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Magnetic phase diagram of a five-orbital Hubbard model in the real-space Hartree-Fock approximation varying the electronic density

机译:改变电子密度的真实空间Hartree-Fock近似中的五轨道Hubbard模型的磁相图

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摘要

Using the real-space Hartree-Fock approximation, the magnetic phase diagram of a five-orbital Hubbard model for the iron-based superconductors is studied varying the electronic density n in the range from five to seven electrons per transition metal atom. The Hubbard interaction U is also varied, at a fixed Hund coupling J/U = 0.25. Several qualitative trends and a variety of competing magnetic states are observed. At n = 5, a robust G-type antiferromagnetic insulator is found, in agreement with experimental results for BaMn_2As_2). As n increases away from 5, magnetic states with an increasing number of nearest-neighbors ferromagnetic links become energetically stable. This includes the well-known C-type antiferromagnetic state at n - 6, the E-phase known to exist in FeTe, and also a variety of novel states not found yet experimentally, some of them involving blocks of ferromagnetically oriented spins. Regions of phase separation, as in Mn oxides, have also been detected. Comparison to previous theoretical investigations indicate that these qualitative trends may be generic characteristics of phase diagrams of multi-orbital Hubbard models.
机译:使用实空间Hartree-Fock逼近,研究了铁基超导体的五轨道Hubbard模型的磁相图,该模型的电子密度n在每个过渡金属原子5至7个电子的范围内变化。在固定的洪德耦合J / U = 0.25时,哈伯德相互作用U也发生变化。观察到一些定性趋势和各种竞争的磁态。在n = 5处,找到了坚固的G型反铁磁绝缘体,与BaMn_2As_2的实验结果一致。当n远离5时,具有最近邻居铁磁链接数量增加的磁态在能量上变得稳定。这包括在n-6处的众所周知的C型反铁磁态,在FeTe中存在的E相,以及实验上尚未发现的多种新型态,其中一些涉及铁磁取向的自旋嵌段。也已经检测到相分离区域,如锰氧化物。与先前理论研究的比较表明,这些定性趋势可能是多轨道哈伯德模型相图的一般特征。

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  • 来源
    《Physical review》 |2014年第4期|045115.1-045115.8|共8页
  • 作者

    Qinlong Luo; Elbio Dagotto;

  • 作者单位

    Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA,Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

    Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA,Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA;

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