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PACS Instrument Overview 1
SPIE 6265-09 24 May 2006Herschel Herschel PhotodetectorPhotodetector Array Camera & SpectrometerArray Camera & SpectrometerAlbrecht Poglitsch, MPE Albrecht Poglitsch, MPE GarchingGarching
Christoffel Waelkens, Katholieke Universiteit Leuven
Otto H. Bauer, Max-Planck-Institut für extraterrestrische Physik
Jordi Cepa, Instituto de Astrofísica de Canarias
Helmut Feuchtgruber, Max-Planck-Institut für extraterrestrische Physik
Thomas Henning, Max-Planck-Institut für Astronomie
Chris van Hoof, Interuniversity Microelectronics Center Leuven
Franz Kerschbaum, Institut für Astronomie der Universität Wien
Dietrich Lemke, Max-Planck-Institut für Astronomie
Etienne Renotte, Centre Spatial de Liège
Louis Rodriguez, Commissariat a l'Energie Atomique
Paolo Saraceno, Istituto di Fisica dello Spazio Interplanetario
Bart Vandenbussche, Katholieke Universiteit Leuven
PACS Instrument Overview 2
SPIE 6265-09 24 May 2006
Instrument Concept• Imaging photometry
– two bands simultaneously (60-85 or 85-130 µm and 130-210 µm) with dichroic beam splitter
– two filled bolometer arrays (32x16 and 64x32 pixels, full beam sampling)
– point source detection limit~4 mJy (5σ, 1h)
• Integral field line spectroscopy– range 57 - 210 µm with 5x5
pixels, image slicer, and long-slit grating spectrograph (R ~ 1500)
– two 16x25 Ge:Ga photoconductor arrays (stressed/unstressed)
– point source detection limit 3…20 x10-18 W/m2 (5σ, 1h)
Focal Plane Footprint
32 x 16 pixels6.4” x 6.4”
64 x 32 pixels3.2” x 3.2”
PACS Instrument Overview 3
SPIE 6265-09 24 May 2006
Instrument Concept• Imaging photometry
– two bands simultaneously (60-85 or 85-130 µm and 130-210 µm) with dichroic beam splitter
– two filled bolometer arrays (32x16 and 64x32 pixels, full beam sampling)
– point source detection limit~4 mJy (5σ, 1h)
• Integral field line spectroscopy– range 57 - 210 µm with 5x5
pixels, image slicer, and long-slit grating spectrograph (R ~ 1500)
– two 16x25 Ge:Ga photoconductor arrays (stressed/unstressed)
– point source detection limit 3…20 x10-18 W/m2 (5σ, 1h)
Focal Plane Footprint
32 x 16 pixels6.4” x 6.4”
64 x 32 pixels3.2” x 3.2”
PACS Instrument Overview 4
SPIE 6265-09 24 May 2006
Observing Modes• Combinations of instrument modes and satellite pointing
modes• Instrument modes:
– photometry (dual-band) – line spectroscopy
• observation of individual lines
– range spectroscopy• observation of extended wavelength ranges
• Pointing modes:– stare/raster/line scan– with/without
nodding/off-position
• Internal chopper– background subtraction– calibration
4
PACS Instrument Overview 5
SPIE 6265-09 24 May 2006
FPU/Optics
sGeGaDetectorRed Spectrometer
Blue Bolometer
Red Bolometer
Calibrator I and II
0.3 K Cooler
Filter Wheel I
Filter Wheel II
Grating
GeGa DetectorBlue Spectrometer
Encoder
Grating Drive
Entrance Optics
PhotometerOptics
Calibrator Optics
SlicerOptics
SpectrometerOptics
Chopper
PACS Instrument Overview 6
SPIE 6265-09 24 May 2006
FPU-Optics
PACS Instrument Overview 7
SPIE 6265-09 24 May 2006
