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Exact solution of the 1D Hubbard model with NN and NNN interactions in the narrow-band limit

机译:具有NN和NNN相互作用的1D Hubbard模型的精确解   窄带限制

摘要

We present the exact solution, obtained by means of the Transfer Matrix (TM)method, of the 1D Hubbard model with nearest-neighbor (NN) andnext-nearest-neighbor (NNN) Coulomb interactions in the atomic limit (t=0). Thecompetition among the interactions ($U$, $V_1$, and $V_2$) generates a plethoraof T=0 phases in the whole range of fillings. $U$, $V_1$, and $V_2$ are theintensities of the local, NN and NNN interactions, respectively. We report theT=0 phase diagram, in which the phases are classified according to the behaviorof the principal correlation functions, and reconstruct a representativeelectronic configuration for each phase. In order to do that, we make ananalytic limit $T\to 0$ in the transfer matrix, which allows us to obtainanalytic expressions for the ground state energies even for extended transfermatrices. Such an extension of the standard TM technique can be easily appliedto a wide class of 1D models with the interaction range beyond NN distance,allowing for a complete determination of the T=0 phase diagrams.
机译:我们提出了通过转移矩阵(TM)方法获得的一维Hubbard模型的精确解,该模型在原子极限(t = 0)中具有最近邻(NN)和近邻(NNN)库仑相互作用。相互作用($ U $,$ V_1 $和$ V_2 $)之间的竞争在整个填充范围内生成了大量的T = 0相。 $ U $,$ V_1 $和$ V_2 $分别是局部,NN和NNN交互的强度。我们报告了T = 0相图,其中根据主要相关函数的行为对相进行了分类,并为每个相重建了一个有代表性的电子配置。为此,我们在传递矩阵中将解析极限$ T \设为0 $,这使我们即使对于扩展的传递矩阵,也可以获得基态能量的解析表达式。标准TM技术的这种扩展可以很容易地应用于相互作用范围超过NN距离的一维一维模型中,从而可以完全确定T = 0相图。

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