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Imaging Technique of the DISR Camera on the Huygens LanderJ.R. Kramm1, H.U. Keller1, R. Bredthauer2 and M. Tomasko31 Max-Planck-Institut für SonnensystemforschungKatlenburg-Lindau, Germany2 Semiconductor Technology Associates, Inc.San Juan Capistrano, CA3 Lunear and Planetary Laboratory,University of Arizona, Tucson, AZ MPS, June 20, 2005
Descent Imager/ Spectral Radiometer (DISR) Instrument Consortium Instrument responsibility: Manufacturing contractor: CCD Imager & electronics: CCD contractor: H/W compression: Infrared detector: LPL, Tucson, AZ Lockheed Martin, Denver, CO Max-Planck-Institut, Germany Loral, Newport Beach, CA Univ. Braunschweig, Germany Observatoire de Paris, France • Scientific Objectives • Medium and high-resolutions Imaging of the surface of Titan • Imaging of clouds and haze at Titan • Spectral investigations, 350 – 1700 nm • Solar Aureole, 500 and 935 nm, horiz. and vertical polarization
DISR Instrument Characteristics • 14 optical apertures total • 9 optical apertures to 1 CCD detector • 1.1 Watt for the CCD, 512 x 256 pixels • Date rate: 8 kbit/s, ~ 1 bit per pixel • 6 years for design, production and calibr. • 7.5 years travel time to Titan, 1997-2005 • 150 min total operation time envisaged • 220 min operation completed • 600 Images acquired + Spectra etc.
The Loral Max-Planck CCD Approach • Dedicated buried channel design for DISR / Max-Planck • Front side illuminated Frame Transfer CCD • 2 phase MPP clocking • Image and Memory sections 256 rows, 512 (+8 dark) columns • Gated lateral anti-blooming, also electronic shutter • 23 μ pixel pitch (17μ x 23μ active area) • Pixel capacity 150,000 e‾ (100,000 e‾ used) • QE up to 50 %, CTE = .999 999 • Line transfer 2 μs/line low image smear on shift • Single stage output amplifier,5- 8 electrons @ 70 kHz • OP16 JFET preamp on Sensor Head Board - (MPS) • Electronics Assembly holds CDS, clock drivers and 12 bit ADC • CCD shielded by 4 mm tungsten to prevent < 62 MeV protons • DISR CCD was also used for Imager for Mars Pathfinder (IMP)and 2x for Mars Polar Lander (Stereo and Robotic Arm Camera)
DISR Bias Frames Imager Bias Frames, 0 ms exposure, 260 K, and MRI Column Amplitude from 1994, 2000, 2005 Dark charge increase approx. 60x upon proton irradiation from a plutonium heater 10 cm apart from the Sensor Head (1997-2005).
CCD Operation Temperature Profile and Dark Charge Temperature Scale
In-flight Irradiation Effects In-flight proton irradiation from a nuclear heater located close to the CCD (~10 cm) Resulting effects: • Perfect thermal balance established • Dark charge increase about 60x with minor effects(low temperature, short exposure times, 7 to 50 ms) • CTE degradation