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Master catalogue used: __master_catalogue_xfls_20171201.fits__<br>
Number of rows: 977,148
<br>
Surveys included:<br>
| Survey | Telescope / Instrument | Filters (detection band in bold) | Location |
|---------------|------------------------|:---------------------------------:|-----------------|
| KPNO-FLS | | R | dmu0_KPNO-FLS |
| INT-WFC | INT/WFC | ugriz | dmu0_INT-WFC |
| PanSTARRS-3SS | PanSTARRS/GPC1 | ugriz | dmu0_PanSTARRS1-3SS |
| Legacy Survey | BASS | grz | dmu0_LegacySurvey |
| UHS | UKIRT | J | dmu0_UHS |
| DataFusion | Spitzer/IRAC | IRAC1234 | dmu0_DataFusion-Spitzer |
Master catalogue used: master_catalogue_xfls_20171201.fits
Number of rows: 977,148
Surveys included:
Survey | Telescope / Instrument | Filters (detection band in bold) | Location |
---|---|---|---|
KPNO-FLS | R | dmu0_KPNO-FLS | |
INT-WFC | INT/WFC | ugriz | dmu0_INT-WFC |
PanSTARRS-3SS | PanSTARRS/GPC1 | ugriz | dmu0_PanSTARRS1-3SS |
Legacy Survey | BASS | grz | dmu0_LegacySurvey |
UHS | UKIRT | J | dmu0_UHS |
DataFusion | Spitzer/IRAC | IRAC1234 | dmu0_DataFusion-Spitzer |
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At faint magnitudes (mag > 24), some surveys have very large errors on the magnitude. These objects may be unreliable for science puposes.<br>
This includes __Legacy Survey aperture and total__ magnitudes (at mag > 26) and __PanSTARRS aperture and total__ magnitudes (at mag > 23). Alse few sources in __IRAC__ have very large __total__ magnitude errors (at mag > 24).<br>
<img src="help_plots/xFLS_magVSmagerr_BASS_g_mag_total.png" />
At
faint magnitudes (mag > 24), some surveys have very large errors on
the magnitude. These objects may be unreliable for science puposes.
This includes Legacy Survey aperture and total magnitudes (at mag > 26) and PanSTARRS aperture and total magnitudes (at mag > 23). Alse few sources in IRAC have very large total magnitude errors (at mag > 24).
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In most of the case when comparing the aperture magnitudes between surveys, we observed a two peak distribution in the difference between the magnitudes ($\Delta_{mag} = mag_{survey1} - mag_{survey2}$). We have one peak around 0 for point-source objects, with a small spread. And a second peak at higher $\Delta_{mag}$ with a larger spread for extended objects; implying a different aperture correction between surveys for these objects.<br>
That means that galaxies will not have the same aperture magnitude in different surveys. <br>
In the ugriz bands, for bright sources, there is a two peaks distribution when comparing INT, Legacy Survey and Pan-STARRS.
<img src="help_plots/xFLS_apcorrIssues_WFC_r_aperture_-_GPC1_r_aperture.png" />
In
most of the case when comparing the aperture magnitudes between
surveys, we observed a two peak distribution in the difference between
the magnitudes (). We have one peak around 0 for point-source objects, with a small spread. And a second peak at higher with a larger spread for extended objects; implying a different aperture correction between surveys for these objects.
That means that galaxies will not have the same aperture magnitude in different surveys.
In the ugriz bands, for bright sources, there is a two peaks distribution when comparing INT, Legacy Survey and Pan-STARRS.
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### II.a. Pan-STARRS aperture magnitude
Few Pan-STARRS sources have exactly the same error (of <font color='blue'>0.0010860000038519502</font>) on the __aperture and total__ magnitudes in all the grizy bands. The corresponding aperture magnitude should not be trusted for these objects.<br>
<img src="help_plots/xFLS_gpc1Issues_GPC1_g_mag_aperture.png" />
Few Pan-STARRS sources have exactly the same error (of 0.0010860000038519502) on the aperture and total magnitudes in all the grizy bands. The corresponding aperture magnitude should not be trusted for these objects.
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### II.c IRAC aperture magnitude
IRAC is available for this field but no source have exactly the same magnitude.
IRAC is available for this field but no source have exactly the same magnitude.
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### II.b. Outliers
By comparing magnitude in the same band between different surveys, we can see that some magnitudes are significanlty different could not be trusted. <br>
The outliers are identified to have a large weighted magnitude difference (equivalent of the $chi^2$).
$$chi^2 = \frac{(mag_{1}-mag_{2})^2}{magerr_{1}^2 + magerr_{2}^2}$$
<br>
We used the 75th and 25th percentile to flagged the objects 5$\sigma$ away on the large values tail of the $chi^2$ ditribution. (__NB:__ bright sources tend to have their errors underestimated with values as low as $10^{-6}$, which is unrealistic. So to avoid high $chi^2$ due to unrealistic small errors, we clip the error to get a minimum value of 0.1% (i.e. all errors smaller then $10^{-3}$ are set to $10^{-3}$).)
<br><br>
$$outliers == [chi^2 > (75th \;percentile + 3.2\times (75th \;percentile - 25th \;percentile))]$$
<img src="help_plots/xFLS_outliers_BASS_g_aperture_-_GPC1_g_aperture.png"/>
By comparing magnitude in the same band between different surveys, we
can see that some magnitudes are significanlty different could not be
trusted.
The outliers are identified to have a large weighted magnitude difference (equivalent of the ).