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Synthetic Metals

Quantum Monte Carlo study of the one-dimensional extended Hubbard Hamiltonian

W. R. Somsky, David K Campbell, H. Q. Lin, X Wang, James E. Gubernatis

Published Jun 1, 1991• 6 citations
Publisher
DOI
10.1016/0379-6779(91)91343-9

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We extend a Quantum Monte Carlo (QMC) algorithm to the Hubbard model containing bond-dependent off-diagonal hoppings, which describes the manganites and other similar systems, such as systems with spin-flip hoppings. To show correctness of this extension, we detect two simple examples of one-dimensional chains. The first one is half-filled and the hopping matrixes between arbitrary nearest neighboring pairs are uniform, i.e., ${t}_{i,i+1}{=t}_{i+1,i+2}$ $(i=1,2,3,\dots{}).$ The other one is quarter-filled and the hopping matrixes alternate every four lattice constants with ${t}_{i,i+1}{=t}_{i+1,i+2}\ensuremath{\ne}{t}_{i+2,i+3}{=t}_{i+3,i+4}$ $(i=1,5,9,\dots{}).$ Results of the two examples are reasonable.

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We extend a Quantum Monte Carlo (QMC) algorithm to the Hubbard model containing bond-dependent off-diagonal hoppings, which describes the manganites and other similar systems, such as systems with spin-flip hoppings. To show correctness of this extension, we detect two simple examples of one-dimensional chains. The first one is half-filled and the hopping matrixes between arbitrary nearest neighboring pairs are uniform, i.e., ti,i+1=ti+1,i+2{t}_{i,i+1}{=t}_{i+1,i+2}ti,i+1​=ti+1,i+2​ (i=1,2,3,…).(i=1,2,3,\dots{}).(i=1,2,3,…). The other one is quarter-filled and the hopping matrixes alternate every four lattice constants with ${t}_{i,i+1}{=t}_{i+1,i+2}\ensuremath{\ne}{t}_{i+2,i+3}{=t}_{i+3,i+4}$ (i=1,5,9,…).(i=1,5,9,\dots{}).(i=1,5,9,…). Results of the two examples are reasonable.