FPU-Optics
FPU
PACS Instrument Overview 8
SPIE 6265-09 24 May 2006
FPU Subunits Picture Gallery
PACS Instrument Overview 9
SPIE 6265-09 24 May 2006
CRE
• Two 25x16 pixel filled arrays• Extrinsic photoconductors (Ge:Ga, stressed/unstressed)• Integrated cryogenic
readout electronics(CRE)
• Near-background-noise limited performanceexpected
Photoconductor Arrays (Spectrometer)
CRE details: Merken et al. [6275-43]
PACS Instrument Overview 10
SPIE 6265-09 24 May 2006
CRE
• Two 25x16 pixel filled arrays• Extrinsic photoconductors (Ge:Ga, stressed/unstressed)• Integrated cryogenic
readout electronics(CRE)
• Near-background-noise limited performanceexpected
Photoconductor Arrays (Spectrometer)
CRE details: Merken et al. [6275-43]
PACS Instrument Overview 11
SPIE 6265-09 24 May 2006
Detector Performance
0
0.2
0.4
0.6
0.8
1
1.2
0 50 100 150 200 250 300wavelength [µm]
rela
tive
spec
tral r
espo
nsiv
ity
• Distribution of spectral response within modules
• Distribution of photometric response within modules
• Distribution of absolute photometric responsivitybetween modules
Mean Responsivity of FM HS Detector Modules for Bias=70mV
0
10
20
30
40
50
60
70
80
FM15
3
FM15
8
FM15
9
FM16
0
FM16
1
FM16
2
FM16
4
FM16
5
FM16
8
FM16
9
FM17
0
FM17
1
FM17
3
FM17
4
FM17
5
FM17
9
FM18
0
FM18
1
FM18
3
FM18
4
FM18
6
FM18
7
FM18
8
FM18
9
FM19
0
r [A
/W]
0
0.2
0.4
0.6
0.8
1
0 2 4 6 8 10 12 14 16pixel number
rela
tive
resp
onsi
vity
PACS Instrument Overview 12
SPIE 6265-09 24 May 2006
Detector/CRE Performance
• Near background-noise limited performance with peak DQE=0.26 achievable for high-stress detectors with FM CREs
• Analysis of proton tests on HS module indicates no significant excess noise with optimized modulation scheme, IR curing works as well as thermal curing
Mean NEP at 1.85K, C=0.14pF, P=4.2e-15W
0
1E-17
2E-17
3E-17
4E-17
5E-17
6E-17
7E-17
8E-17
0 20 40 60 80 100
bias [mV]
W/√
Hz
FM153FM160FM164FM188FM189FM190
Mean NEP at 1.85K, C=0.14pF, P=2.4e-15W
0
1E-17
2E-17
3E-17
4E-17
5E-17
6E-17
7E-17
8E-17
0 20 40 60 80 100
bias [mV]
W/√
Hz
FM153FM160FM164FM188FM189FM190
Measurement with lab equipment (not optimized for noise)
PACS Instrument Overview 13
SPIE 6265-09 24 May 2006
Background- vs. Readout Noise
20 30 40 50 60 70 800
0.5
1
1.5
2
2.5
bias [mV]
signal Circles:measured noise
Dashed line:CRE noise
Squares:CRE noise subtr.
Solid lines:combined model
Dotted lines:background noise
20 30 40 50 60 70 800
0.002
0.004
0.006
0.008
noise
bias [mV]
4.7x10-15 W2.9x10-15 W
• Observed noise explained as photon noise + CRE noise• S/N (of photon noise) requires QE=0.26• With observed noise of readout (integrated with detector), near-BLIP
for HS (red) array expected, but (most likely) not for LS (blue) array
PACS Instrument Overview 14
SPIE 6265-09 24 May 2006
Operation/Performance under p+ Irradiation
NEP as a function of detector/readout setting Simulated chopped observation with one ramp/chopper plateau.For each bias value, 5 ramp lengths tested: 1s, 1/2 s, 1/4 s, 1/8s, 1/16 s.The detector was in its high responsivity plateau, ~2 hours after the last curing.
