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Systematic uncertainty in the silicate strength
It is important to keep in mind that the main uncertainty in the
silicate strength may not be the statistical uncertainty, which may
be as low as 0.01 in silicate strength for a spectrum with very
high S/N. Instead the dominant uncertainty may be systematic in
nature, associated with the choice of interpolation method (spline
or powerlaw continuum), or from the need to invoke deblendIRS.
To quantify the systematic uncertainty we have plotted the
difference of the silicate strength solutions from both methods
in the figure below. The difference is close to zero wherever
the color is yellow. Where it tends to red the silicate strength
from the spline method exceeds the one from the powerlaw method.
Where the color tends to green, blue or purple the silicate
strength from the powerlaw method is larger.
The power law method is prefered for spectra dominated by PAH
emission, which are characterized by S_sil_powerlaw > -2 and
EQW(PAH11)>0.1µm. See the box defined by the dashed lines.
To explore the systematic uncertainty in the silicate strength
we compare the silicate strength solutions for both methods at
the boundary of the two validity ranges.
Galaxies with power law based silicate strengths between -1.8 and
-2.2 and EQW(PAH11)>0.1µm show a median systematic difference between
spline and powerlaw based silicate strengths of -0.21. The 1-sigma
dispersion of the measurements is 0.19. The large majority of
measurements agree to within their uncertainty with the median silicate
strength difference of -0.21.
Galaxies with EQW(PAH11) between 0.1/1.2µm and 0.1x1.2µm and
with a power law silicate strength > -2 show a median systematic
difference between the spline and power law based silicate strengths
of zero, with a 1-sigma dispersion of 0.18.
Based on the above results obtained along the two boundary regions
between power law based and spline based silicate strengths
we deem the systematic difference in the silicate strength to be
0.2.