High-Magnetic Field Phases in U$_{1-x}$Th$_x$Te$_2$

TL;DR

This study explores the complex high-magnetic-field phases of UTe$_2$ and its Th-doped variants, revealing how doping affects the superconducting and magnetic phases, with implications for understanding unconventional superconductivity.

Contribution

It provides the first detailed phase diagram of U$_{1-x}$Th$_x$Te$_2$ under high magnetic fields, showing how Th doping suppresses certain superconducting phases and introduces disorder.

Findings

SC$_{ ext{LF}}$ phase persists with reduced $H_{c2}$ in Th-doped samples.

SC$_{ ext{HF}}$ phase is suppressed by Th doping.

SC$_{ ext{FP}}$ and FP phases are suppressed at higher Th concentrations.

Abstract

At temperatures much lower than its superconducting critical temperature $T_c$ of 2.1 K, the heavy fermion superconductor UTe$_2$ has a remarkable phase diagram of magnetic field $H$ vs. angles $\phi$ and $\theta$ at which $H$ is tilted away from the $b$-axis toward the $a$- and $c$-axes, respectively, in the orthorhombic unit cell. The phase diagram appears to contain three superconducting phases: (1) a low field superconducting phase SC$_{\mathrm{LF}}$ extending over all values of $\phi$ and $\theta$ with an upper critical field $H_{c2}$ with a maximum value of 15 T at $\phi = \theta = 0^\circ$; (2) a high field superconducting phase SC$_{\mathrm{HF}}$ located in a region between $\phi \approx 7^\circ$ and $\theta \approx 4^\circ$ in fields from $H_{c2\mathrm{LF}}$ of the SC$_{\mathrm{LF}}$ phase and the metamagnetic transition at $H_m$ at $\sim 35$ T marking the onset of the magnetic field polarized FP phase: and (3) a SC$_{\mathrm{FP}}$ superconducting phase that resides entirely within the FP phase in a pocket of superconductivity extending from $\theta \approx 20^\circ$ to $40^\circ$ in fields from $\sim 40$ T to above 60 T. In this work, we studied the $H$ vs $\theta$ phase diagram at a base temperature of $\sim 0.6$ K as a function of Th concentration $x$ in U$_{1-x}$Th$_x$Te$_2$ pseudobinary compounds for $0.5\% \lesssim x \lesssim 4.7\%$. We find that for all values of $x$ within this range, the SC$_{\mathrm{LF}}$ phase is retained with a reduced value of $H_{c2}$ of $\sim 10$ T at $\phi = \theta = 0^\circ$ for $x = 4.7\%$, while the SC$_{\mathrm{HF}}$ phase is suppressed. The SC$_{\mathrm{FP}}$ and FP phases are unaffected to values of $x = 2\%$ but are completely suppressed in the region $x = 2.5$ to $4.7\%$ where the residual resistance ratio RRR has decreased from $\sim 14$ at $x = 1.5\%$ to values of $\sim 3$, indicating a significant increase in disorder.