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arXiv 0911.2245cond-mat.supr-concond-mat.mtrl-scicond-mat.str-el
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用角分辨光电子能谱研究镧系铜氧化物中$(π,π)$阴影带的掺杂依赖性

Doping dependence of the $(π,π)$ shadow band in La-based cuprates studied by angle-resolved photoemission spectroscopy

Rui-Hua He, X. J. Zhou, M. Hashimoto, T. Yoshida, K. Tanaka, S. -K. Mo, T. Sasagawa, N. Mannella, W. Meevasana, Hong Yao, M. Fujita, T. Adachi, S. Komiya, S. Uc… 展开作者

Rui-Hua He, X. J. Zhou, M. Hashimoto, T. Yoshida, K. Tanaka, S. -K. Mo, T. Sasagawa, N. Mannella, W. Meevasana, Hong Yao, M. Fujita, T. Adachi, S. Komiya, S. Uchida, Y. Ando, F. Zhou, Z. X. Zhao, A. Fujimori, Y. Koike, K. Yamada, Z. Hussain, Z. -X. Shen

摘要:

用角分辨光电子能谱(ARPES)研究了镧系铜氧化物(La 214)中$(π,π)$阴影带(SB)在$x=0.01$ ~ $x=0.25$的宽掺杂范围内的变化.与基于Bi的铜酸盐家族的充分研究的情况不同,观察到在费米能级($E_F$)处的SB强度的整体强的单调掺杂依赖性。与之前的报告相比,SB的存在仅接近$x=1/8$,我们发现它存在于一个很宽的掺杂范围内,与掺杂无关的$(π,π)$波矢量,但强烈的掺杂依赖强度:它是最强的$x\sim 0.03$和系统地减少,因为掺杂的增加,直到它变得可以忽略不计的过掺杂制度。该SB与所观察到的强度的掺杂依赖性原则上可以由反铁磁波动或已知在系统中持续到$x\sim 0.21$的特定形式的低温正交晶格畸变引起,两者都随着掺杂的增加而减弱。然而,一个详细的结合能依赖于SB在$x=0.07$的分析似乎不支持前一种解释,离开后者作为一个更合理的候选人,尽管在定量连接的SB强度和晶格畸变的大小的掺杂依赖性的挑战。我们的发现强调了一个仔细的和全球性的考虑固有的结构复杂性的必要性,正确理解的铜酸盐费米学及其微观含义。

英文摘要:

The $(π,π)$ shadow band (SB) in La-based cuprate family (La214) was studied by angle-resolved photoemission spectroscopy (ARPES) over a wide doping range from $x=0.01$ to $x=0.25$. Unlike the well-studied case of the Bi-based cuprate family, an overall strong, monotonic doping dependence of the SB intensity at the Fermi level ($E_F$) was observed. In contrast to a previous report for the presence of the SB only close to $x=1/8$, we found it exists in a wide doping range, associated with a doping-independent $(π,π)$ wave vector but strongly doping-dependent intensity: It is the strongest at $x\sim 0.03$ and systematically diminishes as the doping increases until it becomes negligible in the overdoped regime. This SB with the observed doping dependence of intensity can in principle be caused by the antiferromagnetic fluctuations or a particular form of low-temperature orthorhombic lattice distortion known to persist up to $x\sim 0.21$ in the system, with both being weakened with increasing doping. However, a detailed binding energy dependent analysis of the SB at $x=0.07$ does not appear to support the former interpretation, leaving the latter as a more plausible candidate, despite a challenge in quantitatively linking the doping dependences of the SB intensity and the magnitude of the lattice distortion. Our finding highlights the necessity of a careful and global consideration of the inherent structural complications for correctly understanding the cuprate Fermiology and its microscopic implication.

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