Fermion-Spin Transformation to Implement the Charge-Spin Separation
arXiv:cond-mat/9311002 · doi:10.1103/PhysRevB.49.2368
Abstract
A novel approach, the fermion-spin transformation to implement the charge-spin separation, is developed to study the low-dimensional - model. In this approach, the charge and spin degrees of freedom of the physical electron are separated, and the charge degree of freedom is represented by a spinless fermion while the spin degree of freedom is represented by a {\it hard-core boson}. The on-site local constraint for single occupancy is satisfied even in the mean-field approximation and the sum rule for the physical electron is obeyed. This approach can be applied to both one and two-dimensional systems. In the one-dimensional case, the spinon as well as the physical electron behaves like Luttinger liquids. We have obtained a gapless charge and spin excitation spectrum, a good ground state energy, and a reasonable electron-momentum distribution within the mean-field approximation. The correct exponents of the correlation functions and momentum distribution are also obtained if the {\it squeezing} effect and rearrangement of the spin configurations are taken into account. In the two-dimensional case, within the mean-field approximation the magnetized flux state with a gap in the spinon spectrum has the lowest energy at half-filling. The antiferromagnetic long-range order is destroyed by hole doping
REVTEX (42 pages, eight figures upon request), International Centre for Theoretical Physics preprint IC/93/354 (accepted for publication in Physical Review B)
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