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Volumn 81, Issue 1, 2010, Pages

Majority-vote model on hyperbolic lattices

Author keywords

[No Author keywords available]

Indexed keywords

BOUNDARY NODES; COMPARATIVE STUDIES; CRITICAL EXPONENT; CRITICAL PROPERTIES; CURVED SURFACES; EFFECTIVE DIMENSIONS; FINITE SIZE ANALYSIS; HYPERSCALING RELATIONS; MAJORITY-VOTE MODEL; MONTE CARLO SIMULATION; NON EQUILIBRIUM; ORDERING PROCESS; PERIODIC BOUNDARY CONDITIONS; REGULAR LATTICE; STATISTICAL MODELS; UNIVERSALITY CLASS;

EID: 76249122217     PISSN: 15393755     EISSN: 15502376     Source Type: Journal    
DOI: 10.1103/PhysRevE.81.011133     Document Type: Article
Times cited : (59)

References (34)
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    • Note that to facilitate comparisons we select the lattice size N as the scaling variable rather than the more common linear dimension L for the Ising model. If we measure the critical exponents in terms of L instead of N= L2, then 1/ν=1 and β/ν=0.125.
    • Note that to facilitate comparisons we select the lattice size N as the scaling variable rather than the more common linear dimension L for the Ising model. If we measure the critical exponents in terms of L instead of N= L2, then 1/ν=1 and β/ν=0.125.
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    • The local configuration energy in Ref. is defined as E [σi] =- σi S (j Ωi σj), where S (x) and Ωi are the same as defined in Eq. 1. The global configuration energy is obtained from summing the local configuration energy over all the sites.
    • The local configuration energy in Ref. is defined as E [σi] =- σi S (j Ωi σj), where S (x) and Ωi are the same as defined in Eq.1. The global configuration energy is obtained from summing the local configuration energy over all the sites.


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