Instrument model value,based on lab measurementswithout irradiation
• With optimum bias setting (lower than in lab!) and ramp length /chopping parameters, NEP close to lab values possible in space
• Curing may be necessary only after solar flare, or once per day (self-curing under telescope IR background sufficient)
Further details: Katterloher et al. [6275-42]Stegmaier et al. [6265-89]
PACS Instrument Overview 15
SPIE 6265-09 24 May 2006
Bolometer Arrays (Photometer)
• Two filled arrays: 64x32 pixels (blue) and 32x16 pixels (red)• Bolometers and multiplexing readout electronics operating at 0.3K• Detector/readout noise comparable to background-noise (FM)• Cooler hold time ~59h
Pixel
Bluefocal plane
Photometer unitwith blue + red
focal planesand 3He cooler
PACS Instrument Overview 16
SPIE 6265-09 24 May 2006
FM Blue BFP Performance
• Pixel yield ~98%• NEP ~1.7 x BLIP
– But 1/f noise– Best NEP only for fast
modulation (chopping/ scanning)
Further details: Billot et al. [6265-11]Simoens et al. [6275-01]
PACS Instrument Overview 17
SPIE 6265-09 24 May 2006
FM Blue BFP Performance
• Pixel yield ~98%• NEP ~1.7 x BLIP
– But 1/f noise– Best NEP only for fast
modulation (chopping/ scanning)
Further details: Billot et al. [6265-11]Simoens et al. [6275-01]
PACS Instrument Overview 18
SPIE 6265-09 24 May 2006
Grating Efficiency Verification0th ORDER (INCIDENT AND REFLECTED RAYS @ 19°)FTS MEASUREMENTS AND THREE CALCULATIONS USING PCGRATE
0
10
20
30
40
50
60
70
80
90
100
30 50 70 90 110 130 150 170 190 210
wavelength (mu)
Effic
ienc
y (%
) DE( 0) 200 prec UNPOL
Balance 200 prec UNPOL
DE( 0) 100 prec UNPOL
Balance 100 prec UNPOL
DE( 0) 100 prec UNPOL (detail)
Balance 100 prec UNPOL (detail)
GRATING MEASUREMENT
• Measurement done on production sample in different optical configuration than PACS; however, it gives strong indication that– Grating groove profile is correct– Numeric E&M model prediction is correct
PACS Instrument Overview 19
SPIE 6265-09 24 May 2006
Filter Performance
Wavelength [ µm]
Filte
r tra
nsm
issi
on
50 60 70 80 90 100 110Wavelength [ µm]
Filte
r tra
nsm
issi
on
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
Wavelength [ µm]
Filte
r tra
nsm
issi
on
100 120 140 160 180 200 220 240 260
Wavelength [ µm]
Filte
r tra
nsm
issi
on
Wavelength [ µm]
Filte
r tra
nsm
issi
on
Wavelength [ µm]
Filte
r tra
nsm
issi
on
70 80 90 100 110 120 130 140
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
80 100 120 140 160 180 200 2200
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
50 60 70 80 90 100 110 1200
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
50 55 60 65 70 75 80 85 90
Spec
trom
eter
P
hoto
met
er
• Requirement of 40% in-band transmission fulfilled or exceeded in most bands
PACS Instrument Overview 20
SPIE 6265-09 24 May 2006
QM Instrument Test: Optical Performance
“+” beam “-” beam
Blue photometer, chopped/nodded
• Source: ~ diffraction PSF size hole mask in front of external blackbody, contrast ~1%of background
• PSF wider than expected (25-45%); attributed to defocus of test optics
• Lower limit to spectral resolving power from measurement of saturated water lines ok
Wavelength [µm]
BlueSpectrometer
R>1500
Water spectrum(lab air)
Blue spectrometer, partial x-y rasterof focal plane
PACS Instrument Overview 21
SPIE 6265-09 24 May 2006
QM Instrument Test: Photometer Flatfield
CS1CS2 BB1
BB1 (contrast up)
BB2
BB2 (contrast up)
• Chopper scan over full FoV, including internal calibration sources• Chopper scan over full FoV, including internal calibration sources• Illumination: cryogenic BB sources at 2 temperatures• Flatfielding algorithm (through redundant observations) works• Structure/spots in optics (filters? mirrors?) revealed
– elimination by dithering/scanning with satellite
PACS Instrument Overview 22
SPIE 6265-09 24 May 2006
QM ILT: Calibration Sources Performance
• Emissivity– Measured against
cryogenic OGSE blackbody
– Values are within specified range.
– But CS 1 value is likely off due to inhomogeneity
• Homogeneity– Ok for CS 2
CS 2 CS 1
Chopper deflection angle
PACS Instrument Overview 23
SPIE 6265-09 24 May 2006
Predicted Instrument Performance
• Calculated optical efficiencies– telescope main beam (diffraction + WFE)– grating in respective diffraction orders– diffraction losses due to IFU (image slicer)
0
0.2
0.4
0.6
0.8
Wavelength [µm]
Tele
scop
e ef
ficie
ncy
Wavelength [µm]60 80 100 120 140 160 180 200
0
0.2
0.4
0.6
0.8
Diff
ract
ion
thro
ughp
ut
60 80 100 120 140 160 180 20060 80 100 120 140 160 180 2000
0.2
0.4
0.6
0.8
Wavelength [µm]
Gra
ting
effic
ienc
y
PACS Instrument Overview 24
SPIE 6265-09 24 May 2006
Predicted Instrument Performance
0.00
0.10
0.20
0.30
0.40
0.50
0.60
0.70
50 100 150 200 250
PhotometerSensitivity
PhotometricBands
wavelength [µm]
filte
r tr
ansm
issi
on(10'x10'in 1 day)
on-array chopping/line scanning
off-position chopping
wavelength [µm]
[mJy
] (p
oint
sou
rce;
5σ/
1h)
50 100 150 200
5
4
3
2
1
0
60 80 100 120 140 160 1800
1000
2000
3000
4000
5000
SpectrometerResolving power
wavelength [µm]
wavelength [µm]
60 80 100 120 140 160 180 2000
5.10 18
10.10 18
15 .10 18
20.10 18
SpectrometerSensitivity [W/m2](5σ, 1 hour)
(…but cosmic rays)
PACS Instrument Overview 25
SPIE 6265-09 24 May 2006
Observing Modes and AOTs
• Point source photometry– Targeted at observations of sources which are completely
isolated and point-like or smaller than one blue matrix. This AOT uses chopping and nodding, both with amplitude of 1 blue matrix, and dithering with a 1 pixel amplitude, keeping the source on the array at all times.
