Abstract
The semiclassical limit of a weakly coupled nonlinear focusing Schrödinger system in presence of a nonconstant potential is studied. The initial data is of the form (u1, u2) with ui=ri ((x−x˜)/ε)e(i/ε)x·ξ˜, where (r1, r2) is a real ground state solution, belonging to a suitable class, of an associated autonomous elliptic system. For ε sufficiently small, the solution (ϕ1, ϕ2) will been shown to have, locally in time, the form (r1 ((x−x(t))/ε)e(i/ε)x·ξ(t), r2 ((x−x(t))/ε)e(i/ε)x·ξ(t)), where (x(t), ξ(t)) is the solution of the Hamiltonian system x˙(t)=ξ(t), ξ˙(t)=−∇V(x(t)) with x(0)=x˜ and ξ(0)=ξ˜.
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