IR wide field imaging MPIA IR projects and studies
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Transcript of IR wide field imaging MPIA IR projects and studies
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 1
Stability of IR-arrays for robotized observations at dome C
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 2
IR wide field imaging
MPIA IR projects and studies • OMEGA2000: NIR WFI Calar Alto• NACO: NIR AO-supported Imager and Spectr. (VLT) • LUCIFER: NIR AO-supported Imager and Spectr. (LBT) • T-OWL study: TIR and MIR at a 100m telescope
– Science case– Atmospheric constrains– Technical realization
– Problems • MIDIR study: TIR and MIR at a 30m/42m/60m telescope
– Dito, especially for new E-ELT design
• PRIME/Dune (ESA Corner Stone) – All sky 0.5µm – 1.8µm survey– 4x0.5 square deg– 0.15/0.3 arcsec/pixel
• ARENA: TIR and MIR wide field – 0.18arcsec/pixel at J,H,K, 8 arrays Hawaii II – 0.18 arcsec/pixel at L,M 8 arrays InSb– 0.36 arcsec/pixel at N,M 8 arrays Si:As
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 3
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 4
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 5
Infrared Arrays
Company Type Pixel pitch Pixel number Wavelength range
Temperature
Teledyne Hawaii I 18 1024x1024 0.9 – 2.6 77K
Teledyne Hawaii I RG 18 2048x2048 0.9 – 2.6 77K
Teledyne Hawaii II RG 18 2048x2048 0.9 – 2.6 77K
Raytheon(SBRC)
VIRGO 20 2048x2048 0.9 – 2.6 77K
Teledyne Hawaii II RG 18 2038x2048 0.9 – 5.0 40K
Raytheon (SBRC)
Aladdin III InSb 27 1024x1024 0.9 – 5.4 23K
Raytheon (SBRC)
ORION InSb 25 2048 x 2048 0.9 – 5.4 23K
Raytheon (SBRC)
Si:As 50 320 x 240 2 – 28 3K
DRS (Boeing) Si:As BIB 50 256 x 256 2 – 28 3K
DRS (Boeing) Si:As BIB 75 126 x 126 2 - 28 3K
JPL Si:As 18 1024x1024 5-25 3K
Raytheon (SBRC)
Si:As 30 (tentative) 1024x1024 5-28 3K
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 6
MIR survey competitors Mission
Wise:
• cryogenic 40cm-telescope• 3.5, 4.7, 12, 23 µm bands simultaneously• 4x 1kx1k: 2 HgCdTe, 2 Si:As• pixel size:2.7arcsec
confirmation Oct 200650% budget reduction1m->40cm
Spitzer
JWST
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 7
Quantum efficiency of Hawaii-2 array #1005 in H-band
Dark current of Hawaii-2 array #1005
NIR
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 8
Mosaic of 2x2 2Kx2K λc =5 µm HgCdTe arrays
NIR/TIR
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 9
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 10
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 11
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 12
Readout noise as function of number of Fowler sample pairs.
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 13
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 14
Array Aladdin InSb (Hughes SBRC)
Pixel format 1024x1024 27-micron pixels
Spectral Response 1 to 5.5 microns
Dark Current 0.25 e-/s/pix
Dark Background 0.5 e-/s/pix
Read Noise (low background mode) 10 e-/pix
Read Noise (medium background mode) 35 e-/pix
Read Noise (high background mode) 70 e-/pix
Gain 12.3 e-/ADU
Well depth (near-IR) 200,000 e-
Well depth (thermal-IR) 280,000 e-
Quantum efficiency about 90%
Flat field uniformity* +/-18%
Flat field repeatability* +/-0.3%
Residual image retention0.5-1% of a bright (saturated) source in the next
frame
Centered Sub-array dimensions 768x768, 512x512, 256x256 pixels
Gemini (NIRI science array)
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 15
MIRI Assy 7581011.1 Wafer 9601/A05 & Assy 7581009.1 Wafer 9581/A05; Diodes D28 at -1.0 V Bias
0.01
0.10
1.00
0.0 5.0 10.0 15.0 20.0 25.0 30.0
Wavelength (µm)
Re
lati
ve
Re
sp
on
se
/ P
ho
ton
9601 @ - 1.0 volt
hanger queen @-1.0 volt
9581 @ -1.0 volt
10.0 K 9/22/2004
Relative quantum efficiency of MIRI detectors.
MIR
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 16
basic specifications of the Aquarius 1Kx1K Si:As array.
ParameterUnits specs
Pixel pitch µm 30
Number of video outputs 32
Maximum frame rate Hz 150
Storage capacity spectroscopy e- 1E6
Storage capacity imaging e- 1.5E7
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 17
Column shift register
Column shift register
Ro
w sh
ift register
8 or 32 outputs (selectable)
Column shift register
Column shift register
Ro
w sh
ift register
8 or 32 outputs (selectable)
Readout topology of Aquarius array.
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 18
320x240 CRC 774 Si:As array used for ground based instruments such as Michelle, Timmi2, TRECS, VLTI-MIDI, COMICS ...
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 19
How to produce Flat-fields at Dome C
• NIR: best choice: twilight flats sophisticated dome flats or instrumental flats calibrated by sky-flats, use variable DITs
• TIR/MIR: best choice: reconstruction from dithered science obs.
Dark current frames required!
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 20
Flat field Stability
Detector temperature should be stable within +/- 0.005 K. Relatively easy to meet by temperature controller (NACO, CRIRES, ISAAC...)
Stabilization of voltages typically within mV. Technically no problem if independent on external temperature variations (Temperature stabilization of electronics racks). d(ln Gain)/dT= (2-3)x10-4 /K
NIR flat field should be taken every 24h. MIR flat field is deduced from dithered images.
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 21
Special constrains at Dome-C
• Continuous use over years • Cold ambient • No maintenance in situ, no human intervention • Icing problem
• Solutions: CCC instead of LN2 and LHe, respectively
• Entrance window ventilation
Pulse tube cooler at higher frequencies to avoid orientation dependence instead of Stirling type or Gifford-McMahonTB specified for low ambient temperatures
Rainer LenzenMax-Planck-Institut für Astronomie, Heidelberg
27.3.2007, Tenerife Page Nr. 22
Long time Stability
Aging of IR arrays: 1. storage aging (near ambient temperature at non-operation state)2. thermo-cycling aging (“significant only after hundreds of cycles”)3. operational aging (not considering radiation damage for space
application)
Based on experience at Omega2000, CRIRES, NACO etc. (Gert Finger, H.-U. Käufl), operational aging of arrays is not observed over > 5years, neither QE nor hot/dead pixels.
Detector aging mainly due to thermal cycling (not a problem here)
Main problems arise from long time contamination of the detector due to bad vacuum conditions, power interruption, dust within the cryostat (black painting abrasion, Zeolith, etc.).
In consequence, special care should be taken in the design of the cryostat to avoid such long time problems.