TY - JOUR
T1 - Phase diagram of an Ising model with competitive interactions on a Husimi tree and its disordered counterpart
AU - Ostilli, M.
AU - Mukhamedov, F.
AU - Mendes, J. F.F.
N1 - Funding Information:
This work was supported by the FCT (Portugal) grants SFRH/BPD/17419/2004, SFRH/BPD/24214/2005, pocTI/FAT/46241/2002 and pocTI/FAT/46176/2003, and the Dysonet Project. We thank A.V. Goltsev and M. Hase, for many useful discussions and a critical reading of the manuscript.
PY - 2008/5/1
Y1 - 2008/5/1
N2 - We consider an Ising competitive model defined over a triangular Husimi tree where loops, responsible for an explicit frustration, are even allowed. We first analyze the phase diagram of the model with fixed couplings in which a "gas of noninteracting dimers (or spin liquid) - ferro or antiferromagnetic ordered state" zero temperature transition is recognized in the frustrated regions. Then we introduce the disorder for studying the spin glass version of the model: the triangular ± J model. We find out that, for any finite value of the averaged couplings, the model exhibits always a finite temperature phase transition even in the frustrated regions, where the transition turns out to be a glassy transition. The analysis of the random model is done by applying a recently proposed method which allows us to derive the critical surface of a random model through a mapping with a corresponding nonrandom model.
AB - We consider an Ising competitive model defined over a triangular Husimi tree where loops, responsible for an explicit frustration, are even allowed. We first analyze the phase diagram of the model with fixed couplings in which a "gas of noninteracting dimers (or spin liquid) - ferro or antiferromagnetic ordered state" zero temperature transition is recognized in the frustrated regions. Then we introduce the disorder for studying the spin glass version of the model: the triangular ± J model. We find out that, for any finite value of the averaged couplings, the model exhibits always a finite temperature phase transition even in the frustrated regions, where the transition turns out to be a glassy transition. The analysis of the random model is done by applying a recently proposed method which allows us to derive the critical surface of a random model through a mapping with a corresponding nonrandom model.
KW - Competing Ising models
KW - Glass transition
KW - Husumi trees
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U2 - 10.1016/j.physa.2008.01.071
DO - 10.1016/j.physa.2008.01.071
M3 - Article
AN - SCOPUS:40249102979
SN - 0378-4371
VL - 387
SP - 2777
EP - 2792
JO - Physica A: Statistical Mechanics and its Applications
JF - Physica A: Statistical Mechanics and its Applications
IS - 12
ER -