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System Description
The SSUSI mission sensor contains a line scanning
imaging spectrograph covering the far ultraviolet spectrum, and
high sensitivity, nadir viewing photometers operating at 630 nm
(with separate signal and background measurements) and 427.8 nm.
The scanning imaging spectrograph has two modes of operation. The
imaging mode produces horizon to horizon line scan images at five
simultaneous far ultraviolet wavelengths. In the spectrograph mode,
the entire far ultraviolet spectrum is downlinked at one selected
look angle (normally the nadir direction). The photometers are nadir
viewing, and operate only on the night side.
The SSUSI mission sensor consists of three major
subassemblies: the imaging spectrograph, the photometer, and the
support module. (See figure 1 for
block diagram. See figure 1a
for detailed diagram). The support module contains the processor,
control, and power switching circuitry required by the flight unit.
The size, weight, and power specifications for the three subassemblies
are listed in Table 2. Because of the irregular footprint of the
imaging spectrograph, the maximum footprint dimensions are listed.
The maximum height of the spectrograph is listed, which occurs when
the cover is open.
| Table 2. SSUSI Physical Characteristics |
| Subassembly |
Footprint (in.) |
Height (in.) |
Weight (lbs.) |
Peak Power (Watts) |
| Imaging Spectrograph |
28.8 x 12.8 |
11.6 |
22 |
10 |
| Photometer |
12.3 x 8 |
10 |
9 |
10 |
| Support Module |
15 x 8 |
8 |
13 |
15 |
| SSUSI Total |
- |
- |
44 |
35 |
Imaging Spectrograph Design and Operation
The scanning imaging spectrograph (SIS) subassembly
consists of a cross track scanning mirror at the input to the telescope
and spectrograph optics. At the focal plane of the spectrograph
are redundant two-dimensional photon-counting detectors. The detectors
employ a position sensitive anode to determine the photon event
location. While not quite correct, we refer to the quantization
of the position determination on the detector as defining a "pixel".
The resolution of the detector can be increased by increasing the
detector gain (see Section 3).
The imaging spectrograph builds multispectral images
by scanning spatially across the satellite track (see
Figure 2). One dimension of the detector array contains 16 spatial
pixels (along the spacecraft track), and the other dimension consists
of 160 spectral bins over the range of 115 to 180 nm. The scan mirror
sweeps the 16 spatial pixel footprint from horizon to horizon perpendicular
to the spacecraft motion, producing one frame of 16 cross-track
lines in 22 seconds. Simultaneous image frames are generated over
the entire wavelength range in the imaging mode, but the data rate
allocation limits the downlinked image data to five different wavelength
intervals or "colors".
The imaging mode scan cycle consists of a limb
viewing section followed by an Earth viewing section. Limb viewing
pixels are collected from -72.8° from nadir (the start of scan)
to -63.2° from nadir. The limb viewing section has a cross track
resolution of 0.4° per pixel, and consists of 24 cross track pixels
by 8 along track pixels at five wavelengths. The 8 along track pixels
are formed by co-adding adjacent pixels in the 16 spatial pixel
footprint. At -72.8° from nadir and a spacecraft altitude of 830
km, the spectrograph will view approximately 520 km above the horizon.
One should note that the same pixel on the limb is resampled three
times on each orbit due to the wide horizontal field-of-view.
The Earth viewing section has a cross track resolution
of 0.8° per pixel, and always contains 16 along track pixels and
five colors. The number of cross track pixels depends on whether
the spacecraft is flown with a GLOB (Glare Obstructor). Currently,
only the noon-midnight orbit does not fly with a GLOB. With no GLOB,
a full Earth scan from -63.2° from nadir to +61.6° from
nadir is performed, and contains 156 cross track pixels. If the
GLOB is present, then a reduced scan from 63.2° from nadir
to +42.4° from nadir is performed, with 132 cross track pixels.
In the spectrograph mode, the scan mirror is held
at a fixed viewing angle (normally either the nadir direction for
"ground truth" or on the limb for star calibrations). The along
track dimension of the detector array is binned into 6 spatial pixels.
