Critical behavior of the Coulomb-glass model in the zero-disorder limit: Ising universality in a system with long-range interactions

Abstract

The ordering of charges on half-filled hypercubic lattices is investigated numerically, where electroneutrality is ensured by background charges. This system is equivalent to the $s=1/2$ Ising lattice model with antiferromagnetic $1/r$ interaction. The temperature dependences of specific heat, mean staggered occupation, and of a generalized susceptibility indicate continuous order-disorder phase transitions at finite temperatures in two- and three-dimensional systems. In contrast, the susceptibility of the one-dimensional system exhibits singular behavior at vanishing temperature. For the two- and three-dimensional cases, the critical exponents are obtained by means of a finite-size scaling analysis. Their values are consistent with those of the Ising model with short-range interaction, and they imply that the studied model cannot belong to any other known universality class. Samples of up to 1400, $112^2$, and $22^3$ sites are considered for dimensions 1 to 3, respectively.

revtex-file + 14 figures -> 10 pages; two references added, typos corrected

References in corpus (4)

• Mean field theory for the three-dimensional Coulomb glass
• Critical Binder cumulant of two-dimensional Ising models
• Density of States and Critical Behavior of the Coulomb Glass
• Ising analogue to compact-star matter

Cited by in corpus (4)

• Griffiths-McCoy singularity on the diluted Chimera graph: Monte Carlo simulations and experiments on the quantum hardware
• Effect of increasing disorder on domains of the two-dimensional Coulomb glass
• Charge ordering in the three-dimensional Coulomb glass at finite temperatures and low disorders
• Phase Ordering Kinetics of the Asymmetric Coulomb Glass Model