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2005年06月21日

【期刊论文】Phase transitions of the Ashkin-Teller model including antiferromagnetic interactions on a type of diamond hierarchical lattice

杨展如, Jian-Xin Le, , * and Z.R. Yang

PHYSICAL REVIEW E 69, 066107 (2004),-0001,():

-1年11月30日

摘要

Using the real-space renormalization-group transformation, we study the phase transitions of the Ashkin-Teller model including the antiferromagnetic interactions on a type of diamond hierarchical lattices, of which the number of bonds per branch of the generator is odd. The isotropic Ashkin-Teller model and the anisotropic one are, respectively, investigated. We find that the phase diagram, for the isotropic Ashkin-Teller model, consists of five phases, two of which are associated with the partially antiferromagnetic ordering of the system, while the phase diagram, for the anisotropic Ashkin-Teller model, contains 11 phases, six of which are related to the partially antiferromagnetic ordering of the system. The correlation length critical exponents and the crossover exponents are also calculated.

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2005年06月21日

【期刊论文】Phase transitions of the anisotropic Ashkin-Teller model on a family of diamond-type hierarchical lattices

杨展如, Jian-Xin Le, , * and Z.R. Yang

PHYSICAL REVIEW E 68, 066105 (2003),-0001,():

-1年11月30日

摘要

The phase transitions of the anisotropic Ashkin-Teller model on a family of diamond-type hierarchical lattices is studied by means of the transfer-matrix method and the real-space renormalization-group transformation. We find that the phase diagram, for the ferromagnetic case, consists of five phases, i.e., the fully disordered paramagnetic phase P, the fully ordered ferromagnetic phase F, and three partially ordered ferromagnetic phases Fs, F s, and Fs s, as well as ten nontrivial fixed points. The correlation length critical exponents and the crossover exponents are also calculated. In addition, we also investigate the variations of the critical exponents with the fractal dimension df, the number of branches m, and the number of bonds per branch b of the generator of the family of diamond-type hierarchical lattices. Finally we give a brief discussion about universality.

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2005年06月21日

【期刊论文】Multifractality of probability measure on energy-spectrum supports

杨展如, Z.R. Yang

PHYSICAL REVIEW E VOLUME 47, NUMBER 2 FEBRUARY 1993,-0001,():

-1年11月30日

摘要

We have studied quadric type energy (frequency) recursion relations resulting from fractal lattices. We found that the allowed energy intervals in successive levels form two similar two-scale Cantor sets. If WE imagine the iterating procedure as a dynamical process, the iterating results in different levels gen-erate a"time"sequence, and we can introduce an equal probability measure Pu on a Cantor set and con-struct,following Helsey et a1. [Phys. Rev. A 33, 1141 (1986)], a partition function F (q,T) =∑ipq/17; finally, we obtain Dq-q and f (a)-a curves. A number of exactly soluable examples are investigated.

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2005年06月21日

【期刊论文】Lacunarity and universality

杨展如, Ling Hao and Z R Yang

J. Phys. A: Math. Gen. 20 (1987) 1627-1631. Printed in the UK,-0001,():

-1年11月30日

摘要

Lacunarity as a criterion of universality in phase transitions on Sierpinski carpets is studied. The approximate theoretical and numerical results suggest that systems of different lacunarity may belong to a common universality class. There seems to be a lack of solutions to the complete set of universality criteria on Sierpinski carpets.

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2005年06月21日

【期刊论文】Kinetic phase transition of the three-state-vector Potts model

杨展如, Danmei Chen, Z.R. Yang

PHYSICAL REVIEW E VOLUME 49, NUMBER 17 I MAY 1994-I,-0001,():

-1年11月30日

摘要

We have studied the kinetic phase transition of a three-state-vector Potts system on a triangular lattice in contact with a heat bath and subject to an external energy source. The system evolves via the stochas-tic dynamics composed of Glauber and Kawasaki dynamics simulating interaction with the heat bath and energy source, respectively. The pair approximation IS used. It 1S found that there IS a paramagnetic-ferromagnetic transition at small energy flow, and the transition line is obtained. Also, when the energy is large enough, the system always will be in the paramagnetic state.

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  • 杨展如 邀请

    北京师范大学,北京

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