THE CONTINUOUS SPIN RANDOM FIELD MODEL: FERROMAGNETIC ORDERING IN d≥3
From MaRDI portal
Publication:4519826
DOI10.1142/S0129055X99000404zbMath1039.82019arXivmath-ph/9806010MaRDI QIDQ4519826
Publication date: 4 December 2000
Published in: Reviews in Mathematical Physics (Search for Journal in Brave)
Full work available at URL: https://arxiv.org/abs/math-ph/9806010
disordered systemsGibbs measuredouble-well potentialscluster expansionsweak disordercontour-representationlarge energy barriersrenormalizaton group
Interacting random processes; statistical mechanics type models; percolation theory (60K35) Disordered systems (random Ising models, random Schrödinger operators, etc.) in equilibrium statistical mechanics (82B44) Renormalization group methods in equilibrium statistical mechanics (82B28)
Related Items
Cites Work
- Rounding effects of quenched randomness on first-order phase transitions
- Cluster expansion for abstract polymer models
- Renormalization group pathologies and the definition of Gibbs states
- Dobrushin states for classical spin systems with complex interactions
- A low temperature expansion for classical \(N\)-vector models. I: A renormalization group flow
- Projections of Gibbs measures may be non-Gibbsian
- High temperature expansions and dynamical systems
- A low temperature expansion for classical \(N\)-vector models. II: Renormalization group equations
- Regularity properties and pathologies of position-space renormalization-group transformations: scope and limitations of Gibbsian theory
- A RIGOROUS RENORMALIZATION GROUP METHOD FOR INTERFACES IN RANDOM MEDIA
- Gibbs State Describing Coexistence of Phases for a Three-Dimensional Ising Model