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arXiv 0811.0248cond-mat.str-el
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自旋-电荷旋转参考系方法中Hubbard模型的Neel序:从弱耦合到强耦合的交叉

Neel order in the Hubbard model within spin-charge rotating reference frame approach: crossover from weak to strong coupling

T. A. Zaleski, T. K. Kopec

摘要:

利用量子SU(2)xU(1)转子方法研究了二分立方晶格上最近邻跳跃的二维和三维哈伯德模型的反铁磁相,得到了满足Mermin-Wagner定理的反铁磁态的完全自洽处理.电荷和自旋的集体变量分别以时空涨落U(1)相场和SU(2)对称性支配的旋转自旋量子化轴的形式被隔离。结果,相互作用的电子表现为一个由裸费米子和U(1)、SU(2)规范场组成的复合体。由自旋-电荷转子和费米子场组成的有效作用量是库仑排斥力U和跳跃参数t的函数。我们的理论描述了在零温下从Slater(U <<t)到Mott-Heisenberg(U>> t)反铁磁体的演化。给出了反铁磁哈伯德模型的零温亚晶格磁化强度(2D)和有限温(3D)相图与交叉参数U/t的关系,分析了自旋Berry相在相互作用驱动交叉中的作用.

英文摘要:

The antiferromagnetic phase of two-dimensional (2D) and three-dimensional (3D) Hubbard model with nearest neighbors hopping is studied on a bipartite cubic lattice by means of the quantum SU(2)xU(1) rotor approach that yields a fully self-consistent treatment of the antiferromagnetic state that respects the symmetry properties the model and satisfy the Mermin-Wagner theorem. The collective variables for charge and spin are isolated in the form of the space-time fluctuating U(1) phase field and rotating spin quantization axis governed by the SU(2) symmetry, respectively. As a result interacting electrons appear as a composite objects consisting of bare fermions with attached U(1) and SU(2) gauge fields. An effective action consisting of a spin-charge rotor and a fermionic fields is derived as a function of the Coulomb repulsion U and hopping parameter t. At zero temperature, our theory describes the evolution from a Slater (U<<t) to a Mott-Heisenberg (U>>t) antiferromagnet. The results for zero-temperature sublatice magnetization (2D) and finite temperature (3D) phase diagram of the antiferromagnetic Hubbard model as a function of the crossover parameter U/t are presented and the role of the spin Berry phase in the interaction driven crossover is analyzed.

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