Monte Carlo Renormalization Group Method to Study the First-Order Phase Transition in the Complex Ferromagnet
An improved Monte Carlo renormalization group method is established. Based on a new model, as well as the generalized G1auber dynamics, the first-order phase transition is studied in the Erd6s-Rgnyi network, which is used to represent the complex ferromagnet. Both static and dynamic critical exponen...
Saved in:
Published in | Chinese physics letters Vol. 32; no. 12; pp. 5 - 8 |
---|---|
Main Author | |
Format | Journal Article |
Language | English |
Published |
Chinese Physical Society and IOP Publishing
01.12.2015
|
Subjects | |
Online Access | Get full text |
ISSN | 0256-307X 1741-3540 |
DOI | 10.1088/0256-307X/32/12/120501 |
Cover
Summary: | An improved Monte Carlo renormalization group method is established. Based on a new model, as well as the generalized G1auber dynamics, the first-order phase transition is studied in the Erd6s-Rgnyi network, which is used to represent the complex ferromagnet. Both static and dynamic critical exponents can be evaluated simultaneously, and the static critical exponents are evaluated to be independent of the dimension of the system. Thus by using the hyperscaling relation vd* = 2 - ~, the effective dimension d* of complex networks can be found. |
---|---|
Bibliography: | 11-1959/O4 An improved Monte Carlo renormalization group method is established. Based on a new model, as well as the generalized G1auber dynamics, the first-order phase transition is studied in the Erd6s-Rgnyi network, which is used to represent the complex ferromagnet. Both static and dynamic critical exponents can be evaluated simultaneously, and the static critical exponents are evaluated to be independent of the dimension of the system. Thus by using the hyperscaling relation vd* = 2 - ~, the effective dimension d* of complex networks can be found. MENG Qing-Kuan, FENG Dong-Tai, GAO Xu-Tuan(School of Science, Shandong University of Technology, Zibo 255049) |
ISSN: | 0256-307X 1741-3540 |
DOI: | 10.1088/0256-307X/32/12/120501 |