论文标题
cak中的列不断波动的进化
Evolution of nematic fluctuations in CaK(Fe$_{1-x}$Ni$_{x}$)$_{4}$As$_{4}$ with spin-vortex crystal magnetic order
论文作者
论文摘要
cak(fe $ _ {1-x} $ ni $ _ {x} $)$ _ {4} $作为$ _ {4} $超导体类似于原型的基于122型铁的材料,但具有明显较低的对称性的晶体结构。该家族举办了所谓的自旋涡流晶体磁序的少数示例之一,这是一种非连接磁性构型,可保留四方对称性,与原晶体线条条纹型磁性构型相比,这是122型类型的系统。因此,从其相图完全不存在列表。为了在这种情况下调查列的波动的演变,我们在cak(fe $ _ {1-x} $ ni $ _ {x} $)$ _ {4} $ as $ _ {4} $中介绍了弹性和弹性模量测量值,作为$ _ {4}我们发现明确的实验性签名具有相当大的列表波动,包括对年轻的模量$ y _ _ {[110]} $的软化以及cak中B2G弹力率系数的curie-weiss型分歧(fe $ $ _ {0.951} $ ni $ _ $ _ {0.049} $ ________________________ $ __ 4.44。总体而言,本系列中的列表波动与孔掺杂的Ba $ _ {1-x} $ k $ _x $ _x $ fe $ _2 $ AS $ _2 $系列具有很强的相似之处,包括替代诱导的签名更改。我们的理论分析探讨了1144型结构的特定晶体对称性对确定其磁接地状态和列的波动的影响。
The CaK(Fe$_{1-x}$Ni$_{x}$)$_{4}$As$_{4}$ superconductors resemble the archetypal 122-type iron-based materials but have a crystal structure with distinctly lower symmetry. This family hosts one of the few examples of the so-called spin-vortex crystal magnetic order, a non-collinear magnetic configuration that preserves tetragonal symmetry, in contrast to the orthorhombic collinear stripe-type magnetic configuration common to the 122-type systems. Thus, nematic order is completely absent from its phase diagram. To investigate the evolution of nematic fluctuations in such a case, we present elastoresistance and elastic modulus measurements in CaK(Fe$_{1-x}$Ni$_{x}$)$_{4}$As$_{4}$ ($x = 0-0.05$) combined with phenomenological modeling and density functional theory. We find clear experimental signatures of considerable nematic fluctuations, including softening of the Young's modulus $Y_{[110]}$ and a Curie-Weiss type divergence of the B2g elastoresistance coefficient in CaK(Fe$_{0.951}$Ni$_{0.049}$)$_4$As$_4$. Overall, nematic fluctuations within this series bear strong similarities to the hole-doped Ba$_{1-x}$K$_x$Fe$_2$As$_2$ series, including a substitution-induced sign change. Our theoretical analysis addresses the effect of the specific crystal symmetry of the 1144-type structure in determining its magnetic ground state and on the nematic fluctuations.