Finite-Size Effects in Disordered Model
arXiv:1510.02038 · doi:10.1142/S0217979216502076
Abstract
We discuss finite-size effects in one disordered model defined in a -dimensional Euclidean space. We consider that the scalar field satisfies periodic boundary conditions in one dimension and it is coupled with a quenched random field. In order to obtain the average value of the free energy of the system we use the replica method. We first discuss finite-size effects in the one-loop approximation in and . We show that in both cases there is a critical length where the system develop a second-order phase transition, when the system presents long-range correlations with power-law decay. Next, we improve the above result studying the gap equation for the size- dependent squared mass, using the composite field operator method. We obtain again, that the system present a second order phase transition with long-range correlation with power-law decay.
19 pages, 4 figures
References in corpus (10)
- Quantum field theory on toroidal topology: algebraic structure and applications
- Analog model for quantum gravity effects: phonons in random fluids
- Finite size corrections to disordered Ising models on Random Regular Graphs
- Finite size corrections to disordered systems on Erdös-Rényi random graphs
- No spin glass phase in ferromagnetic random-field random-temperature scalar Ginzburg-Landau model
- Thermal Radiation from a Fluctuating Event Horizon
- Accelerated detectors in Dirac vacuum: the effects of horizon fluctuations
- Scalar Quantum Field Theory in Disordered Media
- Random field and random anisotropy O(N) spin systems with a free surface
- Casimir Energy Corrections by Light-Cone Fluctuations