There is a problem w/ your write-up. Check that you have valied entries for \$CAID and \$Campn in your analysis.php file. If that checks out, then Contact Stansberry"; return ; } // get first matching task $row = mysql_fetch_array($result); $title = $row["title"]; $princ = $row["principal"]; $deputy= $row["deputy"]; $campn0 = $row["campn0"]; $aorkeys = $row["aorkeys"]; // get real name of principal, deputies $princ = ioc_get_person($princ); $princ = $princ[0]; $deps = explode(",",$deputy); foreach ($deps as $depty) { $depty = trim($depty); $depty = ioc_get_person($depty); $depty = $depty[0]; $depty = explode(",",$depty); $depty = $depty[0]; // last names only $deplist[] = $depty; } $deplist = implode(", ", $deplist); $caid = sprintf("%03d",$caid); $file = "mips-".$caid.$campn.".analysis.php"; // if more matches, append the AORKEYS from those $numrows = mysql_num_rows($result); if ($numrows > 1) { $aorkeys = " " . $numrows . " Task Executions:  ". $aorkeys; for ($i=0;$i < mysql_num_rows($result); $i++) { $row = mysql_fetch_array($result); $morekeys = $row["aorkeys"]; $aorkeys = $aorkeys .';  '.$morekeys; } } // END PHP. ?> <? echo "MIPS-$caid, Campaign $campn IOC/SV Analysis"; ?>

Principal:
Deputy:
Analyst:
AORKEYS:
Last Updated:


Task Outcome Summary


Abstract

This task is designed to measure the calibration as a function of various parameters such as source brightness, background level, spectral type, and integration time. It is thus similar to the MIPS-315 task (campaign E for 24µm and campaign R for the Ge:Ga arrays), except that it includes all stars observed up to this point. We find that background levels and spectral type have no significant effects on the calibration at 24µm and 70µm, although more data are still needed. There is some flux nonlinearity observed in the Ge:Ga array data (unsurprising since no linearity correction has been made), while the 24µm linearity correction appears to have elminated any nonlinearities. We do not yet find any stars that are obviously poor calibrators. Until the Ge:Ga data reduction is updated with a linearity correction and more asteroids are observed at 160µm, there is little point to revising the Ge:Ga calibration factors. A new fit to all available data at 24µm returns the value 1.5003e5±2335 DN/s/Jy, or 1.033±0.016 µJy/arcsec²/(DN/s).

Analysis

24µm

The raw data were processed through a recent DAT version (typically 2.50 to 2.61 - the results are insensitive to this range of DAT versions) to produce 30 calibrated DCEs per object. These were loaded into IDP3, where aperture photometry was performed using the adopted standard apertures (see the MIPS-920 task writeup) and an aperture correction AC = 1.146. The average photometric DN/s and standard deviation were calculated. A conversion factor was derived by division of the total DN/s by the predicted photospheric flux density in Jy.

A best estimate for the conversion factor was produced by fitting a line to all of the data with "x" the predicted flux density and "y" the measured total DN/s from the target. The line was forced to pass through (0,0). This conversion factor was converted to surface brightness assuming an average pixel size of 2.54 arcseconds.

Final images were constructed by careful alignment of the 30 images in the stack and median combined. The images were not distortion-corrected, and no background has been removed.

Ge:Ga

The data were reduced as described in the MIPS-922 and MIPS-924 task writeups for campaign W, except that DAT v2.61 was used. Photometry was performed as described in those writeups.


Results

24µm

The median combined images can be found here.

Calibration:

The results of the aperture photometry are given in Table 1:

