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Nonequilibrium dynamic phase transition of an Ising spin system driven by various oscillating field
Author(s) -
Youxiang Shao,
Zhong Wei-Rong,
Lin Guang-Ming
Publication year - 2004
Publication title -
wuli xuebao
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.199
H-Index - 47
ISSN - 1000-3290
DOI - 10.7498/aps.53.3165
Subject(s) - sawtooth wave , physics , condensed matter physics , ising model , phase transition , non equilibrium thermodynamics , amplitude , critical point (mathematics) , transition point , field (mathematics) , quantum critical point , spin (aerodynamics) , quantum phase transition , quantum mechanics , thermodynamics , mathematical analysis , mathematics , computer science , pure mathematics , computer vision
We have studied both the dynamic response and the relevant nonequilibrium dynami cal p hase transition of an Ising spin system subject to three sorts of oscillating fi eld i.e. sinusoidal, square and sawtooth waves. The above three sorts of externa l field drive dynamically the Ising spin system in either simply gradual ( abrupt) way or their combination respectively. In the case of both sinusoidal and squar e ways, it was observed that the Ising spin system displays a low_temperature sy mmetr y-breaking ordered phase and a high_temperature symmetric disordered phase as well as the dynamic transition between two dynamical phases above. We also detected the tri_critical point separating high_temperature continuous dynamic transition and low_temperature discontinuous one on the boundary of dynamic transition. The trend of dynamic transition boundary and the dependence of tri_critical point upon the system temperature, the frequency and amplitude of the driving field we re revea led as well. In contrast, nodynamic transition occurs any longer and the system always stays in symmetry-breaking ordered state if the external field takes the form of sawtooth wave. The preceding discrepancy in dynamic response and transi tion is attributed to the perturbative characteristic of different oscillating f ields.

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