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Elusive spin-glass phase in the random field Ising model
Florent Krzakala1, Federico Ricci-Tersenghi, Lenka Zdeborová
1CNRS and ESPCI ParisTech, 10 rue Vauquelin, UMR 7083 Gulliver, Paris 75000 France.
In equilibrium, the random field Ising model cannot have a spin-glass phase. However, a spin-glass phase can emerge when magnetization is fixed below equilibrium values, as demonstrated on the Bethe lattice.
Area of Science:
- Statistical Mechanics
- Condensed Matter Physics
- Disordered Systems
Background:
- The random field Ising model (RFIM) is a fundamental model in statistical mechanics used to study disordered magnetic systems.
- Understanding the conditions for the emergence of different phases, such as ferromagnetic and spin-glass phases, is crucial for characterizing magnetic materials.
Purpose of the Study:
- To rigorously investigate the existence of a spin-glass phase in the random field Ising model under equilibrium conditions.
- To explore the possibility of a spin-glass phase when the system's magnetization is externally controlled.
Main Methods:
- Rigorous mathematical analysis of the spin-glass susceptibility in the RFIM.
- Explicit demonstration of a spin-glass phase on the Bethe lattice for fixed magnetization values.
Main Results:
- The spin-glass susceptibility is rigorously shown to be bounded by the ferromagnetic susceptibility in equilibrium.
- This implies that no equilibrium spin-glass phase can exist outside the ferromagnetic critical line.
- A spin-glass phase is explicitly shown to exist on the Bethe lattice when magnetization is fixed below its equilibrium value.
Conclusions:
- The equilibrium phase diagram of the RFIM is constrained, preventing spin-glass phases away from the ferromagnetic critical line.
- The study highlights the importance of boundary conditions and external control in potentially stabilizing exotic phases like spin-glasses in disordered systems.
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