Object Spectral Type Predicted Flux Density (Jy) Measured DN/s 1-sig (%) Ap Corrected Flux (DN/s) CF (DN/s/Jy) 1-sigCF (DN/s/Jy) Background (DN/s) BG 1sig BG-Sig(%)
HD082308 K5III 4.8816 6.113E+05 4.25 7.005E+05 1.435E+05 6.099E+03 1017.84 11.81 1.16
HD087901 B7 1.6089 2.048E+05 2.07 2.347E+05 1.459E+05 3.019E+03 1253.80 10.66 0.85
HD096833 K1III 4.6375 6.493E+05 4.36 7.441E+05 1.605E+05 6.996E+03 611.34 8.31 1.36
HD138265 K5III 0.9797 1.264E+05 1.83 1.449E+05 1.479E+05 2.706E+03 384.48 6.69 1.74
HD152222 K2III 0.3132 4.540E+04 1.82 5.203E+04 1.661E+05 3.023E+03 359.53 7.05 1.96
HD154391 K2III 0.2073 2.650E+04 1.95 3.037E+04 1.465E+05 2.857E+03 363.09 6.97 1.92
HD158460 A2V 0.0462 6.926E+03 3.34 7.938E+03 1.718E+05 5.737E+03 361.43 6.98 1.93
HD158485 A4V 0.0259 3.100E+03 4.94 3.553E+03 1.373E+05 6.781E+03 362.58 7.40 2.04
HD159048 K0III 0.2596 3.114E+04 1.71 3.569E+04 1.374E+05 2.350E+03 353.41 7.21 2.04
HD163466 A2V 0.0227 2.559E+03 8.28 2.932E+03 1.294E+05 1.072E+04 358.65 7.39 2.06
HD163588 K2III 3.3032 3.963E+05 4.78 4.542E+05 1.375E+05 6.572E+03 387.28 6.78 1.75
HD165459 A2? 0.0174 3.309E+03 3.85 3.792E+03 2.179E+05 8.391E+03 360.26 7.10 1.97
HD166780 K4.5III 0.2318 2.665E+04 1.81 3.055E+04 1.318E+05 2.385E+03 364.20 6.88 1.89
HD170693 K1.5III 1.4177 1.665E+05 3.34 1.909E+05 1.346E+05 4.497E+03 363.78 6.91 1.90
HD172066 G5? 0.0217 2.926E+03 4.67 3.353E+03 1.545E+05 7.215E+03 350.30 6.76 1.93
HD172728 A0V 0.0358 4.047E+03 4.35 4.638E+03 1.294E+05 5.628E+03 355.69 7.50 2.11
HD173511 K5III 0.2734 2.804E+04 1.74 3.214E+04 1.176E+05 2.046E+03 357.96 7.23 2.02
HD173976 K5III 0.3241 4.151E+04 1.88 4.757E+04 1.468E+05 2.759E+03 359.24 7.51 2.09
HD174123 G5? 0.0170 1.990E+03 8.22 2.280E+03 1.344E+05 1.104E+04 349.74 7.10 2.03
HD176841 G5? 0.0246 3.165E+03 8.33 3.627E+03 1.474E+05 1.228E+04 350.43 7.11 2.03
HD180711 G9III 3.5422 5.078E+05 1.99 5.819E+05 1.643E+05 3.269E+03 386.97 7.31 1.89
HD189276 K5Iab 2.8151 3.388E+05 2.12 3.883E+05 1.379E+05 2.924E+03 385.91 6.75 1.75
HD191854 G5 0.0354 4.229E+03 4.58 4.847E+03 1.369E+05 6.270E+03 457.91 7.24 1.58
HD216131 G8II 2.2232 2.864E+05 1.92 3.282E+05 1.476E+05 2.834E+03 592.69 7.94 1.34
HD217382 K4III 2.0289 2.858E+05 1.85 3.276E+05 1.614E+05 2.987E+03 381.14 6.94 1.82

 

These results are plotted in Figures 1 & 2. Figure 1 contains all of the data, while figure 2 contains only those stars with good spectral types. The apparent nonlinearity above 2 Jy can probably be removed by excluding the obviously saturated point at 4.8 Jy from the fit.

Figure 1: Top - Best linear fit to all of the MIPS-400 24um data. Bottom - Residuals from fit.

Figure 2: Top - Best linear fit to the MIPS-400 24um data for those stars with good spectral types. Bottom - Residuals from fit.

Calibration Versus Other Parameters:

Figures 3 & 4 show the Calibration Factor versus measured background and spectral type. No obvious trends are seen.

Figure 3: Calibration factor vs. measured background. Top - All data. Bottom - Only those stars with good spectral types.

 

Figure 4: Top - Calibration factor vs. spectral type. Bottom - The measured backgrounds around each star.


Ge:Ga

The mosaicked images can be found here. The table of Ge:Ga measurements is available in html and csv form, and the results are plotted in Figure 5. The table and figure display the same data found in the task writeup for MIPS-315R, with the addition of the 70µm photometry from the MIPS-400 task. The 160µm results will be added as they become available.


Figure 5: Calibration factors as a function of various parameters. On each panel, the 70µm data use the left-hand scale, while the 160µm data use the right-hand scale.

Conclusions

24µm

The absolute calibration at 24µm does not show any dependencies on background, spectral type, or source flux. Barring new observational results or a change in the Si:As array operating parameters, the calibration factor quoted in the abstract is as close to final as we can make it. We do not recommend that any of the calibration sources be rejected as standards at this time, although we list some targets below that may get rejected in the future as we accumulate more data.

All objects appear to be free of obvious excesses above their predicted photospheres. HD172066 lies in a cluttered field so may not be a desirable target. HD191854 lies in a very patchy, diffuse background.

There are still significant issues in the pipeline data reduction that are causing jail-bars and instrumental variations in the background.

70µm

The 70µm calibration does not show any significant effects due to background or spectral type. There is a nonlinearity of about 30% over a factor of 30 in flux, but no linearity correction has yet been applied to the data. Until the data reduction is finalized, there is no indication from these data that the current calibration factor should be updated.

Careful examination of the table will show that no calibrator below about 40 mJy is listed as detected. This is consistent with current noise estimates on the 70µm array - none of those sources would have been detected at better than 4-sigma significance. We are exploring whether improved data processing can pull out some of these sources, but we do recommend that any source less than 100 mJy should be observed using 10-second DCEs, a change we have implemented in the calibration program. Upcoming campaigns should thus extend the calibrator range downward in flux by a factor of 2-3.

160µm

There are as yet no updates to the conclusions in the MIPS-315R writeup. The 160µm calibration needs a good measurement of the spectral leak and more asteroid data before the calibration can be finalized.

Output and Deliverable Products

Actions Following Analysis

The jail bar problem should be fixed. Accurate spectral types for the few stars that lack these data must be obtained. Analysis for 160µm must be completed.