PACS Instrument Overview 26
SPIE 6265-09 24 May 2006
Observing Modes and AOTs
• “Small source” photometry– Targeted at observations of
sources that are smaller than the array size, yet larger than a single matrix. To be orientation independent, this means sources that fit in 2’ × 2’. This AOT uses chopping and nodding, but the source cannot be kept on the array at all times.
PACS Instrument Overview 27
SPIE 6265-09 24 May 2006
Observing Modes and AOTs
• Large area photometric mapping– This mode is necessary to map sources larger than the array
size, or to cover large contiguous areas of the sky (photometric surveys). There are two ways to perform this kind of observations:
• Scanning (without chopping)– Filled arrays allow arbitrary scanning orientation
• Rastering– Note: Rastering without chopping probably precluded
by 1/f noise
PACS Instrument Overview 28
SPIE 6265-09 24 May 2006
Observing Modes and AOTs
• Line Spectroscopy: observation of individual line(s)– Chop/nod or wavelength switching– POINTED: single satellite pointing– POINTED WITH DITHER: small spacecraft movements
perpendicular to the chopper direction to compensate for slicereffects in case of slightly mispointed targets
– MAPPING: limited to rectangular small regions with a maximum extension of 2.8 arcmin to allow for clean chopper off-positions for each raster point; fixed large chopper throw; map parameters in spacecraft coordinates
– Wavelength switching: For one spectral line, the grating will befrequently switched between on-line and off-line. The same pattern will be repeated a few times at slightly shifted wavelength
– Up to 10 lines can be specified in one observation, but all lines have to be reachable without a filter change
– Spectral sampling >3 samples/FWHM (by small up/down scan)– Minimum execution time: 192 s
PACS Instrument Overview 29
SPIE 6265-09 24 May 2006
Observing Modes and AOTs
• Range Spectroscopy: observation of extended range(s)– POINTED: single satellite pointing + chop/nod– POINTED WITH DITHER: small spacecraft movements
perpendicular to the chopper direction + chop/nod– MAPPING with chop/nod: limited to rectangular small regions with
a maximum extension of 2.8 arcmin to allow for clean chopper off-positions for each raster point; map parameters in spacecraft coordinates
– MAPPING with off-position: crowed fields and extended spectral structures; chopping between sky and internal CS; map parametersin sky coordinates.
– Up to 10 (freely defined) ranges can be specified in one observation, but all lines have to be reachable without a filterchange
– Spectral sampling: high (>3 samples/FWHM)Nyquist (optimized for speed; minimum timefor full first+second order scan: 1440 s)
PACS Instrument Overview 30
SPIE 6265-09 24 May 2006
Observing Modes and AOTs
• SED Mode: full PACS wavelength range with Nyquist sampling– Full grating scan in first order, which covers also the complete
second order in Nyquist sampling. Then, a filter switch is required, followed by a full scan of the third order (+ part of first order)
– POINTED: single satellite pointing + chop/nod– POINTED WITH DITHER: small spacecraft movements
perpendicular to the chopper direction + chop/nod– MAPPING with chop/nod: limited to rectangular small regions with
a maximum extension of 2.8 arcmin to allow for clean chopper off-positions for each raster point; map parameters in spacecraft coordinates
– MAPPING with off-position: crowed fields and extended spectral structures; chopping between sky and internal CS; map parametersin sky coordinates
– Minimum execution time: 2280 s
PACS Instrument Overview 31
SPIE 6265-09 24 May 2006
How to Estimate Observing Times?
• Under preparation: HSPOT (developed from Spitzer SPOT) will give accurate time budgets
• Now: A simple ‘Time Guesstimator’ is available for feasibility checks and rough estimates, follow the link ‘Time Guesstimator’ at http://pacs.ster.kuleuven.ac.be/
• Be aware of confusion limits! (0.6, 3, 11mJy)