Array Type:
Rockwell 128x128 pixel high flux Si:As BIB array,
Wavelength range:
4 µm - 27 µm
Pixel pitch
75 µm
Active area fill factor
100% (focal plane architecture)
Quantum efficiency:
~ 31 %
Bad pixels:
~ 20
Dark current:
2 * 106 electrons/sec
Read noise:
1250 electrons - destructive read mode
Well capacity:
1.73 * 107 electrons
Telescopes:
The camera can be mounted on the
UKIRT
3.8 m telescope.
Pixel scales:
~ 0.27"/pixel
For high accuracy work, the scale and rotation angle should be measured
during your observing run.
Read out options:
dc
|
No chopper
The chip will be read '#Coadds' times, the frames will be added and the sum will be sent to the SunSparc. This will be reapeated '#Repeat' times. Eventually you will get '#Repeat' images. 'eff.IT:' shows the effective integration time per image = FT * #Coadds |
chop
|
The chopper runs:
---------- ---------- object | | | | | | ---------- ---------- sky =>send =>send object sky image imageevery '-' marks a read. The number of reads per chopper-plateau is defined by '#Coadds'. The eff. integration time is 'FT' * '#Coadds' (unit=seconds) per image. Eventually you will have 2 * '#Repeat' images in memory. The image-'display' and the FITS-files contain raw (integrated) data. Note: '#Plateaus' is usually set to '1'. This parameter allows you to add several chopper-plateaus using the hardware coadder. |
chop-d
|
The chopper runs and the readout-scheme is the same as in
'chop' mode. But only the differences of consecutive images (object-sky) are displayed and saved to disk. (-> you will get '#Repeat' difference-images) |
Data system:
Sun SPARC-20 dedicated to camera control. All data are written to disk
as FITS files, which are backed up via tar to a DAT tape.
Sensitivity:
@ 11.5 µm (filter N_11.5w2)
S/N ~ 10
source of 0.1 Jy (~ 6.2 mag)
60 sec on source
during the night of 16 Jan '96
@ Q band (filter Q)
S/N ~ 5
estimated source of 6.23 mJy
1 hour on source
extrapolated data obtained during the night of 29 Nov '96
Filter options:
all wavelength numbers are in microns @ 12 Kelvin
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* avg. Transmission: The avg. Transmission represents the average level of the plateau in the filter trace. There are usually regions of higher and lower transmission than the average.