Laburpena
In space dimension n>=3, we consider the electromagnetic Schrödinger hamiltonian H =
(∇ − i A(x))2 − V and the corresponding Helmholtz equation
(∇ − i A(x))2u + u − V (x)u = f in Rn.
We extend the well-known L p –L q estimates for the solution of the free Helmholtz equation
to the case when the electromagnetic hamiltonian H is considered.