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pdf, 9 MiB - Infoscience - EPFL

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Chapter 5<br />

Bond-order-wave staggered flux<br />

phase for the t−J model on the<br />

square lattice<br />

5.1 Outline<br />

Motivated by the observation of inhomogeneous patterns in some high-T c cuprate<br />

compounds, several variational Gutzwiller-projected wave-functions with built-in<br />

charge and bond order parameters are proposed for the extended t−J −V model<br />

on the square lattice at low doping. First, following a recent Gutzwiller-projected<br />

mean-field approach (Phys. Rev. B. 72, 060508(R) (2005)), we investigate, as<br />

a function of doping and Coulomb repulsion, the stability of the staggered flux<br />

phase with respect to small spontaneous modulations of squared unit cells ranging<br />

from 2 × 2to √ 32 × √ 32. It is found that a 4 × 4 bond-order (BO) modulation<br />

appears spontaneously on top of the staggered flux pattern for hole doping around<br />

1/8. A related wave-function is then constructed and optimized accurately and<br />

its properties studied extensively using an approximation-free variational Monte<br />

Carlo scheme. Finally, the competition of the BO-modulated staggered flux wavefunction<br />

with respect to the d-wave RVB wave-function or the commensurate<br />

flux state is investigated. It is found that a short range Coulomb repulsion<br />

penalizes the d-wave superconductor and that a moderate Coulomb repulsion<br />

brings them very close in energy. Our results are discussed in connection to the<br />

STM observations in the under-doped regime of some cuprates. This work was<br />

done in collaboration with the group of Didier Poilblanc (IRSAMC, Toulouse,<br />

France). The very nice work related to the renormalized mean-field calculations<br />

within this chapter were done by Sylvain Capponi and Didier Poilblanc. The<br />

work was published in PRB 74, 104506 (2006).<br />

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