MMIRS Observing
MMIRS
Detector:

Field-of-view: 6.9 x 6.9 arcmin
Pixel scale: 0.202 arcsec/pix (optical layout)
Detector: 2048 x 2048 pix, HgCdTe Hawaii-2
Electronics gain: 10 e-/DN
Read-noise: 16 e-
Full well: ~230,000 e-, or 23,000 DN
Linearity: Linearity correction is required; usable to 20,500 DN (90% of full well).
Dark current: 0.05 e-/s/pix at 83 K (depends on final operating temperature).
Readout: 32 channels at 180 kHz; 0.7 sec for a single read.
Data Acquisition Strategy: The HAWAII-2 is a CMOS device that reads non-destructively. Thus there is no shutter. Images are obtained by differencing a pair of reads N seconds apart ("double-correlated sampling"), or, better, by taking multiple reads and then fitting a linear slope to each pixel ("up-the-ramp sampling"). Up-the-ramp sampling can measure count rates for pixels that saturate or have cosmic rays hits during an exposure.

Bad Pixel Mask Dark Frame K-band Flat Field
bad pixel mask dark frame flat-field

Imaging: Exposure Time Calculator

Exposure times: Must be integer seconds >= 1 sec.
Filters: Y (data), J (data), H (data), K (data), and a Dark position.
Focus: Provided by wavefront sensor; f/5 focus changes on ~10 minute time-scales at the MMT.
Sky Background: Dominated by narrow OH emission lines and broad H2O absorption bands (additional discussion).
Readout overhead: 5 sec total overhead per exposure, including 30 arcsec telescope dither.
Guiding: Images are unguided.
Observing Strategy: Long integrations are made from a series of short exposures, otherwise the night sky quickly saturates the detector (see Imaging Senstivity table). Images are obtained in a dither sequence. Sky background is measured, and removed, by median-combining a set of dithered images. This works well for sparse fields and point sources, however observations of extended objects require dithering on an OFF field to measure the sky background. Worked example.

Imaging Sensitivity
Magnitude of Point Source
(Vega mag) with S/N=10.
Time [sec] Y J H K
60 20.3 20.1 19.5 18.8
300 21.2 21.0 20.4 19.7
3600 22.5 22.4 21.7 21.0
Exposure time for sky
background to reach half
of saturation [sec]
500 300 40 55
Total System Throughput 0.23 0.24 0.51 0.40


Spectroscopy:

Full field for Spectroscopy: 4 x 6.8 arcmin
Field for Complete Spectra: 2 x 6.8 arcmin
Number of slitlets: Up to 40 slitlets, assuming a minimum length of 10 arcsec
Long Slits available:420 x 0.2, 0.4, 0.6, 0.8, 1.2, 1.6, 2.4 arcsec
Dispersed spectrum: Approx 1400 pixels long, with the available grisms
Calibration lamps: Continuum, Argon
Telluric calibration: Bright G dwarf stars
Observing Strategy: Similar strategy as imaging, except that the target(s) must be dithered along the slit(lets). Exposure times can be much longer because the sky background is dispersed. In addition, argon lamp exposures are required at each pointing to perform wavelegth calibration. To remove telluric observation lines, observe a bright G dwarf star at identical airmass.

Available Grism
Grism Wavelength
Range (um)
grooves
/mm
Resolution
(0.4'' slit)
Theoretical
Efficiency
across band
HK 1.45-2.45 80 1300 55-80%
Planned future grism
R3K 0.9-2.45 62 3500 ~50%
Possible future grism
JH 0.95-1.82 94 1300 55-80%

S/N per resolution element at R=3000
Exposure Time (hrs) Magnitude J H K Jdark Hdark
1 15 118 142 109 125 165
1 17 35 36 22 46 61
2 17 50 51 31 66 86
4 17 71 72 44 93 122
1 19 7 7 4 13 18
2 19 10 9 5 19 25
4 19 15 13 7 27 35


SWIRC stats, perhaps applicable to MMIRS

Distortion: Very small (predicted 0.01% center-to-corner).
Cross-talk: None between quadrants; very little in channels within a quadrant.
Flat-fielding: Sky flats give ~2% accuracy across chip, excluding high dark regions.
Cosmetics: The "scratch" and spot" cosmetics mask out well.

Questions? Contact wbrown@cfa.harvard.edu