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On the nature of the magnetic transition in a Mott insulator

机译:关于莫特绝缘子中磁跃迁的性质

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Using a combination of exact enumeration and the dynamical mean-field theory (DMFT) we study the drastic change of the spectral properties, obtained in the half-filled two-dimensional Hubbard model at a transition from an antiferromagnetic to a paramagnetic Mott insulator, and compare it with the results obtained using the quantum Monte Carlo method. The coherent hole (electron) quasiparticle spin-polaron subbands are gradually smeared out when the AF order disappears, either for increasing Coulomb repulsion U at fixed temperature T, or for increasing T at fixed U. Within the DMFT we present numerical evidence (a continuous disappearence of the order parameter) suggesting that the above magnetic transition is second order both in two and in three dimensions.
机译:使用精确枚举和动态平均场理论(DMFT)的组合,我们研究了在从反铁磁到顺磁Mott绝缘子的过渡中,在半填充二维Hubbard模型中获得的光谱特性的急剧变化,以及将其与使用量子蒙特卡洛方法获得的结果进行比较。当AF阶消失时,相干的空穴(电子)准粒子自旋极化子子带逐渐被抹去,或者用于在固定温度T下增加库仑斥力U,或者用于在固定温度T下增加T。在DMFT中,我们提供了数字证据(连续阶参数的消失)表明上述磁跃变在二维和三维上都是二阶的。

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