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Xavier Andrade edited figures/mask_scheme1/caption.tex
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\label{fig:pes_sheme}
Scheme illustrating the mask method for the calculation of electron photoemission.
A mask function (a) is used to effectively split each Kohn-Sham orbital into bounded and
an unbounded
components localized in different spatial regions $A$ and $B$ according to the diagram in (b).
In $A$ the states are represented on a real-space grid while in $B$ they are described in momentum space.
A striped region indicates the volume where the two representations overlap.
The propagation scheme of
eqs~\eqref{eq:FMM_prop} and \eqref{eq:FMM_prop_aux} eqs.~\eqref{eq:FMM_prop} and~\eqref{eq:FMM_prop_aux} allows seamless transitions from one representations to the other and
is capable to describe electrons following closed trajectories like the one in (b).