论文标题

在压力下,较重的弗里米式超导体UTE2中的上临界场各向异性

Anisotropy of the Upper Critical Field in the Heavy-Fermion Superconductor UTe2 under Pressure

论文作者

Knebel, Georg, Kimata, Motoi, Vališka, Michal, Honda, Fuminori, Li, Dexin, Braithwaite, Daniel, Lapertot, Gérard, Knafo, William, Pourret, Alexandre, Sato, Yoshiki J., Shimizu, Yusei, Kihara, Takumi, Brison, Jean-Pascal, Flouquet, Jacques, Aoki, Dai

论文摘要

我们研究了超导的上临界场的各向异性$ h _ {\ rm c2} $在静水压力下通过磁层测量测量在静水压力下的重型纤维超导体UTE $ _2 $。与以前的实验一致,我们确认超导性在临界压力附近消失$ p _ {\ rm c} \大约1.5 $ 〜GPA,并且出现了磁性有序状态。 $ h \ parallel A $在低温下的不寻常$ h _ {\ rm c2}(t)$表明,在压力下出现的多个超导阶段的$ h _ {\ rm c2} $完全不同。对于沿硬磁化$ b $ axis $ h _ {\ rm c2}(0)$粘贴到元磁过渡$ h _ {\ rm m} $的字段,该$被压制在$ p _ {\ rm c} $上。压力下的$ h _ {\ rm m} $的抑制遵循温度的降低$t_χ^{\ rm max} $,最大程度地沿着$ b $。由于$ t _ {\ rm sc} $的增加,在压力下迅速抑制了$ h _ {\ rm c2} $在$ h \ parallel b $以上的环境压力下的强大加固,并且$ h _ {\ rm mm} $的下降。 $ h _ {\ rm c2}(0)$的各向异性层次结构的变化在接近$ p _ {\ rm c} $时指出,$ c $ axis成为硬磁化轴。

We studied the anisotropy of the superconducting upper critical field $H_{\rm c2}$ in the heavy-fermion superconductor UTe$_2$ under hydrostatic pressure by magnetoresistivity measurements. In agreement with previous experiments we confirm that superconductivity disappears near a critical pressure $p_{\rm c} \approx 1.5$~GPa, and a magnetically ordered state appears. The unusual $H_{\rm c2}(T)$ at low temperatures for $H \parallel a$ suggests that the multiple superconducting phases which appear under pressure have quite different $H_{\rm c2}$. For a field applied along the hard magnetization $b$ axis $H_{\rm c2} (0)$ is glued to the metamagnetic transition $H_{\rm m}$ which is suppressed near $p_{\rm c}$. The suppression of $H_{\rm m}$ with pressure follows the decrease of temperature $T_χ^{\rm max}$, at the maximum in the susceptibility along $b$. The strong reinforcement of $H_{\rm c2}$ at ambient pressure for $H \parallel b$ above 16~T is rapidly suppressed under pressure due to the increase of $T_{\rm sc}$ and the decrease of $H_{\rm m}$. The change in the hierarchy of the anisotropy of $H_{\rm c2}(0)$ on approaching $p_{\rm c}$ points out that the $c$ axis becomes the hard magnetization axis.

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