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

The activity determines the dispersion and wavelength calibration of the MIPS SED mode. Four targets were chosen for observation to guard against poor (or no) emission line detection in an object. Three planetary nebula were chosen (NGC 6543, NGC6826 and IC3568), and an HII region (a region offset slightly north of the nominal center of 30 Dor). The [O III]88µm emission was detected in all of these objects. In NGC 6543 and NGC6826, the [N III]57µm emission line was also detected, resulting in two more measurements of the spectral dispersion. These measurements, averaged along with those in Campaign K, determine the dispersion and wavelength zero point of the SED mode.

Analysis

Raw data file: mips_AOR_7589376_sed_A70_P70S_pos1_3s.fits = NGC6826

Raw data file: mips_AOR_7589632_sed_A70_P70S_pos1_3s.fits = NGC6543

Raw data file: mips_AOR_7589888_sed_A70_P70S_pos1_3s.fits = IC3568

Raw data file: mips_AOR_7589120_sed_A70_P70S_pos1_3s.fits = 30 Dor (with a slight telescope offset to the north of the nominal center of the nebula)

Reduction:

mips_sloper -j CamR -l -q TARGET.raw.fits

mips_caler -C CamR -P mips_caler70S.param TARGET.red.fits

IDL> Iraf_Legacy,'TARGET.cal.fits',RepVal=-9999,/nomask

An illumination correction that was averaged from this and previous IOC campaigns was used in the mips_caler reductions.

Within IRAF: imcombine was used to find medians of the various spacecraft/scan mirror positions used in each AOR. No sky subtraction was performed. Measurements of line positions were only made for Side A of the 70µm array.


Results

The 30 Dor observations were offset by several arcminutes to the north of the brightest part of the nebula. Medians were constructed for each of the two telescope positions and the results were added to increase the area on the array where the [O III]88µm emission line can be detected. No other emission line was detected in the spectrum. The median of columns 2-12 is displayed below and the measured position of the emission line is at pixel 21.77.

Both the [O III] and the [N III]57µm emission lines were detected in the medianed (columns 2-12) spectrum of NGC6543 shown below. The positions of the lines are pixel 21.36 for [O III] and pixel 3.57 for [N III]. This yields a non-distortion-corrected dispersion of 1.72 µm/pixel along the columns (Y) of the detector array.

As with NGC6543, both [O III] and [N III] were detected in the median (columns 2-12) spectrum of NGC6826 (see below). The positions of the lines are pixel 21.30 for [O III] and pixel 3.36 for [N III], yielding a non-distortion-corrected dispersion of 1.70 µm/pixel along the columns (Y) of the detector array.

The planetary nebula IC3568 is much fainter that either NGC6543 or NGC6826, and only the [O III]88µm was detected at both telescope pointings (see the following two figures). The first figure shows the median spectrum for columns 2-6 and the second figure shows the median spectrum for columns 8-14 which includes the bad readout section (i.e., the values for pixels 1-8 in the spectrum are invalid). The [N III] emission line cannot be definitively identified in the spectrum that avoids the bad readout. For comparison with the other objects, and since the [O III] cannot be identified across the entire length of the slit (columns 1-16 for Side A), an average of the two spectra was used to measure the position of [O III]88µm at approximately column 7. As a result, the position of [O III] is at pixel 21.13.

These measurements, averaged with the results of MIPS-145K yield the following parameters for the SED mode (THESE RESULTS SUPERSEDE THOSE FROM CAMPAIGN K):

The position of the [O III]88µm line was measured along the slit in the spatial direction for all four nebulae. It is found that the line center shifts by at most 0.5 pixel in the dispersion direction from one end of the useful portion of the slit to the other (array columns 1-16). These measurements are consistent with the measurements of [O III]88µm made from 30 Dor in IOC Campaign K along the entire length of the SED slit (Side A and B of the 70µm array). The table below shows measurements of the line at various positions along the slit for the four targets.

Columns medianedPosition along slitPosition of emission line

(X; in pixels)(Y; in pixels)



30 Dor N

6-10821.75
11-151321.81
NGC6543

1-5321.30
6-10821.42
11-151321.80
NGC6826

1-5321.35
6-10821.32
11-151321.93
IC3568

2-6421.09
8-141121.18


Conclusions

The MIPS SED mode meets the requirements of providing spectral coverage from about 52µm to 106µm with a dispersion of about 1.7 µm/pixel. The alignment between the dispersive element (diffraction grating) and the 70µm array is very good as there is much less than a 1-pixel difference in the position of an emission line along the useful length of the SED slit. The averaged results presented in this report supersede the earlier results reported from MIPS-145K. The results from MIPS-145R are fully consistent with the results of MIPS-145K.

Output and Deliverable Products


Actions Following Analysis

The combined results from MIPS-145K and MIPS-145R should suffice for the wavelength calibration of the MIPS SED mode. A small correction determined from MIPS-140V for distortion will need to be applied to the dispersion solution due to the tilt of the spectrum on the array. However, preliminary results from MIPS-140V indicate that this correction will be small (on the order of 0.5-1.0 pixel the dispersion axis and less in the spatial direction).