Multifractality of Hamiltonians with power-law transfer terms
arXiv:cond-mat/0306024 · doi:10.1103/PhysRevB.68.184206
Abstract
Finite-size effects in the generalized fractal dimensions are investigated numerically. We concentrate on a one-dimensional disordered model with long-range random hopping amplitudes in both the strong- and the weak-coupling regime. At the macroscopic limit, a linear dependence of on is found in both regimes for values of $q \alt 4g^{-1}$, where is the coupling constant of the model.
RevTex4, 5 two-column pages, 5 .eps figures, to be published in Phys. Rev. B
References in corpus (1)
Cited by in corpus (17)
- Anderson Transitions
- Exact relations between multifractal exponents at the Anderson transition
- Fraction of delocalized eigenstates in the long-range Aubry-André-Harper model
- Dimensional dependence of the metal-insulator transition
- A semiclassical theory of the Anderson transition
- Non-Hermitian Aubry-André model with Power-Law Hopping
- Boundary multifractality in critical 1D systems with long-range hopping
- Differentiable potentials and metallic states in disordered one-dimensional systems
- Anomalous multifractality in quantum chains with strongly correlated disorder
- Power law hopping of single particles in one-dimensional non-Hermitian quasicrystals
- A critical Dyson hierarchical model for the Anderson localization transition
- Long-range hopping in a quasiperiodic potential weakens the non-Hermitian skin effect
- Criticality in the Quantum Kicked Rotor with a Smooth Potential
- Two-level correlation function of critical random-matrix ensembles
- Critical level spacing distribution in long-range hopping Hamiltonians
- Critical properties in long-range hopping Hamiltonians
- Unraveling Multifractality and Mobility Edges in Quasiperiodic Aubry-André-Harper Chains through High-Harmonic Generation