Tuesday, April 30, 2013

Filter Curves CD13 and CD14

I put together a filter curve plot based on what we have for CD13 and CD14.  Note that this should mostly be read for where we have coverage and where we don't.  Each filter throughput has been normalized to its peak at angles > 45 degrees.  We can't currently use this plot for instrument efficiency as a function of wavelength.

Note that for CD14, we were throwing light away as shown by the strong glint.  This will generally mess up the high angle measurements.  For example, I don't think the Soifer, UKIRT, and 18a w/ZnSe really trail off that way.



From the figure and data in hand, we need new MgF2 blockers for the N04582, BP6000, and BP6600 filters.  It would be nice to find a filter that goes down to 15.5 microns since the atmosphere is open there.  Likewise, it would be nice to get something centered at 20 microns, but I think this isn't a high priority given the misalignment in CD14.  There are a few we still have to test for the above plot and then we likely need to do more comprehensive throughput tests.

Monday, April 29, 2013

CD014 High-medium slit resolutions at 17.3um

Report on getting the high-res slit feature resolutions at the 580.5 cm-1 setting (17.3um).
The resolutions are surprisingly high, so I'm showing all my assumptions and methods here.

The data is from  /CD014/cd14_2013mar13/file17.fits-file22.fits

Instrument settings:
filter: 18a + KBr
V_decker=2.1614 V to maximize slit length
V_echelle=8.733 to center the 3 H2O lines in columns 200-300
pumping continuously on gas cell
33 ctdelay; 100 1 egos
Subtracted frame 3 from frame 0 for all data.

There are 3 strong H2O lines in this setting:
580.53650 cm-1
580.73199 cm-1
581.08783 cm-1

These lines appeared in 2 echelon orders, with the 580.7 cm-1 line having another order partially recorded at the bottom of an echelon order.
high-medium spectrum at 580.5 cm-1, with 3 H2O lines

I removed some odd/even by subtracting the median of each row from the image, end then fit vertical columns over the lines with 6-term Gaussians.
I corrected for the projection effect of the slant by multiplying by cos(angle-to-horizontal).
Angles for lines 580.54: -25.7deg   580.7:-24.8deg  581.1: -29.3deg

The reported FWHM are median(sigma*2.355*cos(ang))+/-stddev(the same)-- where sigma is the array of Gaussian widths across the lines.

filename  slit#    FWHM_580.54    FWHM_580.73    FWHM_581.09
file22    slit1    7.75+/-0.18    6.93+/-0.14    8.07+/-0.20
file21    slit2    7.92+/-0.20    7.21+/-0.18    8.33+/-0.17
file20    slit3    8.39+/-0.23    7.73+/-0.18    8.90+/-0.22
file19    slit4    9.38+/-0.24    8.98+/-0.24    10.21+/-0.22
file18    slit5    10.73+/-0.29   10.40+/-0.25   11.73+/-0.28
file17    slit6    12.73+/-0.31   12.71+/-1.65   14.11+/-0.33


To obtain the wavelength solutions, I fit lines vertical centers of the H2O lines (including the second 580.73cm-1), and I fit lines to the echelon order gaps. I took the intersection point of these lines and calculated the distance between them. For the 581.1-580.73 span, this was 507.4 pix, for 0.3558 cm-1
or 0.0007013 cm-1 per pixel @ 581.1cm-1 or 0.3619 km/s per pixel. For the echelon order with 580.54 and 580.73, 0.4036 km/s.

Illustration of how I found the wavelength scale(s)

Resolutions at each line
filename  slit#   R_580.54  R_580.73  R_581.09
file22    slit1    95800    119500    102700
file21    slit2    93800    114900    99400
file20    slit3    88500    107200    93100
file19    slit4    79200    92200     81200
file18    slit5    69200    79700     70600
file17    slit6    58400    65200     58700


The lower resolution of the 580.5 line is mostly due to the larger km/s per pixel value for that right echelon order. The difference in resolutions in 580.7 and 581.09 in the left echelon order is mostly due to the better focus position of the 580.7 cm-1.






Friday, April 26, 2013

TAAS summary

Updated 9/23/13 to include Ted Dunham's email with relevant TAAS information.

This is supposed to be a summary of the TAAS information from CD14.  Data for Pupil Imaging and SCHP are from 2013jan9.

