April 22 - 26, 2024
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QT04.07.01

Exploration of Superconductivity in Layered Perovskite Nickelate La4Ni3O10 under High Pressure

When and Where

Apr 25, 2024
10:00am - 10:30am
Room 445, Level 4, Summit

Presenter(s)

Co-Author(s)

Yoshihiko Takano1,2

National Institute for Materials Science1,University of Tsukuba2

Abstract

Yoshihiko Takano1,2

National Institute for Materials Science1,University of Tsukuba2
Recent discovery of superconductivity in layered perovskite nickelate La<sub>3</sub>Ni<sub>2</sub>O<sub>7</sub> (Tc~80K) attract much attention due to its high superconducting transition temperature (Tc) and similarity of crystal structure to high-Tc cuprate [1]. And its mechanism of superconductivity is expected to be unconventional [2]. La<sub>3</sub>Ni<sub>2</sub>O<sub>7</sub> corresponds to the n = 2 case of the Ruddlesden-Popper phase represented by the general formula of La<sub>n+1</sub>Ni<sub>n</sub>O<sub>3n+1</sub>, and it has two layers of NiO<sub>2</sub> plane. In general, Ruddlesden-Popper phase has two-dimensional crystal and electric structure which is suitable for appearance of superconductivity for instance KCa<sub>2</sub>Nb<sub>3</sub>O<sub>10</sub> [3]. Particularly, La<sub>4</sub>Ni<sub>3</sub>O<sub>10</sub>, is corresponding to n = 3 case of the Ruddlesden-Popper phase having three layers of NiO<sub>2</sub> plane. Due to the similarity between these materials, we expect the possibility of superconductivity in La<sub>4</sub>Ni<sub>3</sub>O<sub>10</sub> under high pressure [4].<br/>We synthesized polycrystalline samples, La<sub>3</sub>Ni<sub>2</sub>O<sub>7</sub> and La<sub>4</sub>Ni<sub>3</sub>O<sub>10</sub>, via solid-phase reaction and Hot Isostatic Pressing process from La<sub>2</sub>O<sub>3 </sub>and NiO [4]. Samples are characterized by powder X-ray diffraction and thermogravimetry. High pressure was generated with Diamond Anvil Cell with boron-doped diamond electrodes designed for four-terminal resistance measurement [5]. Cubic boron nitride powder was used as a pressure-transmitting medium.<br/>La<sub>4</sub>Ni<sub>3</sub>O<sub>10</sub> displays metallic behavior across all measured pressures, with a slight upturn observed at temperatures below approximately 100 K. At 32.8 GPa, a drop in resistance suddenly appears below 5 K. With increasing the pressure beyond 46.2 GPa, the drop of resistance becomes significant. And the temperature where the resistance begins to drop elevated up to 23K at 79.2 GPa. Magnetic field dependence of resistance was measured at 69.4 GPa. As the magnetic field increases, the drop of resistance becomes smaller. Therefore, the drop in resistance is most likely to be the result of a superconducting transition of La<sub>4</sub>Ni<sub>3</sub>O<sub>10</sub> [4].<br/><br/>References:<br/>[1] H. Sun et al., Nature 621, 493 (2023).<br/>[2] M. Nakata et al., Phys. Rev. B 95, 214509 (2017).<br/>[3] Y. Takano et al., Solid State Commun., 103, 215 (1997).<br/>[4] H. Sakakibara et al., arXiv: 2309.09462.<br/>[5] R. Matsumoto et al., Rev. Sci. Instrum. 87, 076103 (2016).

Keywords

crystal growth | electrical properties | metal-insulator transition

Symposium Organizers

Liangzi Deng, University of Houston
Qiang Li, Stony Brook University/Brookhaven National Laboratory
Toshinori Ozaki, Kwansei Gakun University
Ruidan Zhong, Shanghai Jiao Tong University

Symposium Support

Gold
Faraday Factory Japan LLC

Session Chairs

Michael Osofsky
Yoshihiko Takano

In this Session