Finite compressibility in the low-doping region of the two-dimensional model
arXiv:cond-mat/0606659 · doi:10.1103/PhysRevB.74.165122
Abstract
We revisit the important issue of charge fluctuations in the two-dimensional model by using an improved variational method based on a wave function that contains both the antiferromagnetic and the d-wave superconducting order parameters. In particular, we generalize the wave function introduced some time ago by J.P. Bouchaud, A. Georges, and C. Lhuillier [J. de Physique {\bf 49}, 553 (1988)] by considering also a {\it long-range} spin-spin Jastrow factor, in order to correctly reproduce the small- behavior of the spin fluctuations. We mainly focus our attention on the physically relevant region and find that, contrary to previous variational ansatz, this state is stable against phase separation for small hole doping. Moreover, by performing projection Monte Carlo methods based on the so-called fixed-node approach, we obtain a clear evidence that the model does not phase separate for and that the compressibility remains finite close to the antiferromagnetic insulating state.
10 pages
References in corpus (2)
Cited by in corpus (9)
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