# Pressure-induced superconductivity in layered pnictogen diselenide   NdO$_{0.8}$F$_{0.2}$Sb$_{1-x}$Bi$_x$Se$_2$ (x = 0.3 and 0.7)

**Authors:** Ryo Matsumoto, Yosuke Goto, Sayaka Yamamoto, Kenta Sudo, Hidetomo, Usui, Akira Miura, Chikako Moriyoshi, Yoshihiro Kuroiwa, Shintaro Adachi,, Tetsuo Irifune, Hiroyuki Takeya, Hiromi Tanaka, Kazuhiko Kuroki, Yoshikazu, Mizuguchi, and Yoshihiko Takano

arXiv: 1903.07791 · 2019-10-02

## TL;DR

This study demonstrates pressure-induced superconductivity in layered pnictogen diselenide NdO0.8F0.2Sb1-xBixSe2, revealing new superconducting phases in SbCh2-based compounds with detailed pressure and composition dependence.

## Contribution

First report of superconductivity in layered SbCh2-based compounds, showing pressure-induced superconductivity in NdO0.8F0.2Sb1-xBixSe2 with systematic analysis of Bi doping effects.

## Key findings

- Superconductivity observed at high pressures for x=0.3 and 0.7.
- Superconducting transition temperature (Tc) increases with pressure for x=0.3.
- Upper critical field (Hc2) evaluated to be ~10 T for x=0.7.

## Abstract

Polycrystalline samples of layered pnictogen diselenide NdO0.8F0.2Sb1-xBixSe2 (x = 0 to 0.8) were successfully synthesized by solid-state reactions. Electrical resistivity in the synthesized samples was systematically decreased with an increase in Bi content x. Crystal structure analysis using synchrotron X-ray diffraction suggests that insulator to metal transition upon Bi doping correlates with anomalous change in c-axis length and/or corrugation in conducting layer. The emergence of superconductivity under high pressure is demonstrated using diamond anvil cell (DAC) with boron-doped diamond electrodes, for x = 0.3 and 0.7 as the representative samples. For Sb-rich one (x = 0.3), we observed a superconducting transition with Tconset = 5.3 K at 50 GPa, which is the first-ever report of the superconductivity in layered SbCh2-based (Ch: chalcogen) compounds. The Tconset of x = 0.3 increased with increasing pressure and reached 7.9 K at 70.8 GPa, followed by the gradual decrease in Tc up to 90 GPa. For Bi-rich one (x = 0.7), a superconducting transition with Tconset = 5.9 K was observed at 43.5 GPa, which is the almost comparable to that of x = 0.3; besides, upper critical field (Hc2) is evaluated to be ~10 T for x = 0.7, which is higher than that of x = 0.3 (Hc2 = 6.7 T at 50 GPa).

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Source: https://tomesphere.com/paper/1903.07791