2015
DOI: 10.1103/physreva.92.053622
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Enhancing quantum coherence with short-range correlated disorder

Abstract: We introduce a two-dimensional short-range correlated disorder that is the natural generalization of the well-known one-dimensional dual random dimer model [Phys. Rev. Lett 65, 88 (1990)]. We demonstrate that, as in one dimension, this model induces a localization-delocalization transition in the single-particle spectrum. Moreover we show that the effect of such a disorder on a weaklyinteracting boson gas is to enhance the condensate spatial homogeneity and delocalisation, and to increase the condensate fracti… Show more

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Cited by 4 publications
(14 citation statements)
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“…3 we compare the time evolution of a density perturbation in an UN-RAND lattice and in a 2D-DRDM one for t = 3t, different values of ∆ and p = 0.25. We consider a system with a weak interaction U/t = 10 −2 and average number of particles per site n i = 5 [6]. For any value of ∆ in the UN-RAND model, the density perturbation distorts as it moves through the system; whereas in the 2D-DRDM, if ∆ is close to the resonant value ∆ res = 32t, the density perturbation propagates for a long time without a pronounced dispersion.…”
Section: Density Wave Propagationmentioning
confidence: 99%
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“…3 we compare the time evolution of a density perturbation in an UN-RAND lattice and in a 2D-DRDM one for t = 3t, different values of ∆ and p = 0.25. We consider a system with a weak interaction U/t = 10 −2 and average number of particles per site n i = 5 [6]. For any value of ∆ in the UN-RAND model, the density perturbation distorts as it moves through the system; whereas in the 2D-DRDM, if ∆ is close to the resonant value ∆ res = 32t, the density perturbation propagates for a long time without a pronounced dispersion.…”
Section: Density Wave Propagationmentioning
confidence: 99%
“…If the Hamiltonian parameters are tuned * Electronic address: capuzzi@df.uba.ar † Electronic address: Patrizia.Vignolo@inphyni.cnrs.fr so that the resonance energy matches the ground-state energy, the ground state is not affected by the disorder, even in the presence of weak interactions. The density homogenization induced by the resonance drives the superfluid fraction [6]. This happens at the ground-state energy, but, as soon as the system is perturbed, higher energy states are involved, and it is not straightforward to derive the response of the system.…”
Section: Introductionmentioning
confidence: 99%
“…and ù=r 2 /r 1 . For any eigenvalue of the momentum q, let x(q, s) be the sth zero of the crossproduct of Bessel functions (49), with x q s x q s , 1 ,…”
Section: Radial Part Of the Schrödinger Equationmentioning
confidence: 99%
“…The values x(q, s) can be obtained by solving numerically (49); for larger values of s one can also use the asymptotic expansion provided by the McMahon formula [65].…”
Section: Radial Part Of the Schrödinger Equationmentioning
confidence: 99%
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