This paper is concerned with Cauchy problems for the linear Schrödinger evolution equation (
i(∂/∂
t) + Δ + |
x –
a(
t)|
–1 +
V1(
x,
t))
u(
x,
t) =
f(
x,
t) in
RN × [0,
T], subject to initial condition:
u(·,0) ∈
H2(
RN) ∩
H2(
RN), where
i := $\sqrt{-1}$,
N ≥ 3,
T > 0 and
a : [0,
T] →
RN expresses the center of the Coulomb potential,
V1 and
f are another real-valued potential and an inhomogeneous term, respectively, while
H2(
RN) := {
v ∈
L2(
RN); |
x|
2v ∈
L2(
RN)}. We show that under some conditions on
V1 and
f the equation has a classical solution
u(·) ∈
C1([0,
T];
L2(
RN)) ∩
C([0,
T];
H2(
RN) ∩
H2(
RN)).
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