continuous perturbation
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Author(s):  
Benoit Pausader ◽  
Klaus Widmayer

AbstractWe consider the Vlasov–Poisson system with repulsive interactions. For initial data a small, radial, absolutely continuous perturbation of a point charge, we show that the solution is global and disperses to infinity via a modified scattering along trajectories of the linearized flow. This is done by an exact integration of the linearized equation, followed by the analysis of the perturbed Hamiltonian equation in action-angle coordinates.


Author(s):  
Guy Vallet ◽  
Aleksandra Zimmermann

Abstract We consider the well-posedness of a stochastic evolution problem in a bounded Lipschitz domain D ⊂ ℝ d with homogeneous Dirichlet boundary conditions and an initial condition in L2(D). The main technical difficulties in proving the result of existence and uniqueness of a solution arise from the nonlinear diffusion-convection operator in divergence form which is given by the sum of a Carathéodory function satisfying p-type growth associated with coercivity assumptions and a Lipschitz continuous perturbation. In particular, we consider the case 1 < p < 2 with an appropriate lower bound on p determined by the space dimension. Another difficulty arises from the fact that the additive stochastic perturbation with values in L2(D) on the right-hand side of the equation does not inherit the Sobolev spatial regularity from the solution as in the multiplicative noise case.


2020 ◽  
Vol 9 (1) ◽  
pp. 27-38
Author(s):  
Doria Affane ◽  
◽  
Meriem Aissous ◽  
Mustapha Fateh Yarou

PLoS ONE ◽  
2016 ◽  
Vol 11 (11) ◽  
pp. e0165735 ◽  
Author(s):  
Carolyn A. Duncan ◽  
Tony G. J. Ingram ◽  
Avril Mansfield ◽  
Jeannette M. Byrne ◽  
William E. McIlroy

1993 ◽  
Vol 48 (5-6) ◽  
pp. 629-632 ◽  
Author(s):  
K. Pyragas

Abstract The methods of stabilization of unstable periodic and aperiodic orbits of a strange attractor with the help of a small time-continuous perturbation are discussed. The perturbation is applied to the system in such a way that the desired periopdic or aperiodic orbits remain unperturbed. An experimental application of the methods can be carried out by a purely analogous technique without use of any computer.


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