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Anisotropy Reversal of the Upper Critical Field at Low Temperatures and Spin-Locked Superconductivity in K2Cr3As3

Abstract

We report the first measurements of the anisotropic upper critical field Hc2(T)H_{c2}(T) for K2_{2}Cr3_{3}As3_{3} single crystals up to 60 T and T>0.6T > 0.6 K. Our results show that the upper critical field parallel to the Cr chains, Hc2(T)H_{c2}^\parallel (T), exhibits a paramagnetically-limited behavior, whereas the shape of the Hc2(T)H_{c2}^\perp (T) curve (perpendicular to the Cr chains) has no evidence of paramagnetic effects. As a result, the curves Hc2(T)H_{c2}^\perp (T) and Hc2(T)H_{c2}^\parallel(T) cross at T4T\approx 4 K, so that the anisotropy parameter γH(T)=Hc2/Hc2(T)\gamma_H(T)=H_{c2}^\perp/H_{c2}^\parallel (T) increases from γH(Tc)0.35\gamma_H(T_c)\approx 0.35 near TcT_c to γH(0)1.7\gamma_H(0)\approx 1.7 at 0.6 K. This behavior of Hc2(T)H_{c2}^\|(T) is inconsistent with triplet superconductivity but suggests a form of singlet superconductivity with the electron spins locked onto the direction of Cr chains

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