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Electronic state of superconductivity in line nodal material CaSb2 under pressure up to 4.2 GPa

Shumpei Oguchi, Kenji Ishida, Atsutoshi Ikeda, Yoshiteru Maeno, Shunsaku Kitagawa

Abstract

We report the results of resistance measurements under pressure up to $4.2\,\mathrm{GPa}$ on single-crystalline $\mathrm{CaSb}_2$ , which shows the maximum of superconducting transition temperature $T_\mathrm{c}$ at $3.1\,\mathrm{GPa}$. At room temperature, $R(P)$ shows a subtle anomaly at $3.1\,\mathrm{GPa}$. However, Bloch-Grüneisen analysis of $R(T)$ indicates that the electronic state does not change significantly across $3.1\,\mathrm{GPa}$.

Electronic state of superconductivity in line nodal material CaSb2 under pressure up to 4.2 GPa

Abstract

We report the results of resistance measurements under pressure up to on single-crystalline , which shows the maximum of superconducting transition temperature at . At room temperature, shows a subtle anomaly at . However, Bloch-Grüneisen analysis of indicates that the electronic state does not change significantly across .

Paper Structure

This paper contains 1 section, 2 equations, 2 figures.

Figures (2)

  • Figure 1: (Color online) Temperature dependence of resistance under various pressures for (a) the sample1 and (b) the sample2. The arrows in the insets represent $T_{\mathrm{c}}$ determined from the onset of superconductivity. (c) Pressure dependence of $T_{\mathrm{c}}$ of $\mathrm{CaSb}_2$. The dashed lines are guides to the eye taken from ref. kitagawa2021. (d) Pressure dependence of the resistance normalized at ambient pressure.
  • Figure 2: (Color online) (a) Temperature dependence of resistance of the sample2 at $3.0 \,\mathrm{GPa}$. Solid line is experimental data, dashed line is fitting line with eq.(3) using the normal-state data up to $100 \,\mathrm{K}$. (b)(c) Pressure dependence of the fitting parameters, $A$, $\theta_R$. Closed symbols mean that fitting range is up to $50\,\mathrm{K}$. Open symbols mean up to $100\,\mathrm{K}$.