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arXiv 2203.09386cond-mat.mtrl-scicond-mat.supr-con
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kagome金属CsV$_3$Sb$_5$中在T$_{CDW}$以上和超导T$_c$以下的电荷密度波序与涨落

Charge density wave order and fluctuations above T$_{CDW}$ and below superconducting T$_c$ in the kagome metal CsV$_{3}$Sb$_{5}$

Q. Chen, D. Chen, W. Schnelle, C. Felser, B. D. Gaulin

AI总结:

本文通过300 K至约2 K的X射线散射研究CsV$_3$Sb$_5$,发现CDW涨落延伸至160 K,并证明CDW与超导在$T_c$以下共存。

摘要:

kagome金属家族\ch{AV3Sb5}(A = K、Rb、Cs)的相图同时具有超导性和电荷密度波(CDW)不稳定性,近来引起了极大关注。尽管如此,仍有重要问题存在。特别是,CDW态随温度的演化及其消亡尚未得到广泛研究,而且低温下CDW与超导共存的情况仍知之甚少。我们报道了一项针对\ch{CsV3Sb5}的X射线散射研究,测量覆盖从300 K到约2 K的宽温度范围,其中2 K低于其在$T_c\sim$2.9 K处开始出现的超导转变。对$2\times2\times2$ CDW结构序参量的测量显示,其具有不同寻常且延伸范围很宽的线性温度依赖,该依赖始于$T^*\sim$160 K,远高于与$T_{CDW}=94$ K处CDW序相关的磁化率反常。这意味着强CDW涨落一直存在至约$1.7\times T_{CDW}$。观测到CDW序参量在$T=16$ K至2 K之间保持恒定,表明CDW序与超导序在$T_c$以下共存;并且在环境压力下,两个序参量之间任何可能的竞争即使存在,也只会表现在远低于$T_c$的温度。晶格参数温度依赖中的反常分别表现为:$c(T)$与$T_{CDW}$重合,而$a(T)$与$T^*$重合。

英文摘要:

The phase diagram of the kagome metal family \ch{AV3Sb5} (A = K, Rb, Cs) features both superconductivity and charge density wave (CDW) instabilities, which have generated tremendous recent attention. Nonetheless, significant questions remain. In particular, the temperature evolution and demise of the CDW state has not been extensively studied, and little is known about the co-existence of the CDW with superconductivity at low temperatures. We report an x-ray scattering study of \ch{CsV3Sb5} over a broad range of temperatures from 300 K to $\sim$ 2 K, below the onset of its superconductivity at $\textit{T}_\text{c}\sim$ 2.9 K. Order parameter measurements of the $2\times2\times2$ CDW structure show an unusual and extended linear temperature dependence onsetting at $T^*$ $\sim$ 160 K, much higher than the susceptibility anomaly associated with CDW order at $\textit{T}_\text{CDW}=94$ K. This implies strong CDW fluctuations exist to $\sim1.7\times\textit{T}_\text{CDW}$. The CDW order parameter is observed to be constant from $T=16$ K to 2 K, implying that the CDW and superconducting order co-exist below $\textit{T}_\text{c}$, and, at ambient pressure, any possible competition between the two order parameters is manifested at temperatures well below $\textit{T}_\text{c}$, if at all. Anomalies in the temperature dependence in the lattice parameters coincide with $\textit{T}_\text{CDW}$ for $\textit{c}(T)$ and with $T^*$ for $a(T)$.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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