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首页> 外文期刊>Physical review, B >La-139 NMR investigation of the interplay between lattice, charge, and spin dynamics in the charge-ordered high-T-c cuprate La1.875Ba0.125CuO4
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La-139 NMR investigation of the interplay between lattice, charge, and spin dynamics in the charge-ordered high-T-c cuprate La1.875Ba0.125CuO4

机译:LA-139核仁核武器,电荷,电荷和旋转动力学之间的相互调查在电荷有序的高T-C铜酸铜铜替代品La1.875ba0.125cuo4中的相互作用

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We investigate the interplay between the lattice, charge, and spin dynamics in charge-ordered high T cuprate La1.875Ba0.125CuO4 (T-c = 4 K) based on the inverse Laplace transform (ILT) analysis of the La-139 nuclear spin-lattice relaxation rate 1/T-1 (dubbed ILTT1 analysis hereafter). A major thrust of the ILTT1 analysis is that one can deduce the probability density function P(1/T-1) of distributed 1/T-1. We demonstrate that 1/T-1(lm), defined as the log mean (i.e., the center of gravity on a logarithmic scale) of P(1/T-1), can be well approximated by 1/T-1(str) deduced from the phenomenological stretched fit; however, P(1/T-1) can provide much richer insight into how the lattice, charge, and spin fluctuations and their distribution develop near and below the long-range charge order at T-charge similar to 54 K. Upon entering the charge-ordered state, a divergent increase of 1/T-1(lm) toward the spin ordering at T-spin(mu SR) similar or equal to 35 K is accompanied by an asymmetric broadening of P(1/T-1). Even deep inside the charge-ordered state, 1/T-1 at a gradually diminishing fraction of La-139 sites continues to slow down as temperature is lowered, as expected for canonical superconducting CuO2 planes without enhanced spin fluctuations. The fraction of such canonical La-139 sites almost disappears by similar or equal to 40 K. In contrast, nearly half of the La-139 sites in La1.885Sr0.115CUO4 (T-charge similar or equal to 80 K) still exhibit the canonical behavior without enhanced spin fluctuations even near its T-c = 31 K. These contrasting behaviors explain why superconductivity in La1.875Ba0.125CuO4 is more strongly suppressed than in La1.885Sr0.115CuO4 despite the lower onset temperature of the charge order.
机译:我们基于LA-139核自旋 - 晶格的逆拉普拉斯变换(ILT)的分析调查晶格,电荷,自旋和主管下令高Tg铜氧化物La1.875Ba0.125CuO4(TC = 4 K)动力学之间的相互作用松弛率1 / T-1(配成ILTT1分析下文)。所述ILTT1分析的主要推力是一个可以推断分布式1 / T-1的概率密度函数P(1 / T-1)。我们证明,1 / T-1(LM),其定义为对数平均(即,重力对数刻度的中心)P(1 / T-1)的,可以通过很好地近似1 / T-1( STR)从现象拉伸拟合推导出然而,P(1 / T-1)可以提供更丰富的洞察晶格,电荷,和自旋涨落和它们的分布如何发展接近和低于在T-电荷类似于54 K.当进入长程加料顺序电荷有序状态,1 / T-1(LM)的发散增加朝向旋排序在T - 自旋(亩SR)类似或等于35 K被伴随着P的非对称展宽(1 / T-1) 。甚至在深拉-139位点上逐渐减小分数电荷有序状态,1 / T-1的内部继续减慢如温度降低时,如预期的,而不增强自旋涨落典型超导CuO2平面。这种正则的La-139位点的分数几乎通过类似于消失或等于40 K.相反,将近一半的在La1.885Sr0.115CUO4 LA-139位点(T-电荷相似或等于80 K)仍表现出甚至没有接近其锝= 31 K.这些行为对比增强自旋涨落规范的行为解释为什么La1.875Ba0.125CuO4超导比在La1.885Sr0.115CuO4尽管充电整理的下起始温度更强烈地抑制。

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  • 来源
    《Physical review, B 》 |2020年第17期| 共9页
  • 作者单位

    Rice Univ Dept Chem &

    Bimol Engn 6100 Main St Houston TX 77005 USA;

    McMaster Univ Dept Phys &

    Astron Hamilton ON L8S 4M1 Canada;

    McMaster Univ Dept Phys &

    Astron Hamilton ON L8S 4M1 Canada;

    Tohoku Univ Inst Mat Res Sendai Miyagi 9808577 Japan;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 固体物理学 ;
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