Detector Characteristics
CCDs |
System Response and Throughput |
Flexure and Fringing |
Shutters |
CCD Controllers |
Field Size and Orientation
CCDs
Both sides use uv-flooded Reticon 1200x400 devices with 27 micron
pixels, which corresponds to 0.78 arcsec per pixel. These have
excellent UV response (QE at 3200 A ~40%) and are relatively free of
blemishes.
NOTICE: During Feb 2008 the Kast Blue CCD failed
and was replaced on 29 Feb 2008 by CCD #9, a similar
(though not identical) Reticon 1200x400 device, which will henceforth
be referred to as the Kast Blue CCD.
The CCDs must be kept cold to preserve the flood, and they should be
protected from unnecessary exposure to bright lights. The telescope
technicians are responsible for keeping the dewars cold.
The full well depth is in excess of 200,000 e-, but the ADC saturates at
about 32k minus the baseline, or usually about 30,000 DN, but starts being
non-linear in response at about 27,000 DN. An easy to
remember not-to-exceed number might be 25,000 DN. Gain on both sides
is about 3.9 e-/DN for the red side and 2.3 e-/DN for the blue side.
Readnoise depends on the read speed for the chip,
as listed below.
| CCD | Read Speed | Gain1 |
Read Noise1 |
Approx. Readout Time2 |
| Blue | slow | 2.3 e-/DN | 8 e- | 45 sec |
| Blue | fast | 2.3 e-/DN | 13 e- | 25 sec |
| Red | slow | 3.9 e-/DN | 8.3 e- | 45 sec |
| Red | fast | 3.9 e-/DN | 20 e- | 25 sec |
1Read noise and gain measured 2007 Feb 13 for red side, measured 2008 Mar 1 for blue side (E. Gates).
2Readout time is for full 400x1200 chip. Typical sub-region
of CCD of 160x1200 reads out in 16 sec (8 sec) for slow (fast) readout speed.
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On the red side there is a 3db attenuator in the output line which
doubles the dynamic range at the expense of under sampling the read
noise and very faint signals. If you are observing at low
signal-to-noise ratios, you may wish to have the attenuator removed.
In that case, the gain will be half of the nominal value, or 1.9
e-/DN. The usual choice, and the default, is to operate with the
attenuator in place. Ask the telescope technicians for help if you
wish to remove it.
Suggested operating temperature for both sides is in the range of -110
to -125. A warmer temperature will increase the dark current but
diminish charge transfewr inefficiencies, and vice versa.
In general, if you don't have any prior knowledge of the expected
exposure time, a good practice is to take a one second exposure (not
recorded), and then scale that to the desired count level to determine
the exposure time. It's best not ot overexpose the CCDs. Although no
permanent harm will be done, it may take some time to completely flush
the extra charge.
This is a small point, but perhaps worth mentioning. The saturation
level is determined not by the well depth, but by the limitation
imposed by the 15 bit A-D converter. Thus, if you bin pixels, you may
need to reduce the exposure time correspondingly to stay within the 32k
capacity of the A-D. Remember too that the actual dynamic range
available is not 32k, but 32k minus the baseline. (The baseline is
displayed during startup of the DTS).
System Response and Throughput
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The cameras on both sides are all-refractive. The camera lenses are
temperature controlled; focus is a function of lens temperature. The
focal planes on both sides appear to be quite flat. You may observe
some small-scale variations in the focus due to irregularities of the
chip.
Blue: The design range of the camera is 3000-7000 A. It looks good to
atmospheric cutoff. Peak efficiencey of the entire system including
the telescope is between 5 and 20%, depending on setup. The blue side
operates in first oder, and due to the wavelength coverage, red leak
should not be a problem. If you're imaging on the blue side, remember
that the lens performance deteriorates past 7000 A.
Red: The design range of the camera is 4000-11000 A. Peak system
efficiency is in the vicinity of 30-40%, depending on configuration.
Response is decreasing rapidly by 10,500 A, but successful
observations have been made out to 10,830 A. You will need to
suppress second order if you go beyond twice the effective cut-on
point of the dichroic you use. Remember that the old filter wheels
are in common for both beams, so use the 5.5" round filters in the red
camera filter wheel. Noticeable fringing on the red side starts at
about 7000 A. For most objects, red exposures will probably go
faster. Do multiple reds if necessary to avoid red saturation during
one blue exposure.
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Shane 3 meter Kast Throughput
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Flexure and Fringing
As the position of the telescope changes, the Kast spectrograph
flexes. There is about three to five pixels of total shift on each
side, moving between extreme positions on the sky.
The blue side may shift as much as five pixels parallel to dispersion,
but fringing will not generally be a concern, and the shift may
ordinarily be accounted for by reference to skylines.
The red side may also shift as much as five pixels in the dispersion
direction, and because of fringing this may be a more serious problem
than on the blue side. The usual red fringes start to appear at about
7000 A. This may become a particular problem due to the flexure
described just above, because if observations at large zenith
distances are flattened with straight up flats, the object and flat
fringes may not match. If this is a concern, you may with to take
"local" flats.
Shutters
The Ilex shutter has a minimum exposure time of 1 sec, with timing
errors of a few milliseconds.
CCD Controllers
There is a separate controller for each side. They are mounted one
above the other in a rack near the dewars. They contain most of the
temperature and readout electronics for the CCDs, and will be set up
by the dome crew. The only things the observer need to be concerned
about is the temperature readout in the upper right corner of each
controller. It reads in degrees Celsius to the nearest 1/10th degree
at a location in the dewar near the chip. It should be fairly stable,
and in the range -110 to -125 for the Reticon 400x1200 chips.
Field Size and Orientation
The long slit capability of the spectrograph is very useful for
extended objects as well as collinear ones. For these sorts of
observations, one nearly always wants to rotate the instrument TUB to
some predetemined (or in some cases, determined on the spot from the
guide camera or CCD direct frames) position angle. It's useful to
know which diretions are which, for various position angles, in order
to plan setups and verify that they are correct.
On the guide camera, the scale and orientation varies with diagonal
mirror position. If the TUB is at the standard position angle of 90
degrees, then in mirror position 2 one sees a field about 2 arcmin
across on the guider with north up and east to the left. When offset
guiding in position 3, this remains the same. The slit runs left-right
on the guide camera. At a position angle of 90 degrees, this means the
slit runs E-W. In position 4, the field size is roughly halved to
about 1 arcmin, so about half the total slit length is seen on the guide
camera at a given guide camera position. The guide camera may be moved by
the telescope operator on its stage to view locations farther along
the slit if necessary.
On the CCDs, with the TUB at position angle 90 degrees, north is right
and east is at the top for both red and blue sides. It could be
worse; at least these are simple rotations of most charts. The slit is
of course still E-W, so on the CCDs the slit appears vertical, with
east at the top, and dispersion is thus along the rows.
For different position angles of the TUB, the relative orientations of
the guide camera, slit and CCDs are unchanged, since they all move
together. The effect of going to a higher position angle (that is, in
the usual sense of north through east) is to rotate images on both the
guider and CCDs clockwise.