论文标题
$ s $ - 非中心对称W $ _3 $ al $ _2 $ C超导的超导率:NMR研究
$s$-wave superconductivity in the noncentrosymmetric W$_3$Al$_2$C superconductor: An NMR study
论文作者
论文摘要
我们报告了一项对非中心对称超导体W $ _3 $ al $ _2 $ C(带有$ T_C $ = 7.6 K)的微观研究,主要是通过$^{27} $ al-和$ al-和$^{13} $ C {13} $ C核磁共振(NMR)。由于在这种材料中,费米水平的状态密度主要由钨的5 $ d $轨道构成,因此我们预计旋转轨道耦合(SOC)效应很大。 w $ _3 $ al $ _2 $ c的普通状态电子特性类似于标准金属的物质,但具有Korringa产品$ 1/(T_ {1} T)$明显小于金属AL的产品,这反映了$ S $ -Electrons扮演的边际作用。在超导状态下,我们观察到骑士移位的减少和NMR松弛率的指数降低$ 1/t_1 $,典型的$ s $ - 波超导率。在$^{13} $ c nmr放松率中,观察到$^{13} $ t_c $低于$ t_c $的小而独特的连贯峰进一步支持了这一点,这与从$ t_c $低于$ t_c $的电子特定热数据中推断出的完全相处的超导态。将上述功能与同一家庭成员的功能进行了比较,尤其是Mo $ _3 $ al $ _2 $ C,通常声称表现出非常规超导性。我们讨论为什么尽管有增强的SOC,但W $ _3 $ al $ _2 $ C并未在其超导状态下显示旋转三曲线特征,并考虑了我们对非中心对称超导体的结果的更大后果。
We report on a microscopic study of the noncentrosymmetric superconductor W$_3$Al$_2$C (with $T_c$ = 7.6 K), mostly by means of $^{27}$Al- and $^{13}$C nuclear magnetic resonance (NMR). Since in this material the density of states at the Fermi level is dominated by the tungsten's 5$d$ orbitals, we expect a sizeable spin-orbit coupling (SOC) effect. The normal-state electronic properties of W$_3$Al$_2$C resemble those of a standard metal, but with a Korringa product $1/(T_{1}T)$ significantly smaller than that of metallic Al, reflecting the marginal role played by $s$-electrons. In the superconducting state, we observe a reduction of the Knight shift and an exponential decrease of the NMR relaxation rate $1/T_1$, typical of $s$-wave superconductivity. This is further supported by the observation of a small but distinct coherence peak just below $T_c$ in the $^{13}$C NMR relaxation-rate, in agreement with the fully-gapped superconducting state inferred from the electronic specific-heat data well below $T_c$. The above features are compared to those of members of the same family, in particular, Mo$_3$Al$_2$C, often claimed to exhibit unconventional superconductivity. We discuss why, despite the enhanced SOC, W$_3$Al$_2$C does not show spin-triplet features in its superconducting state and consider the broader consequences of our results for noncentrosymmetric superconductors in general.