Effective approach to the Nagaoka regime of the two-dimensional t-J model

被引:12
|
作者
Maska, M. M. [1 ]
Mierzejewski, M. [1 ]
Kochetov, E. A. [2 ]
Vidmar, L. [3 ]
Bonca, J. [3 ,4 ]
Sushkov, O. P. [5 ]
机构
[1] Univ Silesia, Inst Phys, Dept Theoret Phys, PL-40007 Katowice, Poland
[2] Joint Inst Nucl Res, Theoret Phys Lab, Dubna 141980, Russia
[3] J Stefan Inst, SI-1000 Ljubljana, Slovenia
[4] Univ Ljubljana, FMF, Dept Phys, SI-1000 Ljubljana, Slovenia
[5] Univ New S Wales, Sch Phys, Sydney, NSW 2052, Australia
来源
PHYSICAL REVIEW B | 2012年 / 85卷 / 24期
关键词
HIGH-TEMPERATURE SUPERCONDUCTORS; STRONGLY CORRELATED ELECTRONS; U HUBBARD-MODEL; FILLED S-BAND; PHASE-SEPARATION; HOLES; NARROW; STATE; ANTIFERROMAGNET; FERROMAGNETISM;
D O I
10.1103/PhysRevB.85.245113
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We argue that the t-J model and the recently proposed Ising version of this model give the same physical picture of the Nagaoka regime for J/t << 1. In particular, both models are shown to give compatible results for a single Nagaoka polaron as well as for a Nagaoka bipolaron. When compared to the standard t-J or t-J(z) models, the Ising version allows for a numerical analysis on much larger clusters by means of classical Monte Carlo simulations. Taking advantage of this fact, we study the low doping regime of the t-J model for J/t << 1 and show that the ground state exhibits phase separation into hole-rich ferromagnetic and hole-depleted antiferromagnetic regions. This picture holds true up to a threshold concentration of holes delta <= delta(t) similar or equal to 0.44v root J/t. Analytical calculations show that delta(t) = root J/2 pi t.
引用
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页数:9
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