Exact Free Energies of Statistical Systems on Random Networks
arXiv:1402.0740 · doi:10.3842/SIGMA.2014.087
Abstract
Statistical systems on random networks can be formulated in terms of partition functions expressed with integrals by regarding Feynman diagrams as random networks. We consider the cases of random networks with bounded but generic degrees of vertices, and show that the free energies can be exactly evaluated in the thermodynamic limit by the Laplace method, and that the exact expressions can in principle be obtained by solving polynomial equations for mean fields. As demonstrations, we apply our method to the ferromagnetic Ising models on random networks. The free energy of the ferromagnetic Ising model on random networks with trivalent vertices is shown to exactly reproduce that of the ferromagnetic Ising model on the Bethe lattice. We also consider the cases with heterogeneity with mixtures of orders of vertices, and derive the known formula of the Curie temperature.
References in corpus (1)
Cited by in corpus (11)
- Physical states in the canonical tensor model from the perspective of random tensor networks
- Symmetric configurations highlighted by collective quantum coherence
- Emergent symmetries in the canonical tensor model
- Equation of motion of canonical tensor model and Hamilton-Jacobi equation of general relativity
- A random matrix model with non-pairwise contracted indices
- Emergent classical geometries on boundaries of randomly connected tensor networks
- An extension of Canonical Tensor Model
- A Gaussian integral that counts regular graphs
- Tensors and Algebras: An Algebraic Spacetime Interpretation for Tensor Models
- Mother canonical tensor model
- Constraint algebra of general relativity from a formal continuum limit of canonical tensor model