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IRAC Instrument Handbook - IRSA - California Institute of Technology

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List <strong>of</strong> Figures 190<br />

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

FIGURE 4.2: <strong>IRAC</strong> INSTRUMENT SUPER SKYFLATS SHOWING THE FLATFIELD RESPONSE<br />

AS MEASURED ONBOARD, FOR CHANNELS 1–4................................................................34<br />

FIGURE 4.3. ARRAY LOCATION-DEPENDENT PHOTOMETRIC CORRECTION IMAGES. CH 1<br />

IS IN THE UPPER LEFT, CH 2 IN THE UPPER RIGHT, CH 3 IN THE LOWER LEFT AND<br />

CHANNEL 4 IN THE LOWER RIGHT. ....................................................................................44<br />

FIGURE 4.4: DEPENDENCE OF POINT SOURCE PHOTOMETRY ON THE DISTANCE OF THE<br />

CENTROID OF A POINT SOURCE FROM THE NEAREST PIXEL CENTER IN CHANNEL 1.<br />

THE RATIO ON THE VERTICAL AXIS IS THE MEASURED FLUX DENSITY TO THE MEAN<br />

VALUE FOR THE STAR, AND THE QUANTITY ON THE HORIZONTAL AXIS IS THE<br />

FRACTIONAL DISTANCE OF THE CENTROID FROM THE NEAREST PIXEL CENTER. .....46<br />

FIGURE 4.5. THE IN-FLIGHT <strong>IRAC</strong> POINT RESPONSE FUNCTIONS (PRFS) AT 3.6, 4.5, 5.8 AND<br />

8 MICRONS. THE PRFS WERE RECONSTRUCTED ONTO A GRID OF 0.3” PIXELS, ¼ THE<br />

SIZE OF THE <strong>IRAC</strong> PIXEL, USING THE DRIZZLE ALGORITHM. WE DISPLAY THE PRF<br />

WITH BOTH A SQUARE ROOT AND LOGARITHMIC SCALING, TO EMPHASIZE THE<br />

STRUCTURE IN THE CORE AND WINGS OF THE PRF, RESPECTIVELY. WE ALSO SHOW<br />

THE PRF AS IT APPEARS AT THE <strong>IRAC</strong> PIXEL SCALE OF 1.2”. THE RECONSTRUCTED<br />

IMAGES CLEARLY SHOW THE FIRST AND SECOND AIRY RINGS, WITH THE FIRST<br />

AIRY RING BLENDING WITH THE CORE IN THE 3.6 AND 4.5 µM DATA...........................47<br />

FIGURE 4.6. THE <strong>IRAC</strong> POINT RESPONSE FUNCTIONS (PRFS) AT 3.6, 4.5, 5.8 AND 8.0<br />

MICRONS. THE PRFS WERE GENERATED FROM MODELS REFINED WITH IN-FLIGHT<br />

CALIBRATION TEST DATA INVOLVING A BRIGHT CALIBRATION STAR OBSERVED AT<br />

SEVERAL EPOCHS. CENTRAL PRFS FOR EACH CHANNEL ARE SHOWN ABOVE WITH A<br />

LOGARITHMIC SCALING TO HELP DISPLAY THE ENTIRE DYNAMIC RANGE. THE PRFS<br />

ARE SHOWN AS THEY APPEAR WITH 1/5TH THE NATIVE <strong>IRAC</strong> PIXEL SAMPLING OF 1.2<br />

ARCSECONDS TO HIGHLIGHT THE CORE STRUCTURE. ...................................................49<br />

FIGURE 4.7. EXTENDED SOURCE FLUX CORRECTION FACTORS; SOLID LINES REPRESENT<br />

EXPONENTIAL FUNCTION FITS TO THE DATA. ALSO INDICATED ARE CORRECTION<br />

FACTORS DERIVED FROM ZODIACAL LIGHT TESTS, AND GALACTIC HII REGION<br />

TESTS (E.G. MARTIN COHEN'S GLIMPSE VS. MSX, PRIVATE COMMUNICATION)..........58<br />

FIGURE 4.8. EXTENDED SOURCE FLUX CORRECTION FACTORS FOR GALAXIES (SOLID<br />

LINES) VERSUS THE PSF APERTURE CORRECTION FACTORS (DOTTED LINES). THE<br />

MAIN DIFFERENCE BETWEEN THE TWO IS THE TRULY DIFFUSE SCATTERING<br />

INTERNAL TO THE ARRAY...................................................................................................58<br />

FIGURE 4.9. NOISE VERSUS BINNING LENGTH IN CHANNEL 1. TO MAKE THIS PLOT THE<br />

SURFACE BRIGHTNESS WAS MEASURED IN NINE REGIONS ACROSS AN OBJECT-<br />

MASKED MOSAIC. THESE REGIONS ARE NOT NEAR THE BRIGHT GALAXIES, STARS,<br />

OR DIFFUSE PLUMES. THE NOISE IS DEFINED AS THE STANDARD DEVIATION OF<br />

THOSE NINE REGIONS. THE BOX SIZE IS INCREMENTALLY INCREASED UNTIL THE<br />

BOX LENGTH IS MANY HUNDREDS OF PIXELS. FOR REFERENCE THE SOLID LINE<br />

SHOWS THE EXPECTED LINEAR RELATION. .....................................................................61<br />

FIGURE 4.10. NOISE VERSUS BINNING LENGTH IN CHANNEL 2. TO MAKE THIS PLOT THE<br />

SURFACE BRIGHTNESS WAS MEASURED IN SIX REGIONS ACROSS AN OBJECT-<br />

MASKED MOSAIC. THESE REGIONS ARE NOT NEAR THE BRIGHT GALAXIES, STARS,<br />

OR DIFFUSE PLUMES. THE NOISE IS DEFINED AS THE STANDARD DEVIATION OF

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