Here we describe the 80 IDEOS observables that are available for the
targets in the IDEOS galaxy sample. Most quantities have an
uncertainty associated with them, which is provided in a variable
OBSERVABLE_ERR. Similarly, there may be an associated flag denoting
a detection (0), upper limit (+1), lower limit (+2), or the lack of
a measurement (-1). This value would be stored in the variable OBSERVABLE_FLAG.
Line fluxes of
forbidden lines |
Observable |
Description |
Unit |
AR2FLUX | Integrated flux of the 6.99µm [Ar II] emission line | 10-21 W/cm2 |
AR3FLUX | Integrated flux of the 8.99µm [Ar III] emission line | 10-21 W/cm2 |
S4FLUX | Integrated flux of the 10.51µm [S IV] emission line | 10-21 W/cm2 |
NE2FLUX | Integrated flux of the 12.81µm [Ne II] emission line | 10-21 W/cm2 |
NE5_14FLUX | Integrated flux of the 14.32µm [Ne V] emission line | 10-21 W/cm2 |
CL2FLUX | Integrated flux of the 14.37µm [Cl II] emission line | 10-21 W/cm2 |
NE3_15FLUX | Integrated flux of the 15.56µm [Ne III] emission line | 10-21 W/cm2 |
S3_18FLUX | Integrated flux of the 18.71µm [S III] emission line | 10-21 W/cm2 |
NE5_24FLUX | Integrated flux of the 24.32µm [Ne V] emission line | 10-21 W/cm2 |
O4FLUX | Integrated flux of the 25.89µm [O IV] emission line | 10-21 W/cm2 |
FE2FLUX | Integrated flux of the 25.99µm [Fe II] emission line | 10-21 W/cm2 |
S3_33FLUX | Integrated flux of the 33.48µm [S III] emission line | 10-21 W/cm2 |
SI2FLUX | Integrated flux of the 34.82µm [Si II] emission line | 10-21 W/cm2 |
NE3_36FLUX | Integrated flux of the 36.01µm [Ne III] emission line | 10-21 W/cm2 |
Line ratio of
forbidden lines |
Observable |
Description |
Unit |
AR3AR2RATIO | Ratio of the 8.99µm [Ar III] to the 6.99µm [Ar II] line flux | |
NE3_15NE2RATIO | Ratio of the 15.56µm [Ne III] to the 12.81µm [Ne II] line flux | |
NE5_14NE2RATIO | Ratio of the 14.32µm [Ne V] to the 12.81µm [Ne II] line flux | |
NE5_24NE2RATIO | Ratio of the 24.32µm [Ne V] to the 12.81µm [Ne II] line flux | |
O4NE2RATIO | Ratio of the 25.89µm [O IV] to the 12.81µm [Ne II] line flux | |
O4S_33RATIO | Ratio of the 25.89µm [O IV] to the 33.48µm [S III] line flux | |
O4S_18RATIO | Ratio of the 25.89µm [O IV] to the 18.71µm [S III] line flux | |
S4S3_18RATIO | Ratio of the 10.51µm [S IV] to the 18.71µm [S III] line flux | |
SI2_S3_33RATIO | Ratio of the 34.82µm [Si II] to the 33.48µm [S III] line flux | |
Line fluxes of H2 lines |
Observable |
Description |
Unit |
H2S0FLUX | Integrated flux of the 28.2µm H2 S(0) emission line | 10-21 W/cm2 |
H2S1FLUX | Integrated flux of the 17.02µm H2 S(1) emission line | 10-21 W/cm2 |
H2S2FLUX | Integrated flux of the 12.28µm H2 S(2) emission line | 10-21 W/cm2 |
H2S3FLUX | Integrated flux of the 9.66µm H2 S(3) emission line | 10-21 W/cm2 |
H2S5FLUX | Integrated flux of the 6.91µm H2 S(5) emission line | 10-21 W/cm2 |
H2S7FLUX | Integrated flux of the 5.51µm H2 S(7) emission line | 10-21 W/cm2 |
Rest frame
continuum flux densities |
Observable |
Description |
Unit |
CONT37FLUX | Rest frame continuum flux density at 3.7µm | mJy |
CONT42FLUX | Rest frame continuum flux density at 4.2µm | mJy |
CONT55FLUX | Rest frame continuum flux density at 5.5µm | mJy |
CONT97FLUX | Rest frame continuum flux density at 9.7µm | mJy |
CONT15FLUX | Rest frame continuum flux density at 15µm | mJy |
CONT24FLUX | Rest frame continuum flux density at 24µm | mJy |
CONT30FLUX | Rest frame continuum flux density at 30µm | mJy |
Rest frame
continuum ratio |
Observable |
Description |
Unit |
C15C55RATIO | Ratio of 15µm to 5.5µm rest frame continuum flux density | |
C24C55RATIO | Ratio of 24µm to 5.5µm rest frame continuum flux density | |
C30C55RATIO | Ratio of 30µm to 5.5µm rest frame continuum flux density | |
Solid-state features |
Observable |
Description |
Unit |
SILSTRENGTH | Strength of 9.7µm amorphous silicate band | |
CRYST19STRENGTH | Strength of 19µm crystalline silicate band | |
CRYST23STRENGTH | Strength of 23µm crystalline silicate band | |
CRYST28STRENGTH | Strength of 28µm crystalline silicate band | |
CRYST33STRENGTH | Strength of 33µm crystalline silicate band | |
