Numerical study of disorder effects on the three-dimensional Hubbard model
arXiv:cond-mat/0005270 · doi:10.1088/0953-8984/12/44/312
Abstract
Combined effects of interactions and disorder are investigated using a finite temperature quantum Monte Carlo technique for the three-dimensional Hubbard model with random potentials of a finite range. Temperature dependence of the charge compressibility shows that the Mott gap collapses beyond a finite disorder strength. This is a quantum phase transition from an incompressible phase to a compressible phase driven by disorder. We calculate the antiferromagnetic structure factor in the presence of disorder as well. Strong antiferromagnetic correlation, which is characteristic of the Mott insulator, is destroyed by a finite amount of disorder.
3 pages, 2 figures, submitted to Phys. Rev. B
Cited by in corpus (11)
- Dynamical Mean Field Study of the Two-Dimensional Disordered Hubbard Model
- Non Fermi liquid behavior and continuously tunable resistivity exponents in the Anderson-Hubbard model at finite temperature
- Local Spectroscopies Reveal Percolative Metal in Disordered Mott Insulators
- Variational Monte Carlo Study of Anderson Localization in the Hubbard Model
- Doping-dependent metal-insulator transition in a disordered Hubbard model
- Strong-coupling perturbative study of the disordered Hubbard model on honeycomb lattice
- Optical conductivity of a metal-insulator transition for the Anderson-Hubbard model in 3 dimensions away from 1/2 filling
- Critiquing Variational Theories of the Anderson-Hubbard Model: Real-Space Self-Consistent Hartree-Fock Solutions
- Transport and spectroscopic signatures of a disorder-stabilized metal in two-dimensional frustrated Mott insulators
- Magnetic phase transition in disordered interacting Dirac fermion systems via the Zeeman field
- Dielectric response of the interacting 1D spinless fermions with disorder