Stationary states and fractional dynamics in systems with long range interactions
arXiv:0912.3060 · doi:10.1209/0295-5075/89/50010
Abstract
Dynamics of many-body Hamiltonian systems with long range interactions is studied, in the context of the so called HMF model. Building on the analogy with the related mean field model, we construct stationary states of the HMF model for which the spatial organization satisfies a fractional equation. At variance, the microscopic dynamics turns out to be regular and explicitly known. As a consequence, dynamical regularity is achieved at the price of strong spatial complexity, namely a microscopic inhomogeneity which locally displays scale invariance.
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- Existence of Quasi-stationary states at the Long Range threshold
- Action diffusion and lifetimes of quasistationary states in the Hamiltonian Mean Field model
- Emergence of a non trivial fluctuating phase in the XY model on regular networks
- Crafting networks to achieve, or not achieve, chaotic states
- Emergence of a collective crystal in a classical system with long-range interactions
- Full Self-Consistent Vlasov-Maxwell Solution