17.12.2012 Views

IRAC Instrument Handbook - IRSA - California Institute of Technology

IRAC Instrument Handbook - IRSA - California Institute of Technology

IRAC Instrument Handbook - IRSA - California Institute of Technology

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

Point Source Fitting <strong>IRAC</strong> Images<br />

with a PRF<br />

164<br />

<strong>IRAC</strong> <strong>Instrument</strong> <strong>Handbook</strong><br />

2. Artifact correction: use CBCDs or preprocess your <strong>IRAC</strong> BCD data to remove or mask artifacts<br />

as necessary.<br />

3. Rmasks: assuming the data were taken with overlapping (C)BCDs, make a mosaic with MOPEX,<br />

doing outlier rejection, and creating Rmasks. Then include the appropriate Rmasks with your<br />

input data to APEX.<br />

4. PRF: put the center H<strong>of</strong>fmann 100x PRF (the one with ...col129_row129...) in your MOPEX cal/<br />

subdirectory for command-line (this will be PRF_FILE_NAME in the namelist file), or type it<br />

into the GUI. Although you can run APEX with just the center PRF, we recommend using the<br />

whole PRF Map set, as it noticeably improves the quality <strong>of</strong> the fits for sources outside <strong>of</strong> the<br />

central region <strong>of</strong> the arrays. To do this, create a table like the one linked from the PSF/PRF<br />

section <strong>of</strong> the <strong>IRAC</strong> web pages (substituting appropriate filenames and paths). PRF position<br />

refers to the bottom-left corner <strong>of</strong> the region <strong>of</strong> size NAXIS1, NAXIS2 over which the PRF is<br />

valid (in native pixels). This will be PRFMAP_FILE_NAME in a namelist, or you can type it into<br />

the GUI. Figure C.5 shows how the PRFs are distributed over the arrays.<br />

5. Normalization Radius: the H<strong>of</strong>fmann PRFs require a normalization that matches the <strong>IRAC</strong><br />

calibration radius. In the Sourcestimate block, set Normalization_Radius = 1000 (since it is in<br />

PRF pixels and the sampling is 100x).<br />

6. Run APEX. If doing command-line for <strong>IRAC</strong>1, edit the default namelist for your data and run:<br />

apex.pl -n apex_I1_yourdata.nl<br />

7. PRF Flux: The PRF flux column is called ''flux'' in the extract.tbl output file, and the units are<br />

micro-Jy. These need to be divided by the appropriate photometric correction factors from Table<br />

C.1: 1.021 (<strong>IRAC</strong> 1), 1.012 (<strong>IRAC</strong>2), 1.022 (<strong>IRAC</strong>3) and 1.014 (<strong>IRAC</strong>4).<br />

8. PRF Flux Uncertainty: The column labelled ''delta_flux'' is the formal uncertainty from the leastsquares<br />

fit. It will in general underestimate the flux uncertainty. Do not use the column labelled<br />

“SNR”' for <strong>IRAC</strong>, as it only takes into account the background noise, and ignores the Poisson<br />

(shot) noise term which typically dominates the error. The best estimate is the aperture<br />

uncertainty (calculated from the data uncertainties) in a 3 pixel radius. This covers the majority <strong>of</strong><br />

the PSF without going too far out. (For the default namelist, the relevant uncertainty is in column<br />

''ap_unc2'' [microJy].)<br />

9. Array Location-Dependent Photometric Corrections: Multiply the (C)BCDs by the correction<br />

image ("...photcorr...") and run APEX on the resulting images. The fluxes will be correct for<br />

"blue" sources (where blue means having the colors <strong>of</strong> an early-type stellar photosphere). For<br />

"red" sources (objects with colors close to that <strong>of</strong> the zodiacal light) use fluxes derived from<br />

running APEX on unmodified CBCDs.<br />

10. Color Correction: This is the correction needed to get the right monochromatic flux if your source<br />

spectrum is different from the reference spectrum used to calibrate the <strong>IRAC</strong> filters<br />

( νFν = constant). There is a good discussion <strong>of</strong> this in Chapter 4 <strong>of</strong> this <strong>Handbook</strong>.<br />

If all these steps are followed, then the systematic error in the flux measurement for bright, isolated point<br />

sources should be ~1%. A comparable systematic error exists in the flux density scale. Background<br />

estimation errors will contribute significantly to the error budget for fainter sources and in confused<br />

fie lds.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!