E. Cuevas
University of Murcia
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Publication
Featured researches published by E. Cuevas.
Physical Review B | 2003
E. Cuevas
The system size dependence of the multifractal spectrum
Physical Review Letters | 2001
E. Cuevas; M. Ortuño; V. Gasparian; Antonio Pérez-Garrido
f(\ensuremath{\alpha})
Physical Review B | 2007
Antonio M. García-García; E. Cuevas
and its singularity strength
Physical Review Letters | 2001
E. Cuevas; V. Gasparian; M. Ortuño
\ensuremath{\alpha}
Physical Review Letters | 1999
E. Cuevas
is investigated numerically. We focus on one-dimensional (1D) and 2D disordered systems with long-range random hopping amplitudes in both the strong and the weak disorder regime. At the macroscopic limit, it is shown that
Physical Review B | 2010
V. E. Kravtsov; A. Ossipov; Oleg M. Yevtushenko; E. Cuevas
f(\ensuremath{\alpha})
Journal of Physics A | 2010
S Kronmüller; Oleg M. Yevtushenko; E. Cuevas
is parabolic in the weak disorder regime. In the case of strong disorder, on the other hand,
Physical Review B | 2009
Antonio M. García-García; E. Cuevas
f(\ensuremath{\alpha})
EPL | 1999
M. Ortuño; E. Cuevas
strongly deviates from parabolicity. Within our numerical uncertainties it has been found that all corrections to the parabolic form vanish at some finite value of the coupling strength.
Journal of Physics A | 1996
A. Pérez‐Garrido; M. Ortuño; E. Cuevas; J. Ruiz
We investigate numerically the inverse participation ratio, P(2), of the 3D Anderson model and of the power-law random banded matrix (PRBM) model at criticality. We found that the variance of lnP(2) scales with system size L as sigma(2)(L) = sigma(2)(infinity)-AL(-D(2)/2d), with D(2) being the correlation dimension and d the system dimension. Therefore the concept of a correlation dimension is well defined in the two models considered. The 3D Anderson transition and the PRBM transition for b = 0.3 (see the text for the definition of b) are fairly similar with respect to all critical magnitudes studied.