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Revisiting the 63Cu NMR Signature of Charge Order in La1.875Ba0.125CuO4
Journal of the Physical Society of Japan ( IF 1.5 ) Pub Date : 2021-02-05 , DOI: 10.7566/jpsj.90.034705
Takashi Imai 1 , Philip M. Singer 2 , Alexandre Arsenault 1 , Masaki Fujita 3
Affiliation  

We use single crystal 63Cu NMR techniques to revisit the early 63Cu NQR signature of charge order observed for La1.875Ba0.125CuO4 (Tc = 4 K) [A. W. Hunt et al., Phys. Rev. Lett. 82, 4300 (1999)]. We show that the growth of spin correlations is accelerated below ∼80 K, where the inverse Laplace transform (ILT) T1 analysis of the 139La NMR spin–lattice relaxation curve recently uncovered emergence of the slow components in the lattice and/or charge fluctuations [P. M. Singer et al., Phys. Rev. B 101, 174508 (2020)]. From the accurate measurements of the 63Cu NMR signal intensity, spin echo decay M(2τ), spin–lattice relaxation rate 631/T1, and its density distribution function P(631/T1), we also demonstrate that charge order at Tcharge \( \simeq \) 54 K turns on strong enhancement of spin fluctuations within charge ordered domains, thereby making the CuO2 planes extremely inhomogeneous. The charge ordered domains grow quickly below Tcharge, and the volume fraction FCA of the canonical domains unaffected by charge order gradually diminishes by ∼35 K. This finding agrees with our independent estimations of FCA based entirely on the 139La ILTT1 analyses, but is in a stark contrast with much slower growth of charge ordered domains observed for La1.885Sr0.115CuO4 from its Tcharge \( \simeq \) 80 K to Tc \( \simeq \) 30 K.

中文翻译:

重新审视La1.875Ba0.125CuO4中电荷顺序的63Cu NMR特征

我们使用单晶63 Cu NMR技术重现了La 1.875 Ba 0.125 CuO 4T c = 4 K)观察到的电荷顺序的早期63 Cu NQR签名[AW Hunt等,Phys。牧师 82,4300(1999)]。我们表明,自旋相关性的增长在〜80 K以下加速,其中139 La NMR自旋-晶格弛豫曲线的逆拉普拉斯变换(ILT)T 1分析最近发现了晶格和/或电荷中慢速成分的出现。波动[PM Singer等人,Phys。版本B 101,174508(2020)]。从63的准确测量Cu NMR信号强度,自旋回波衰减M),自旋-晶格弛豫速率63 1 / T 1及其密度分布函数P63 1 / T 1),我们还证明了T电荷的电荷顺序 \(\ simeq \)54 K开启了电荷有序域内自旋涨落的强烈增强,从而使CuO 2平面极为不均匀。电荷有序域在T电荷以下快速增长,不受电荷阶数影响的规范域的体积分数F CA逐渐减小约35K。这一发现与我们完全基于139 La ILTT 1分析得出的F CA独立估计相符。,但与La 1.885 Sr 0.115 CuO 4从其T观察到的电荷有序域的增长要慢得多收费 \(\ simeq \)80 K为T c \(\ simeq \) 30K。
更新日期:2021-02-05
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