki
AU - Okamura, Hidekazu
AU - Mizokawa, Takashi
AU - Katayama, Naoyuki
AU - Nakano, Akitoshi
AU - Sawa, Hiroshi
AU - Kaneko, Tatsuya
AU - Toriyama, Tatsuya
AU - Konishi, Takehisa
AU - Ohta, Yukinori
AU - Arima, Hiroto
AU - Yamanaka, Rina
AU - Hisada, Akihiko
AU - Okada, Taku
AU - Ikemoto, Yuka
AU - Moriwaki, Taro
AU - Munakata, Koji
AU - Nakao, Akiko
AU - Nohara, Minoru
AU - Lu, Yangfan
AU - Takagi, Hidenori
AU - Uwatoko, Yoshiya
N1 - Funding Information:
Acknowledgment We thank K. Okazaki, Y. Fuseya, H. Matsuura, K. Miyake, M. Ogata, H. Fukuyama, A. Yaresko, and A. Rost for fruitful discussions, and K. Kitagawa for experimental support and discussions. This work was partly supported by the Futaba Electronics Memorial Foundation, Japan Society for the Promotion of Science (JSPS) KAKENHI (Nos. 26400349, 15H05852, 15H03681, 17H01140, 17K05530, 18H04312, 18H01172, 19H00648, and 20H01849) and Alexander von Humboldt foundation. T.K. and T.T. acknowledge support from the JSPS Research Fellowship for Young Scientists. Experiments at SPring-8 were performed under the approval by JASRI (2013A1085, 2014B1749, 2014B1751, 2015B1698, 2015A1528, 2016A3782, 2016A1166). A part of this work were performed under the Shared Use Program of the QST Facilities (proposal No. 2016A-E17) supported by the QST Advanced Characterization Nanotechnology Platform of the Ministry of Education, Culture, Sports, Science and Technology (MEXT), Japan (proposal No. A-16-QS-0009). The use of the facilities of Coordinated Center for UEC Research Facilities and Cryogenic Center at University of Electro-Communications is appreciated.
Funding Information:
We thank K. Okazaki, Y. Fuseya, H. Matsuura, K. Miyake, M. Ogata, H. Fukuyama, A. Yaresko, and A. Rost for fruitful discussions, and K. Kitagawa for experimental support and discussions. This work was partly supported by the Futaba Electronics Memorial Foundation, Japan Society for the Promotion of Science (JSPS) KAKENHI (Nos. 26400349, 15H05852, 15H03681, 17H01140, 17K05530, 18H04312, 18H01172, 19H00648, and 20H01849) and Alexander von Humboldt foundation. T.K. and T.T. acknowledge support from the JSPS Research Fellowship for Young Scientists. Experiments at SPring-8 were performed under the approval by JASRI (2013A1085, 2014B1749, 2014B1751, 2015B1698, 2015A1528, 2016A3782, 2016A1166). A part of this work were performed under the Shared Use Program of the QST Facilities (proposal No. 2016A-E17) supported by the QST Advanced Characterization Nanotechnology Platform of the Ministry of Education, Culture, Sports, Science and Technology (MEXT), Japan (proposal No. A-16-QS-0009). The use of the facilities of Coordinated Center for UEC Research Facilities and Cryogenic Center at University of Electro-Communications is appreciated.
Publisher Copyright:
© 2021 The Physical Society of Japan.
PY - 2021/7/1
Y1 - 2021/7/1
N2 - The excitonic insulator Ta2NiSe5 experiences a first-order structural transition under pressure from rippled to flat layer-structure at Ps ~ 3 GPa, which drives the system from an almost zero-gap semiconductor to a semimetal. The pressure-induced semimetal, with lowering temperature, experiences a transition to another semimetal with a partial-gap of ~0.1-0.2 eV, accompanied with a monoclinic distortion analogous to that occurs at the excitonic transition below Ps. We argue that the partial-gap originates primarily from a symmetry-allowed hybridization of Ta-conduction and Nivalence bands due to the lattice distortion, indicative of the importance of electron-lattice coupling. The transition is suppressed with increasing pressure to Pc ~ 8 GPa. Superconductivity with a maximum Tsc ~ 1.2K emerges around Pc, likely mediated by strongly electron-coupled soft phonons. The electron-lattice coupling is as important ingredient as the excitonic instability in Ta2NiSe5.
AB - The excitonic insulator Ta2NiSe5 experiences a first-order structural transition under pressure from rippled to flat layer-structure at Ps ~ 3 GPa, which drives the system from an almost zero-gap semiconductor to a semimetal. The pressure-induced semimetal, with lowering temperature, experiences a transition to another semimetal with a partial-gap of ~0.1-0.2 eV, accompanied with a monoclinic distortion analogous to that occurs at the excitonic transition below Ps. We argue that the partial-gap originates primarily from a symmetry-allowed hybridization of Ta-conduction and Nivalence bands due to the lattice distortion, indicative of the importance of electron-lattice coupling. The transition is suppressed with increasing pressure to Pc ~ 8 GPa. Superconductivity with a maximum Tsc ~ 1.2K emerges around Pc, likely mediated by strongly electron-coupled soft phonons. The electron-lattice coupling is as important ingredient as the excitonic instability in Ta2NiSe5.
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U2 - 10.7566/JPSJ.90.074706
DO - 10.7566/JPSJ.90.074706
M3 - Article
AN - SCOPUS:85107996488
SN - 0031-9015
VL - 90
JO - journal of the physical society of japan
JF - journal of the physical society of japan
IS - 7
M1 - 074706
ER -