Continuous phase transitions with a convex dip in the microcanonical entropy
arXiv:cond-mat/0606283 · doi:10.1103/PhysRevE.74.011108
Abstract
The appearance of a convex dip in the microcanonical entropy of finite systems usually signals a first order transition. However, a convex dip also shows up in some systems with a continuous transition as for example in the Baxter-Wu model and in the four-state Potts model in two dimensions. We demonstrate that the appearance of a convex dip in those cases can be traced back to a finite-size effect. The properties of the dip are markedly different from those associated with a first order transition and can be understood within a microcanonical finite-size scaling theory for continuous phase transitions. Results obtained from numerical simulations corroborate the predictions of the scaling theory.
8 pages, 7 figures, to appear in Phys. Rev. E
References in corpus (3)
Cited by in corpus (6)
- Microcanonical Analyses of Peptide Aggregation Processes
- Thermodynamics of Peptide Aggregation Processes. An Analysis from Perspectives of Three Statistical Ensembles
- First-order transition features of the 3D bimodal random-field Ising model
- Microcanonical versus Canonical Analysis of Protein Folding
- First-order transition features of the triangular Ising model with nearest- and next-nearest-neighbor antiferromagnetic interactions
- On the application of the Critical Minimum Energy Subspace method to disordered systems