Joint Workshop LANL/NIMS Quantum and Functional Materials and MANA International Symposium 2024


Quantum Materials - 04

Title

Pressure-Induced Superconductivity in Trilayer Nickelate La4Ni3O10+δ

Author's photo

Authors

Hibiki Nagata1,2, Hiroya Sakurai1, Yuta Ueki1,2, Kazuki Yamane1,2,
Ryo Matsumoto1 Kensei Terashima1, Keisuke Hirose3, Hiroto Ohta3,
Masaki Kato3, and Yoshihiko Takano1,2

Affiliations

1.Frontier Superconducting Materials Group, MANA, NIMS
2.Graduate School of Pure and Applied Sciences, University of Tsukuba
3.Faculty of Science and Engineering, Doshisha University

URL

https://www.nims.go.jp/NFM/

Email

NAGATA.Hibiki@nims.go.jp

Abstract

Recently, La3Ni2O7 was reported to show superconductivity under pressure of 14 GPa, with transition temperature(Tc) of 80 K[1]. La3Ni2O7 is a bilayer Ruddlesden-Popper phase nickelate that has two layers of NiO2 plane in its unit cell, while there also exists trilayer family compound: La4Ni3O10. As there had been no studies yet that reports superconductivity in La4Ni3O10, we investigated the possibility of superconductivity in this compound under high pressure [2].
The polycrystalline La4Ni3O10+δ samples were synthesized via solid-state reaction and hot isostatic pressing process, and characterized by powder X-ray diffraction and thermogravimetric analysis to find it to be single phase La4Ni3O10.04 and La4Ni3O9.99. We used diamond anvil cell with boron-doped diamond electrodes designed for four-terminal resistance measurement under high pressure [3].
The temperature dependence of the resistance of La4Ni3O10.04 and La4Ni3O9.99 under various pressures are shown in Fig.1 [4]. In the case of La4Ni3O10.04, the resistance exhibits a slight suppression below 5 K at 20.2 GPa, with this suppression becoming more pronounced under higher pressures. The suppression is most likely attributable to the onset of superconductivity because it was suppressed by magnetic field. For La4Ni3O10.04, Tc rapidly increases with increasing pressure from 20.2 GPa, reaches at 36 K at 48.0 GPa, and then gradually decreases with further pressure increase. In contrast, for La4Ni3O9.99, superconductivity begins to appear at 32.8 GPa and Tc gradually increases with increasing pressure. Thus, Tc of La4Ni3O10+δ exhibits a strong dependence on oxygen-content within the pressure range of approximately 20 to 80 GPa.

Fig. 1. Temperature dependence of the resistance of La4Ni3O10.04 (a) and La4Ni3O9.99 (b) under various pressures. The dashed lines represent the linear temperature dependence just above Tc, and the arrows indicate Tc estimated[4]

Reference

  1. H. Sun, M. Huo, X. Hu, J. Li, Z. Liu, Y. Han, L. Tang, Z. Mao, P. Yang, B. Wang, J. Cheng, D.-X. Yao, G.-M. Zhang, and M. Wang, Nature621, 493, (2023). DOI 10.1038/s41586-023-06408-7
  2. H. Sakakibara, M. Ochi, H. Nagata, Y. Ueki, H. Sakurai, R. Matsumoto, K. Terashima, K. Hirose, H. Ohta, M. Kato, Y. Takano, and K. Kuroki, Phys. Rev. B 109, 144511, (2024). DOI 10.1103/PhysRevB.109.144511
  3. R. Matsumoto, Y. Sasama, M. Fujioka, T. Irifune, M. Tanaka, T. Yamaguchi, H. Takeya, and Y. Takano, Rev. Sci. Instrum. 87, 076103, (2016). DOI 10.1063/1.4959154
  4. H. Nagata, H. Sakurai, Y. Ueki, K. Yamane, R. Matsumoto, K. Terashima, K. Hirose, H. Ohta, M. Kato, and Y. Takano, J. Phys. Soc. Jpn. 93, 095003, (2024). DOI 10.7566/JPSJ.93.095003