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Correlated-Electron Systems and High-Temperature Superconductivity

机译:相关电子系统和高温超导

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We present recent theoretical results on superconductivity in correlated-electron systems, especially in the two-dimensional Hubbard model and the three-band d-p model. The mechanism of superconductivity in high-temperature superconductors has been extensively studied on the basis of various electronic models and also electron-phonon models. In this study, we investigate the properties of superconductivity in correlated-electron systems by using numerical methods such as the variational Monte Carlo method and the quantum Monte Carlomethod. The Hubbard model is one of basic models for strongly correlated electron systems, and is regarded as the model of cuprate high temperature superconductors. The d-p model is more realistic model for cuprates. The superconducting condensation energy obtained by adopting the Gutzwiller ansatz is in reasonable agreement with the condensation energy estimated for YBa2Cu3O7. We show the phase diagram of the ground state using this method. We have further investigated the stability of striped and checkerboard states in the under-doped region. Holes doped in a half-filled square lattice lead to an incommensurate spin and charge density wave. The relationship of the hole density x and incommensurability δ, δ~x, is satisfied in the lower doping region, as indicated by the variationalMonte Carlocalculations for the two-dimensional Hubbard model. A checkerboard-like charge-density modulation with a roughly period has also been observed by scanning tunneling microscopy experiments in Bi2212 and Na-CCOC compounds. We have performed a variational Monte Carlo simulation on a two-dimensional t-t′-t″- U Hubbard model with a Bi-2212 type band structure and found that the period checkerboard spin modulation, that is characterized by multi Q vectors, is indeed stabilized. We have further performed an investigation by using a quantumMonte Carlomethod, which is a numerical method that can be used to simulate the behavior of correlated electron systems. We present a new algorithm of the quantum Monte Carlo diagonalization that is a method for the evaluation of expectation value without the negative sign problem. We compute pair correlation functions and show that pair correlation is indeed enhanced with hole doping.
机译:我们提出了有关相关电子系统中超导性的最新理论结果,尤其是在二维Hubbard模型和三波段d-p模型中。在各种电子模型以及电子-声子模型的基础上,对高温超导体中的超导机理进行了广泛的研究。在这项研究中,我们使用变分蒙特卡罗方法和量子蒙特卡洛方法等数值方法研究了相关电子系统中的超导性质。哈伯德模型是强相关电子系统的基本模型之一,被视为铜酸盐高温超导体的模型。 d-p模型是更实用的铜价模型。通过采用Gutzwiller ansatz获得的超导冷凝能量与YBa2Cu3O7估计的冷凝能量在合理范围内一致。我们使用这种方法显示了基态的相图。我们进一步研究了掺杂不足区域中条纹和棋盘状状态的稳定性。掺杂在半填充方格中的空穴会导致自旋和电荷密度波不相称。如在二维哈伯德模型中的变分蒙特卡罗计算所表明的那样,在较低的掺杂区域中满足了空穴密度x和不可通约性δ,δ〜x的关系。通过在Bi2212和Na-CCOC化合物中进行扫描隧道显微镜实验,还观察到了大致呈棋盘状的电荷密度调制。我们对具有Bi-2212型带结构的二维tt'-t“ -U Hubbard模型进行了变分蒙特卡罗模拟,发现以多个Q矢量为特征的周期棋盘旋转调制确实稳定了。我们通过使用量子蒙特卡洛方法(QuantumMonte Carlomethod)进行了进一步的研究,这是一种可以用来模拟相关电子系统行为的数值方法。我们提出了一种新的量子蒙特卡洛对角化算法,该算法是一种用于评估期望值而没有负号问题的方法。我们计算了对相关函数,并显示出空穴掺杂确实增强了对相关性。

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