Condensation of helium in aerogels and athermal dynamics of the Random Field Ising Model
arXiv:1309.1243 · doi:10.1103/PhysRevLett.113.085301
Abstract
High resolution measurements reveal that condensation isotherms of He in a silica aerogel become discontinuous below a critical temperature. We show that this behaviour does not correspond to an equilibrium phase transition modified by the disorder induced by the aerogel structure, but to the disorder-driven critical point predicted for the athermal out-of-equilibrium dynamics of the Random Field Ising Model. Our results evidence the key role of non-equilibrium effects in the phase transitions of disordered systems.
5 p + suppl. material
References in corpus (15)
- Crackling Noise
- Hysteresis and hierarchies: dynamics of disorder-driven first-order phase transformations
- Capillary condensation in disordered porous materials: hysteresis versus equilibrium behavior
- Avalanches, Barkhausen Noise, and Plain Old Criticality
- Disorder-Induced Critical Phenomena in Hysteresis: Numerical Scaling in Three and Higher Dimensions
- Universality in the three-dimensional random-field Ising model
- Local mean-field study of capillary condensation in silica aerogels
- Elusive Glassy Phase in the Random Field Ising Model
- Helium condensation in aerogel: avalanches and disorder-induced phase transition
- Disorder induced critical phenomena in magnetically glassy Cu-Al-Mn alloys
- Helium adsorption in silica aerogel near the liquid-vapor critical point
- Evidence for a disorder driven phase transition in the condensation of 4He in aerogels
- A temperature-controlled device for volumetric measurements of Helium adsorption in porous media
- Fluids in porous media: The case of neutral walls
- Critical behavior of the liquid gas transition of 4 He confined in a silica aerogel
Cited by in corpus (4)
- Spinodals with Disorder: from Avalanches in Random Magnets to Glassy Dynamics
- Finite-dimensional vestige of spinodal criticality above the dynamical glass transition
- Thermal vestiges of avalanches in the driven random field Ising model
- Inverse transitions and disappearance of the λ-line in the asymmetric random field Ising and Blume-Capel models