Author:
Bambusi Dario,Gérard Patrick
Abstract
AbstractWe consider a perturbation of the Benjamin Ono equation with periodic boundary conditions on a segment. We consider the case where the perturbation is Hamiltonian and the corresponding Hamiltonian vector field is analytic as a map from the energy space to itself. Let $$\epsilon $$
ϵ
be the size of the perturbation. We prove that for initial data close in energy norm to an N-gap state of the unperturbed equation all the actions of the Benjamin Ono equation remain $${\mathcal {O}}(\epsilon ^{\frac{1}{2(N+1)}})$$
O
(
ϵ
1
2
(
N
+
1
)
)
close to their initial value for times exponentially long with $$\epsilon ^{-\frac{1}{2(N+1)}}$$
ϵ
-
1
2
(
N
+
1
)
.
Funder
Università degli Studi di Milano
Publisher
Springer Science and Business Media LLC
Cited by
1 articles.
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