TAUICE | Optical depth of the 6µm ice feature | |
TAU685 | Optical depth of the 6.85µm aliphatic feature | |
Synthetic Spitzer and WISE Photometry |
Observable |
Description |
Unit |
IRAC8FLUX | Synthetic IRAC 8µm photometry | mJy |
WISE12FLUX | Synthetic WISE 12µm photometry | mJy |
IRS15FLUX | Synthetic IRS 15µm photometry | mJy |
WISE22FLUX | Synthetic WISE 22µm photometry | mJy |
IRS22FLUX | Synthetic IRS 22µm photometry | mJy |
MIPS24FLUX | Synthetic MIPS 24µm photometry | mJy |
Synthetic MIRI Photometry |
Observable |
Description |
Unit |
MIRI56FLUX | Synthetic MIRI 5.6µm photometry | mJy |
MIRI77FLUX | Synthetic MIRI 7.7µm photometry | mJy |
MIRI10FLUX | Synthetic MIRI 10.0µm photometry | mJy |
MIRI11FLUX | Synthetic MIRI 11.3µm photometry | mJy |
MIRI13FLUX | Synthetic MIRI 12.8µm photometry | mJy |
MIRI15FLUX | Synthetic MIRI 15µm photometry | mJy |
MIRI18FLUX | Synthetic MIRI 18µm photometry | mJy |
MIRI21FLUX | Synthetic MIRI 21µm photometry | mJy |
MIRI25FLUX | Synthetic MIRI 25.5µm photometry | mJy |
Spline-based PAH measurements |
Observable |
Description |
Unit |
PAH62FLUX | Integrated flux of the
6.2µm PAH feature | 10-21 W/cm2 |
PAH62EQW | Ice-corrected equivalent width of the
6.2µm PAH feature | µm |
PAH77FLUX | Integrated flux of the
7.7µm PAH feature | 10-21 W/cm2 |
PAH77EQW | Equivalent width of the
7.7µm PAH feature | µm |
PAH86FLUX | Integrated flux of the
8.6µm PAH feature | 10-21 W/cm2 |
PAH86EQW | Equivalent width of the
8.6µm PAH feature | µm |
PAH11FLUX | Integrated flux of the
11.2µm PAH feature | 10-21 W/cm2 |
PAH11EQW | Equivalent width of the
11.2µm PAH feature | µm |
PAH127FLUX | Integrated flux of the
12.7µm PAH feature | 10-21 W/cm2 |
PAH127EQW | Equivalent width of the
12.7µm PAH feature | µm |
PAH fluxes and equivalent widths obtained using PAHFIT
(Smith et al. 2007, ApJ 656, 770) or QUESTFIT (Veilleux et al. 2009, ApJS 182, 628)
differ strongly from those measured using the spline-based method
in the following ways:
1) PAH emission bands are assumed to have Drude profiles, which
have broader wings than Gauss profiles or Pearson-IV profiles. The
PAH fluxes are therefore larger than from the spline-based method.
2) The continuum underneath the PAH emission bands lies below the
observed/pseudo continuum, because part of the observed continuum level
is formed by the overlapping wings of the Drude shaped PAH profiles. The
equivalent widths of PAH features are therefore larger.
The DRUDE observables in the table below originate from either PAHFIT
or QUESTFIT depending on whether the source has a strong silicate
absorption feature or not. In the former case the DRUDE observables
were supplied by QUESTFIT, in the latter case by PAHFIT.
We have used a modified version of PAHFIT (Gallimore et
al. 2010, ApJS 187, 172), which assumes PAH features and emission lines to
be un-attenuated. Our PAHFIT PAH fluxes and equivalent widths
therefore have not been extinction corrected.
Like PAHFIT, QUESTFIT assumes PAH fluxes and
equivalent widths to have Drude shaped feature profiles. The big
difference with PAHFIT is that the 24 PAH components are not allowed to
vary freely amongst themselves during the fit. Instead they are
constrained to two sets of pre-determined PAH component ratios -- or
"PAH templates" -- each of which stems from fits to Spitzer-IRS
spectra of multiple star forming galaxies (Smith et al. 2007, ApJ 656, 770).
The contribution of either PAH
template can be varied in the overall QUESTFIT optimization.
Unlike PAHFIT (and the modified version that we used), QUESTFIT includes
screen absorption by water ice (6µm), aliphatic hydrocarbon (6.85 and 7.25µm) and
crystalline silicate absorption (23µm) on the thermal dust emission
components as free parameters.
Like for our modified version of PAHFIT, QUESTFIT assumes attenuation
on PAH emission to be negligible. Extinction on the PAH templates is
hence not a parameter in the fit.
QUESTFIT is only used to fit spectra of moderately to deeply
obscured targets, for which the number of degrees of freedom on the
shape of the PAH emission spectrum is too large to produce realistic
fits in all cases.