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Hole doped state in extremely lightly doped lanthanum copper oxide.

机译:极轻掺杂的镧氧化铜中的空穴掺杂状态。

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摘要

An effective approach to understanding cuprate physics is to study the physical properties of cuprates at the initial doping level. Experimental studies in the extremely lightly doped region will provide intrinsic initial doping behaviors of cuprates. This information is important for understanding the fundamental mechanism of high temperature superconductivity. In this study, by preparing the samples through controlling the post heat-treatment process and adjusting the hole concentration using the electrochemical method, we investigated the magnetic properties of La2CuO4+delta in the extremely lightly doped region. We find: (1) A ferromagnetic-like anomaly coupled with the three-dimensional anti ferromagnetic transition can be observed after annealing the sample in flowing oxygen at a temperature range from 1040°C to 800°C, which is comparable to the coupling energy of a two-dimension anti ferromagnetic lattice. This result suggests that the ferromagnetic-like anomaly corresponds to an electronic quantum state formed at a temperature where the two-dimensional antiferromagnetic correlation begins to develop. (2) The Neel temperature can be expressed as 1-TN(ph)/TN(0) ≈ 6.2 ph+ (ph/0.025) 2 in the sample prepared with hole concentration steps of 0.001 using the electrochemical method. The Neel temperature in both cation and anion doped La2CuO4 follows the same expression. These results suggest that the suppression of the Neel temperature by doped holes is attributed to a combinatorial effect of dilution and finite size and that the combinatorial effect is an intrinsic property of the doped-hole state. (3) The Neel temperature remained constant at around 250 K when the hole concentration reached ∼0.01 in our La 2CuO4+delta samples. This suggests that there is an intrinsic, critical hole concentration in the La2CuO4+delta system. When the critical hole concentration is reached, the electronic phase separation takes place and the La2CuO4+delta system enters the miscibility gap.
机译:了解铜酸盐物理学的一种有效方法是研究初始掺杂水平下铜酸盐的物理性质。在极轻掺杂区的实验研究将提供固有的铜酸盐初始掺杂行为。该信息对于理解高温超导性的基本机理很重要。在这项研究中,通过控制后热处理过程并使用电化学方法调节空穴浓度来制备样品,我们研究了La2CuO4 +δ在极轻掺杂区的磁性能。我们发现:(1)在1040°C至800°C的温度范围内的流动氧气中对样品进行退火后,可以观察到与三维反铁磁跃迁耦合的类铁磁异常。二维反铁磁晶格该结果表明,类似铁磁的异常对应于在二维反铁磁相关性开始发展的温度下形成的电子量子态。 (2)尼尔温度可以表示为1-TN(ph)/ TN(0)≈。使用电化学方法,以0.001的空穴浓度步骤制备的样品中的6.2ph +(ph / 0.025)2。阳离子和阴离子掺杂的La2CuO4中的Neel温度遵循相同的表达式。这些结果表明,掺杂孔对Neel温度的抑制归因于稀释和有限尺寸的组合效应,并且该组合效应是掺杂孔态的固有性质。 (3)当我们的La 2CuO4 +δ样品中空穴浓度达到〜0.01时,尼尔温度保持恒定在250 K左右。这表明La2CuO4 +δ系统中存在固有的临界空穴浓度。当达到临界空穴浓度时,发生电子相分离,La2CuO4 +δ体系进入混溶间隙。

著录项

  • 作者

    Wu, Zheng.;

  • 作者单位

    University of Houston.;

  • 授予单位 University of Houston.;
  • 学科 Physics Condensed Matter.
  • 学位 Ph.D.
  • 年度 2004
  • 页码 99 p.
  • 总页数 99
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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