Differences between the insulating limit quasiparticles of one-band and three-band cuprate models

被引:32
作者
Ebrahimnejad, H. [1 ]
Sawatzky, G. A. [1 ,2 ]
Berciu, M. [1 ,2 ]
机构
[1] Univ British Columbia, Dept Phys & Astron, Vancouver, BC V6T 1Z1, Canada
[2] Univ British Columbia, Quantum Matter Inst, Vancouver, BC V6T 1Z4, Canada
基金
加拿大自然科学与工程研究理事会;
关键词
strongly correlated systems; high temperature superconductivity; quasiparticle dynamics; T-J MODEL; HIGH-TEMPERATURE SUPERCONDUCTIVITY; ANGLE-RESOLVED PHOTOEMISSION; D-P MODEL; 2-DIMENSIONAL QUANTUM ANTIFERROMAGNETS; SPIN-1/2; HEISENBERG-ANTIFERROMAGNET; MONTE-CARLO SIMULATIONS; SINGLE-HOLE; HUBBARD-MODEL; SPECTRAL-FUNCTION;
D O I
10.1088/0953-8984/28/10/105603
中图分类号
O469 [凝聚态物理学];
学科分类号
070205 ;
摘要
We study the charge dynamics of the quasiparticle that forms when a single hole is doped in a two-dimensional antiferromagnet as described by the one-band t-t'-t''-J model, using a variational approximation that includes spin fluctuations in the vicinity of the hole. We explain why the spin fluctuations and the longer range hopping have complementary contributions to the quasiparticle dynamics, and thus why both are essential to obtain a dispersion in agreement with that measured experimentally. This is very different from the three-band Emery model in the strongly-correlated limit, where the same variational approximation shows that spin fluctuations have a minor effect on the quasiparticle dynamics. This difference proves that these one-band and three-band models describe qualitatively different quasiparticles in the insulating limit, and therefore that they cannot both be suitable to describe the physics of very underdoped cuprates.
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页数:14
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