Treating unbound states¶
Identifying unbound states¶
Unbound states appear above the state dissociations. The Duo is developed to treat bound state problems
with an effective boundary condition for the rovibronic eigenfunctions to vanish at the borders of the simulation grid.
However it is a typical problem when an electronic system contans unbound region between states or above their dissociations,
where unboud solutions are possible. Moreover, some of these unbound eigenfunctions are exactly zero at
(other side is automatically zero duo to the steep repulsive wall).
Duo methodology can be applied also to compute the unbound spectra, here we show how to remove the spurious unbound states from the spectra (line lists)
calculations and thus to produce bound a line list. The unbound wavefunctions
can be identified based on their asymptotic properties
via non-zero density in the small region of
at the right border
:
is a small threshold value. The default threshold value is
is chosen as
.
The threshold value can be specified in the input file using the keyword thresh_bound.
Excluding unbound states¶
Once the unboud states are identified they can be excluded from the intensity or line list calculations using the bound keyword in the INTENSITY section, which tells Duo to compute boud-bound spectra only, e.g.:
Example:
intensity
absorption
bound
thresh_intes 1e-50
thresh_bound 1e-6
temperature 3000 (K)
nspin 2.5 1.5
linelist AlCl-37_61_J160
J 0, 20
freq-window 0.0 48000.0
energy low 0.0 30000, upper 0.0,48000
end
Excluding bound upper states¶
Sometimes only the transitions to the unbound state are needed. In this case we exclude tansitions to the upper bound states with a keyword unbound placed anywehere in the INTENSITY section.
Example:
intensity
absorption
unbound
thresh_intes 1e-50
thresh_bound 1e-6
temperature 3000 (K)
nspin 2.5 1.5
linelist AlCl-37_61_J160
J 0, 20
freq-window 0.0 48000.0
energy low 0.0 30000, upper 0.0,48000
end