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Slave-rotor mean-field theories of strongly correlated systems and the Mott transition in finite dimensions

机译:强相关系统的从转子平均场理论和有限维数的Mott跃迁

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摘要

The multiorbital Hubbard model is expressed in terms of quantum phase variables ("slave rotors") conjugate to the local charge, and of auxiliary fermions, providing an economical representation of the Hilbert space of strongly correlated systems. When the phase variables are treated in a local mean-field manner, similar results to the dynamical mean-field theory are obtained, namely a Brinkman-Rice transition at commensurate fillings together with a "preformed" Mott gap in the single-particle density of states. The slave-rotor formalism allows to go beyond the local description and take into account spatial correlations, following an analogy to the superfluid-insulator transition of bosonic systems. We find that the divergence of the effective mass at the metal-insulator transition is suppressed by short range magnetic correlations in finite-dimensional systems. Furthermore, the strict separation of energy scales between the Fermi-liquid coherence scale and the Mott gap, found in the local picture, holds only approximately in finite dimensions, due to the existence of low-energy collective modes related to zero-sound.
机译:多轨道哈伯德模型用与局部电荷共轭的量子相位变量(“从动转子”)和辅助费米子表示,从而提供了经济相关的强相关系统希尔伯特空间的表示。当以局部平均场方式处理相位变量时,可获得与动态平均场理论相似的结果,即在相称填充处的Brinkman-Rice跃迁以及单粒子密度的“预制” Mott间隙。状态。从动转子形式主义可以超越对局部的描述,并可以像对玻色子系统的超流体-绝缘体转变一样考虑空间相关性。我们发现,有限元系统中的短程磁相关抑制了金属-绝缘体转变时有效质量的发散。此外,由于存在与零声有关的低能集体模态,在局部图中发现的费米-液体相干尺度和莫特间隙之间的能级严格分离仅在有限的维度上有效。

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