Spectral data from all 160 bins are produced for the 6 spatial pixels
every 3.0 seconds. The six spatial pixels are contained within the
center most 8.88 degrees of the 11.84 degree instantaneous along
track field of view. The 6 along track pixels are formed by co-adding
adjacent pixels in the center most 12 of the 16 spatial pixel footprint.
The entire spectrum, consisting of all 160 bins, can be downlinked
in the allocated "spare" words in the OLS data stream. We only send
down the central six pixels since for this orbit (830km altitude
- circular) the FOV moves about one pixel in three seconds. The
spectrograph mode (in which the entire spectrum is downlinked) would
be used predominantly during stellar calibration operations and
for "ground truth" campaigns in which we will stare at the radiating
volume above a ground site.
The imaging spectrograph contains three entrance
slits of varying widths. The intermediate width slit is intended
for use during imaging mode operation. The widest slit would be
used in imaging mode to increase the sensitivity should the optical
efficiency of the system decrease over time or to minimize the statistical
error for low count rate scenes such as when the FUV nightglow is
to be observed. The narrowest slit improves the spectral resolution.
Any slit can be used in any mode of operation. Furthermore, the
slit mechanism is designed so that two motors must fail (they are
independent) in a specific (i.e. "closed") mode in order for the
aperature to be "shuttered". The expected "failure" mode would be
one that would leave us with a fixed slit.
Table 3 summarizes the SIS performance characteristics.
Note that normally imaging mode uses the 0.30 deg slit and that
to reduce the size of the table we have indicated the "normal" slit
for the spectrograph mode as being the narrowest (.18 deg) even
though any one of the three slit widths can be used for either of
the two modes.
| Table 3. SSUSI Imaging Spectrograph
Performance Characteristics |
| Parameter |
Imaging (full scan) |
Imaging (reduced) |
Spectrograph |
| Instantaneous Field of View |
cross track (normal mode) |
0.30 deg |
0.30 deg |
0.18 deg |
| (wide slit) |
0.74 deg |
0.74 deg |
0.74 deg |
| along track |
11.84 deg |
11.84 deg |
11.84 deg |
|
| Pixel Field of View |
Earth Limb |
cross track (normal) |
0.30 deg |
0.30 deg |
- |
| along track |
1.48 deg |
1.48 deg |
- |
| Earth Disk |
cross track (normal) |
0.30 deg |
0.30 deg |
0.18 deg |
| along track |
0.74 deg |
0.74 deg |
1.48 deg |
|
| Scanned Field of View |
Earth Limb |
cross track |
9.6 deg |
9.6 deg |
- |
| step resolution |
0.4 deg |
0.4 deg |
- |
| Earth Disk |
cross track |
124.8 deg |
105.6 deg |
- |
| step resolution |
0.8 deg |
0.8 deg |
0.8 deg |
|
| Spatial resolution at nadir |
cross track |
10 km |
10 km |
2.3 km |
| along track |
10 km |
10 km |
20 km |
|
| Pixel Step Period |
Earth Limb |
0.112 sec |
0.156 sec |
- |
| Earth Disk |
0.112 sec |
0.112 sec |
- |
|
| Spectral Resolution |
narrow slit |
1.2 nm |
1.2 nm |
1.2 nm |
| normal slit |
1.9 nm |
1.9 nm |
1.2 nm |
| wide slit |
4.2 nm |
4.2 nm |
4.2 nm |
|
| Sensitivity (counts/sec/Rayleigh) |
121.6 nm |
0.016 |
0.016 |
0.019 |
| 130.4 nm |
0.120 |
0.120 |
0.144 |
| 135.6 nm |
0.160 |
0.160 |
0.192 |
| 140-150 nm |
0.160 |
0.160 |
0.192 |
| 165-180 nm |
0.020 |
0.020 |
0.024 |
|
| Data Frame |
Data Rate |
3816 bits/sec |
3816 bits/sec |
3816 bits/sec |
| Data Frame Period |
22 sec |
22 sec |
3.0 sec |
|
| Spatial pixels per frame |
Earth Limb |
cross track |
24 |
24 |
- |
| along track |
8 |
8 |
- |
| Earth Disk |
cross track |
156 |
132 |
1 |
| along track |
16 |
16 |
6 |
|
| Output Word Size |
Earth Limb |
6 bits |
7 bits |
- |
| Earth Disk |
6 bits |
7 bits |
10 bits |
The SIS consists of a cross-track scanning
mirror at the input to a telescope (a 75mm focal length off-axis
parabola system with a 25mmx50mm clear aperature) and a Rowland
circle spectrograph. The SIS is an f/3 system with a spherical
toroidal grating. The optical path incorporates baffles to prevent
stray light from reaching the focal plane at the slit and the detector.
