4.1.17. Etau: simple transmission model¶
This model calculates the transmission between energies
and
for a simple (often unphysical!) case:
with the optical depth given by:
In addition, we put here for
and
, where
and
are adjustable
parameters. This allows the user for example to mimick an edge. Note
however, that in most circumstances there are more physical models
present in SPEX that contain realistic transmissions of edges! If you do
not want or need edges, simply keep
and
at their
default values.
Note that should be non-negative. For
the
spectrum has a high-energy cut-off, for
it has a low-energy
cut-off, and for
the transmission is flat. The larger the
value of
, the sharper the cut-off is.
The model can be used as a basis for more complicated continuum
absorption models. For example, if the optical depth is given as a
polynomial in the photon energy , say for example
, one may define three etau components,
with
values of 2, 3, and 4, and indices
of 0, 1
and 2. This is because of the mathematical identity
.
The parameters of the model are:
- tau0:
Optical depth
at
keV. Default value: 1.
- a:
The index
defined above. Default value: 1.
- e1:
Lower energy
(keV). Default value:
.
- e2:
Upper energy
(keV). Default value:
.
- icov:
Type of the covering fraction. Default value: 2 (constant, set by fcov). If icov=1, full covering is applied. If icov=3, covering fraction follows a tangent function that increases with energy. If icov=4, covering fraction follows an inverse tangent function that decreases with energy. See description in
pion.- fcov:
The covering factor of the absorber if icov=2. Default value: 1 (full covering). If icov=3 or 4, it sets the covering factor at the high energy end.
- lcov:
The covering factor of the absorber at the low energy end. Default value: 1. lcov is applied only when icov=3 or 4. See description in
pion.- ecov:
The energy when the covering factor changes from lcov to fcov. Only applied if icov=3 or 4.
- acov:
The width of the transit on covering factor. Only applied if icov=3 or 4.