PUPIL IMAGING

For imaging the pupil, we compared the ZnSe and the KRS5 lenses, which are at different distances from the detector.  The pupil had a set of wires taped across it as a target (see post).  The figure below shows the ZnSe and the KRS5 images.  The different lenses (distances) clearly have different platescales.  The  location of the two images probably depends on the rotation.  The focus appears better to me with the ZnSe, but hard to be quantitative.  Since the detector is tilted and the focus will depend on the echelle mirror that we subsequently moved far away (these are near best echelle focus or ~5 turns), I'm not going to care too much.

zoom on Pupil images with ZnSe lens and KRS5 lens.  The lenses were at different distances from the (tilted) detector.  The SCHP was not on.  
The wires outlined in red are separated by 10.4 mm.  From the intersections in pixels, I calculate pupil platescales of 0.258 mm/pixel for ZnSe and 0.207 mm/pix for KRS5, for what it is worth.

Next cooldown, we probably want to see how moving echelle mirror effect pupil focus.

SCHP

Our first image of SCHP was with it located at (144,144) in its coordinates.  According to Ted Dunham's email (Feb 7, 2013), they found the DAOF TAAS matched SOFIA when it had the SCHP at (140.5,115.3), although there is no guarantee the two TAAS's are exactly alike.  Our center ended up being at (131, 116).  This should move us, in EXES pixels, around (-7,7).  We will be moving away from the red wire outlines in the figure above.

We moved the SCHP around (with KRS5 lens in place) and found that the SCHP coordinate distances are roughly 95% the size of our pixel distances and tilted at a 45 degree angle.  Moving SCHP by (0,10) gave pixel difference of (7,7), but I expect there are 1 pixel inaccuracies.

We used the SCHP images to find the location of our center and to size the cold stop relative to the secondary.  According to Curtis's measurements and Bob Thompson's email, the SCHP has a 2.5 inch aperture located 2950 mm away.  The LCHP has a 6 inch aperture and matches the angular size of the SOFIA secondary, so 2.5/6 = 0.42 or the SCHP is 42% the size of the SOFIA secondary.   The SCHP in the ZnSe image (below)  has a radius of 30 pixels and the cold stop radius is 76 pixels.  These values suggest the EXES cold stop is 94% of the image of the SOFIA secondary.



Note that when we compared EXES bolted to SI flange with cart snug underneath and EXES unbolted and resting on cart (images 24 and 25, respectively), we saw a change in the location of the SCHP (but not cold stop) of ~2 EXES pixels.  Based on by eye circles, looked mostly vertical in image, but difference image made it look more along the green wire.

FCLS (data from 6 Feb 13)

Finally, we tried using the FCLS.  In imaging, the shape of the field suggests the F/D/S wheels were not all open/open/open.  We moved the slit in place and must have noted a pixel near the center since the slit circle in image below is centered differently than imaging circles.

The plate scale based on the numbers in the figure below is roughly 21.5 EXES pixels per FCLS position unit.  The same sort of 45 degree tilt is present.

Ted Dunham (Feb 7, 2013 email) has notes that say the FCLS(x,z) = (46.1, 31.9) when centered on the flange.  The units for FCLS movement are millimeters and he found that 1mm FCLS motion moved the source by 4.16" on his array, which is the predicted platescale at the SOFIA focal plane to 1%.


Some prettied up images of the FCLS.

For focus, we found a best focus of 6832 on the FCLS.  Not sure of these units.  Pretty certain that more positive means the telescope focus moves further forward (in aircraft coordinates).  Ted said that their best focus was at 7050 and that +-75 counts would not be surprising.  They're focus is 319 mm forward (in aircraft coordinates) of the SI mounting surface.  I believe the focal range for SOFIA is -300 mm to +900 mm relative to the SI flange.  Our design telescope focus should be, I believe, at +300mm or just slightly aft of Ted's.

Tuesday, April 09, 2013

CD014 Filter Scans

BP14100_850, No blocker

BP6600_320, CaF2 blocker

University of Reading 6.2um, MgF2 blocker

N04582-8, CaF2 blocker

N04679-4, CaF2 blocker

OCLI Q, BaF2 blocker

OCLI R, BaF2 blocker
BP6000-250, CaF2 blocker

Soifer Filter, partial scan
UKIRT Filter


18a filter + ZnSe Window, KBr Blocker

18a filter, KBr blocker


Scans were typically taken with a decker dash crossed with a slit, looking at the room, or looking at the black body. Slit width and ctdelay and readout pattern (e.g. 4 1 egos, 100 1 egos were chosen to get high, unsaturated signal. Details will be reported in notes later.
The four decker wheel broad band filters were scanned and will be posted later.


To get a representative value of the illuminated part of the image, I used the mean value of pixels between the 70% and 99.5% percentile. Visually, this did a good job finding the orders. It needs modification, though, if it will reject scattered light.


