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Published on: May 15, 2017
Phase transition properties of the Bell-Lavis model
M Šimėnas1, A Ibenskas1, E E Tornau1
1Semiconductor Physics Institute, Center for Physical Sciences and Technology, Goštauto 11, LT-01108 Vilnius, Lithuania.
Monte Carlo calculations reveal phase transitions in a triangular antiferromagnetic model. Most transitions align with the three-state Potts universality class, except at phase boundaries where first-order transitions or crossovers occur.
Area of Science:
- Statistical Mechanics
- Condensed Matter Physics
- Computational Physics
Background:
- The study investigates phase transitions in a triangular antiferromagnetic three-state Bell-Lavis model.
- Understanding the order and universality classes of these transitions is crucial for characterizing complex magnetic systems.
Purpose of the Study:
- To analyze the order and universality class of phase transitions into the low-density honeycomb phase.
- To determine the behavior of these transitions across a range of chemical potentials.
- To compare the model's behavior with related models like the Blume-Capel model.
Main Methods:
- Utilizing Monte Carlo calculations to simulate the model.
- Analyzing the behavior of the system across a range of chemical potentials (μ).
- Identifying the universality class of the observed phase transitions.
Main Results:
- Phase transitions are primarily attributed to the three-state Potts universality class for most chemical potentials.
- Transitions become first-order at the boundary between the honeycomb and low-density gas phases.
- A crossover from three-state Potts to Ising universality class is observed at the honeycomb-to-frustrated phase boundary.
- A Schottky anomaly in specific heat is detected near this boundary.
- The intermediate planar phase observed in the Blume-Capel model is absent in the Bell-Lavis model.
Conclusions:
- The Bell-Lavis model exhibits complex phase transition behavior, predominantly following the three-state Potts universality class.
- Specific phase boundaries lead to deviations, including first-order transitions and crossovers to Ising universality.
- The absence of an intermediate planar phase distinguishes it from the similar Blume-Capel model.
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