Dynamical real-space renormalization group calculations with a new clustering scheme on random networks
arXiv:cond-mat/0408619 · doi:10.1103/PhysRevE.71.026130
Abstract
We have defined a new type of clustering scheme preserving the connectivity of the nodes in network ignored by the conventional Migdal-Kadanoff bond moving process. Our new clustering scheme performs much better for correlation length and dynamical critical exponents in high dimensions, where the conventional Migdal-Kadanoff bond moving scheme breaks down. In two and three dimensions we find the dynamical critical exponents for the kinetic Ising Model to be z=2.13 and z=2.09, respectively at pure Ising fixed point. These values are in very good agreement with recent Monte Carlo results. We investigate the phase diagram and the critical behaviour for randomly bond diluted lattices in d=2 and 3, in the light of this new transformation. We also provide exact correlation exponent and dynamical critical exponent values on hierarchical lattices with power-law degree distributions, both in the pure and random cases.
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References in corpus (10)
- Evolution of networks
- Regularity Properties and Pathologies of Position-Space Renormalization-Group Transformations
- Critical exponents of the three dimensional diluted Ising model
- Dynamic Monte Carlo Measurement of Critical Exponents
- The Dynamic Exponent of the Two-Dimensional Ising Model and Monte Carlo Computation of the Sub-Dominant Eigenvalue of the Stochastic Matrix
- Self-Averaging, Distribution of Pseudo-Critical Temperatures and Finite Size Scaling in Critical Disordered Systems
- Bond dilution in the 3D Ising model: a Monte Carlo study
- The Harris-Luck criterion for random lattices
- Harris criterion on hierarchical lattices: Rigorous inequalities and counterexamples in Ising systems
- Random bond Ising systems on a general hierarchical lattice: Exact inequalities