Removal
of telluric lines
Telluric lines disturbe more and more with increasing resolution
(R > 8000), but they are then also resolved and thus be eliminable in principle.
They are also included in low-resolution spectra, but they are not resolved
there. That is, in a broad H alpha line of a star, they are hidden and not resolved
and therefore cannot be eliminated. In this case we cannot remove in no way
the effects of the telluric lines from the measured spectrum.
The intensities (equivalent width W = area under a line in the normalized spectrum)
of the telluric lines are dependent on
- humidity in air (weather),
- the height of the object above the horizon (air mass),
- the height of the observer above sea level (air mass).
Therefore, professional spectrographs will be used on telescopes, which are
on high mountains in territories of low humidity (eg at the periphery of a desert).
The intensity ratio of water lines (abbreviated as WL) is constant among each
other. The same is true for the oxygen bands. If you have a model derived from
the practice range of telluric lines and folds it with the apparatus function
(in practice, by modeling a modifiable Gaussian function), we can apply the
theoretical spectrum as a normalization spectrum to the measured spectrum and
thus removes telluric lines - loosely speaking - we dehumidify the spectrum.
VSpec for
example, offers a tool that is operated with the mouse and is very intuitive.
For MIDAS,
I have a script that does this task with a command.
Link
to telluric lines webpage of C. Buil.
Examples:
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The graph on the left side shows the H alpha line from Mizar A. The bottom
spectrum with the sharp spikes of the water lines is measured. In the
upper spectrum the WL's are minimized to a few small remnants( using MIDAS).
The remnants are produced by
- Inaccuracies in the chosen (adopted) apparatus function,
- Inaccuracies in the calibration,
- The line profiles are not exaktly Gauss function like (blends).
In case of high standards of accuracy in the determination of the equivalent
widths (W), the telluric lines need to be eliminated, because they mimic
typically increased EW's by about 5%. The 5% is only a fist value. In
reality, it depends on the air humidity.
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Here is a second example:
The graph shows the used reference spectrum of the telluric lines
in a narrow wavelength window. This is the graphical interpretation of
a table of the ESO, which contains the wavelengths and relative intensities
of each line input.
Such a table of telluric lines is also implemented in VSpec (file H2O.dat).
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To use the above reference spectrum the 1-pixel sharp lines in the diagram
are transformed into Gaussian profiles. This occurs within MIDAS by a
function that is determined from the measured spectrum:
- One parameter is the measured FWHM of the water lines to be specified
by the user.
- The second parameter is an intensity factor (represents the observed
intensities of WL in the measured spectrum depending on air humidity
conditions).
The "theoretical" water lines are "shaped" that they coincide approximately
with the measured water lines. Exact is of course impossible, as measured
lines have only approximately a Gaussian profile.
Is shown on the leftside the tailored reference spectrum to an individual
spectrum. It shows the theoretical spectrum now as if I had measured it
at a star, which itself has a normalized continuum with no own photospheric
lines, so that only the telluric lines would be measured.
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Left, a measured spectrum of eps Aur is shown (black line). In this above
adaptive reference spectrum was used (standardization). The result is
in red. The water lines are significantly reduced. The remaining residues
would play in a EW calculation not matter anymore.
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