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Published on: June 7, 2018
Percolation of Fortuin-Kasteleyn clusters for the random-bond Ising model
Hauke Fajen1, Alexander K Hartmann1, A P Young2
1Institut für Physik, Universität Oldenburg, 26111 Oldenburg, Germany.
We studied the 3D ±1 random-bond Ising model using cluster algorithms. The Fortuin-Kasteleyn percolation transition occurs above the magnetic ordering temperature for most bond concentrations, indicating universality.
Area of Science:
- Statistical Mechanics
- Condensed Matter Physics
- Computational Physics
Background:
- The 3D ±1 random-bond Ising model exhibits complex magnetic behavior dependent on temperature and antiferromagnetic bond concentration.
- Ground states transition from ferromagnetic to spin-glass phases at a critical concentration p_c ≈ 0.222.
- Understanding phase transitions and universality classes is crucial in statistical physics.
Purpose of the Study:
- To investigate the percolation transition of Fortuin-Kasteleyn clusters in the 3D ±1 random-bond Ising model.
- To determine the relationship between the percolation transition temperature and the magnetic ordering temperature.
- To analyze the universality of the percolation transition across different ground states and bond concentrations.
Main Methods:
- Application of generalized Swendson-Wang and Wolff cluster algorithms.
- Construction of Fortuin-Kasteleyn clusters.
- Simulations performed on large system sizes up to N=200^3 spins.
Main Results:
- The Fortuin-Kasteleyn percolation transition temperature consistently exceeds the magnetic ordering temperature for p > 0.
- Evidence suggests this difference exists even for small concentrations of negative bonds.
- For p > 0, the percolation transition appears universal and belongs to the standard percolation universality class, regardless of ground state order.
Conclusions:
- Fortuin-Kasteleyn cluster percolation is generally distinct from magnetic ordering in this model.
- Bond occupancy correlations within clusters are irrelevant for universality, except at p=0.
- At p=0, the percolation transition aligns with the Ising universality class due to direct ties to Ising correlations.
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