Dynamics of systems with isotropic competing interactions in an external field: a Langevin approach
arXiv:1011.5137 · doi:10.1140/epjb/e2011-20185-y
Abstract
We study the Langevin dynamics of a ferromagnetic Ginzburg-Landau Hamiltonian with a competing long-range repulsive term in the presence of an external magnetic field. The model is analytically solved within the self consistent Hartree approximation for two different initial conditions: disordered or zero field cooled (ZFC), and fully magnetized or field cooled (FC). To test the predictions of the approximation we develop a suitable numerical scheme to ensure the isotropic nature of the interactions. Both the analytical approach and the numerical simulations of two-dimensional finite systems confirm a simple aging scenario at zero temperature and zero field. At zero temperature a critical field is found below which the initial conditions are relevant for the long time dynamics of the system. For a logarithmic growth of modulated domains is found in the numerical simulations but this behavior is not captured by the analytical approach which predicts a growth law at .
References in corpus (5)
- Structural and dynamical features of multiple metastable glassy states in a colloidal system with competing interactions
- Pattern formation and glassy phase in the theory with screened electrostatic repulsion
- Fluctuations in the coarsening dynamics of the O(N) model: are they similar to those in glassy systems?
- Langevin simulations of a model for ultrathin magnetic films
- Langevin dynamics of fluctuation induced first order phase transitions: self consistent Hartree Approximation
Cited by in corpus (4)
- Nature of Long-Range Order in Stripe-Forming Systems with Long-Range Repulsive Interactions
- On the mechanism behind the inverse melting in systems with competing interactions
- Melting of the two-dimensional solid phase in the Gaussian-core model
- The frustrated spherical model: an alternative to Ginzburg-Landau Hamiltonians with competing interactions