Abstract
We obtain a solution of the time-dependent Schrödinger equation for
a two-electron system confined to a plane by an isotropic parabolic
potential whose curvature is periodically modulated in time. From
this solution we compute the “exact” time-dependent exchange correlation
potential vxc, which enters the Kohn-Sham equation of time-dependent
density functional theory. Our “exact” result provides a benchmark
against which various approximate forms for vxc can be compared.
Finally, vxc is separated in an adiabatic and a pure dynamical part
and it is shown that, for the particular system studied, the dynamical
part is negligible.
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