Conditions for predicting quasistationary states by rearrangement formula
arXiv:1411.6750 · doi:10.1103/PhysRevE.92.042131
Abstract
Predicting the long-lasting quasistationary state for a given initial state is one of central issues in Hamiltonian systems having long-range interaction. A recently proposed method is based on the Vlasov description and uniformly redistributes the initial distribution along contours of the asymptotic effective Hamiltonian, which is defined by the obtained quasistationary state and is determined self-consistently. The method, to which we refer as the rearrangement formula, was suggested to give precise prediction under limited situations. Restricting initial states consisting of spatially homogeneous part and small perturbation, we numerically reveal two conditions that the rearrangement formula prefers: One is no Landau damping condition for unperturbed homogeneous part, and the other comes from the Casimir invariants. Mechanisms of these conditions are discussed. Clarifying these conditions, we inform validity to use the rearrangement formula as the response theory for an external field, and we shed light on improving the theory as a nonequilibrium statistical mechanics.
11pages, 4 figures
References in corpus (7)
- Statistical mechanics and dynamics of solvable models with long-range interactions
- Diverging equilibration times in long-range quantum spin models
- Collisionless relaxation in gravitational systems: From violent relaxation to gravothermal collapse
- Core-halo distribution in the Hamiltonian Mean-Field Model
- Statistical Mechanics of Unbound Two Dimensional Self-Gravitating Systems
- Nonequilibrium stationary states of 3D self-gravitating systems
- Out of Equilibrium Solutions in the -Hamiltonian Mean Field model
Cited by in corpus (5)
- Strange Scaling and Temporal Evolution of Finite-Size Fluctuation in Thermal Equilibrium
- Collective fluctuation by pseudo-Casimir-invariants
- Discontinuous codimension-two bifurcation in a Vlasov equation
- Quantum fluctuations inhibit symmetry breaking in the HMF model
- Nondivergent and negative susceptibilities around critical points of a long-range Hamiltonian system with two order parameters