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Coupling of structure to magnetic and superconducting orders in quasi-one-dimensional K_2Cr_3As_3

机译:准一维K_2Cr_3As_3中结构与磁和超导阶的耦合

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Quasi-one-dimensional A_2Cr_3As_3 (with A = K, Cs, Rb) is an intriguing new family of superconductors which exhibit many similar features to the cuprate and iron-based unconventional superconductor families. Yet, in contrast to these systems, no charge or magnetic ordering has been observed which could provide the electronic correlations presumed necessary for an unconventional superconducting pairing mechanism— an absence which defies predictions of first-principles models. We report the results of neutron scattering experiments on polycrystalline K_2Cr_3As_3 (T_c ~ 7 K) which probed the low-temperature dynamics near T_c. Neutron diffraction data evidence a subtle response of the nuclear lattice to the onset of superconductivity while inelastic scattering reveals a highly dispersive column of intensity at the commensurate wave vector q = (001/2) which loses intensity beneath T_c—indicative of short-range magnetic fluctuations. Using linear spin-wave theory, we model the observed scattering and suggest a possible structure to the short-range magnetic order. These observations suggest that K_2Cr_3 As_3 is in close proximity to a magnetic instability and that the incipient magnetic order both couples strongly to the lattice and competes with superconductivity, in direct analogy with the iron-based superconductors.
机译:准一维A_2Cr_3As_3(A = K,Cs,Rb)是一个令人着迷的超导体新系列,与铜酸盐和铁基非常规超导体系列具有许多相似的特征。但是,与这些系统相比,没有观察到电荷或磁排序可以提供非常规超导配对机制所必需的电子相关性,而这种缺失不符合第一性原理模型的预测。我们报告了在多晶K_2Cr_3As_3(T_c〜7 K)上中子散射实验的结果,该晶体探测了T_c附近的低温动力学。中子衍射数据表明核晶格对超导性的起了微妙的反应,而无弹性散射则在相应的波矢q =(001/2)处显示出高度分散的强度列,该列在T_c以下失去了强度,这表明是短程磁波动。使用线性自旋波理论,我们对观察到的散射进行建模,并为短程磁阶建议了一种可能的结构。这些观察结果表明,K_2Cr_3 As_3非常接近于磁性不稳定性,并且与铁基超导体直接相似,初生磁阶既与晶格强烈耦合,又与超导竞争。

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    《Physical review. B, Condensed Matter And Materals Physics》 |2017年第18期|180506.1-180506.5|共5页
  • 作者单位

    Quantum Condensed Matter Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

    Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

    Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

    Quantum Condensed Matter Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

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