Below are notes on each filter scan:

18a + KBr blocker:
cd14_2013feb01/file0-file36
Decker: 0.6082 V (14-pix dash), Slit: 5.0134 V (3.5km/s)
70 ctdelay, Readout pattern not recorded …

18a+ZnSe + KBr blocker:
cd14_2013feb01/file37-file72
Decker: 0.6082 V (14-pix dash), Slit: 5.0134 V (3.5km/s)
70 ctdelay, Readout pattern not recorded …

N04679-4 + CaF2 blocker:
cd14_2013mar22/file16-file54

N04582-8 + CaF2 blocker:
cd14_2013mar22/file56-file92

BP6000-250 + CaF2 blocker:
cd14_2013mar23/file0-file37

University of Reading 6.2um + MgF2 blocker:
cd14_2013mar23/file42-file78

BP6600-320 + CaF2 blocker:
cd14_2013feb13/file131-file161
Decker: 0.6086 V (14-pix dash), Slit: 5.0122 V (3.5km/s)
100 ctdelay, 6 1 egos

Soifer Filter:
cd14_2013feb13/file68-file98
file68-file80 (6.5V-7.7V,  -> 18.1um-23.9um) were apparently overwritten by files from 2/14/2013.
Decker: 0.6086 V (14-pix dash),Slit: 5.0122 V (3.5km/s)
70 ctdelay, 4 1 egos
leaks: none


OCLI R + BaF2 blocker:
cd14_2013mar26/file51-file89

OCLI Q + BaF2 blocker:
cd14_2013feb13/file99-file130
Decker: 0.6086 V (14-pix dash), Slit: 5.0122 V (3.5km/s)
70 ctdelay, 4 1 egos

BP14100_850:
cd14_2013feb14/file31-file65
Decker: 0.6086 V (14-pix dash), Slit: 5.0123 V (3.5km/s)
70 ctdelay, 4 1 egos


UKIRT:
cd14_2013feb12/UKIRTScan2013_Feb12/file0-file35
Decker: 0.608 V (14-pix dash), Slit: 5.01 V (3.5km/s)
70 ctdelay, 4 1 egos




Tuesday, April 02, 2013

reset oddity(?)

I was looking at the Fowler 7 tests that Mike did.  The files are (per email):

7 N's, 5 S's, 6 N's, 1 D                file c:/data/CD014/cd14_2013mar20/cold.lab.00016.fits
7 N's, 17 S's, 6 N's, 1 D               file c:/data/CD014/cd14_2013mar20/cold.lab.00017.fits


Mostly I was looking at the data in 00016, but what I noticed appears to be true in 00017 as well.

For most of the differences, data values are fine.  There is, however, a strange behavior during frames with resets.  The plot below plots:

white: 00016 12thN-13thN vs 13thN - D
red: 00016 4thN-5thN vs 6thN-7thN
blue: 00016 10thN-11thN vs 9thN vs 10thN
green: 00017 10thN-11thN vs 9thN vs 10thN
yellow: 00017 12thN - 13thN vs 13thN - D


You can see that the ones involving resets (white, yellow) have two states while the red, blue, and green, which do not have resets, are fine.  

A separate plot of just even row differences (ie, 00016 12thN-13thN vs 13thN-D just even rows) and just odd rows shows that the odd rows are the ones behaving differently.  Remember that IDL starts with Row 0, so evens are the first row.

CD14 High-medium slit resolutions at 14um

CD014 high-medium spectrum of 4th order Q-branch of C2H2.
Line FWHM (pixels) of Q-branch lines with slit1-6 during CD014

Line FWHM (pixels) of Q-branch lines with slit1-6 during CD013


The plot above shows the spectral line FWHM we got from slits 1-6 in high-medium mode at 14um for CD013 and CD014.
Each point on the graph is for a particular spectral line and is the median value of FWHM in the spectral dimension. To convert from the Gaussian 1-sig width in the vertical dimension to FWHM in the spectral dimension, I multiplied by 2.355 x cos(28), where 28 deg is the typical slant of the lines in CD014.
The typical line slant in CD013 was 21 degrees

I calculated a new wavelength solution, using the positions of Q11-Q15 line centers (wavenums=[729.75,729.86,729.97,730.10,730.23]) and got 0.3647 km/s per pixel. In the previous cooldown, Matt calculated 0.3793 km/s per pixel for CD013 data.

More to come here, but it appears we're very close to, or surpassing R=100K with slit3, which I think was our goal.