The telescope mirror can not see any surfaces, other than baffle
knife edges, that are illuminated by sources beyond the entrance
opening of the spectrograph. The optical surfaces are coated with
ARC Coating #1200 or ARC Coating #1600 to tune the system performance
to the observational requirements of Table 1.
Figure 3 shows two views of the SIS. Figure
3a is a schematic side view. The scan mirror feeds the off-axis
parabola and the spherical toroidal grating. Two detectors lie at
the focal plane. Figure 3b shows a
labeled photo of the SIS SN01 housing.
SIS DETECTOR
The imaging spectrograph includes two, redundant
detectors. Either one can be used since the pop-up mirror, which
enters the optical path when the second detector is to be used,
is retractable. Only one detector is operated at a time. The detector
characteristics are listed in Table 4. The use of the secondary
detector will lower the sensitivity of the imaging spectrograph
due to the extra reflection of the pop-up mirror. The sensitivity
with the secondary detector in place will be approximately 75% of
the sensitivity with the primary detector since the pop-mirror has
the ARC #1200 MgF2 overcoat. The sensitivities listed
in Table 3 are for the primary detector.
The detector consists of a microchannel plate intensifier
with a wedge and strip anode. Since maintanence of performance specifications
over the mission lifetime is a design driver, the HVPS is commandable
so that the detector gain can be maintained at 4x10 even at a charge
extraction rate as high as 10Coulomb/yr.
| Table 4. UV Detector
Characteristics |
| Minimum Frame period |
0.112 seconds |
| Maximum Count Rate |
200 K counts/sec |
| Photocathode |
Cesium Iodide deposited on MCP front surface |
| Input Window |
Magnesium Fluoride |
| Detector size |
25 mm diameter |
| MCP Arrangement |
Z stack (3 plates) |
| Anode |
Wedge and Strip, 3 electrode |
| Quantum efficiency |
10 % at 135 nm |
| Supplier |
SAIC/EVSD Model T221-001 |
| Position resolution |
  spatial dimension |
16 elements across 16.5 mm |
|   spectral dimension |
160 elements across 15.6 mm |
| Output |
4 bit by 8 bit photon position |
| High Voltage Power Supply |
adjustable for variable gain |
| Mean Gain |
4x106 electrons/photon |
| Power |
3 Watts |
| Weight |
4 lbs |
| Qualification Temperature |
-29 deg C to +50 deg C |
NADIR Photometer SYSTEM (NPD) Design and operation
The NPS operates only on the nightside. It is intended
to provide the height of the F-region ionosphere and to corroborate
the characteristic energy and flux of precipitating electrons in
the aurora as determined by the SIS 2,6. To do this, three detectors
are required for the SSUSI photometer subsystem. The detectors will
be identical except for the optical filter characteristics. For
427.8 nm observations, one detector is required with a fixed wavelength
filter at 427.8 nm with a bandwidth of 5.0 nm. Two detectors are
required for the 630 nm observations because a correction must be
made for the Earth albedo and the contribution from backscattered
moonlight and starlight. One detector will have a filter with a
center wavelength of 630 nm and a bandwidth of 0.3 nm, and the detector
measuring background will use a filter with a center wavelength
of 629.4 nm and a bandwidth of 0.3 nm.
Each photometer unit includes an integrated detector
package consisting of a photomultiplier tube, high voltage power
supply, and pulse amplitude discriminator electronics. The performance
characteristics for the SSUSI photometers are listed in Table 5.
The photometer detector characteristics are listed in Table 6.
|
Table 5. Photometer Performance Characteristics |
| Parameter |
Unit #1 |
Unit #2 |
Unit #3 |
| Pixel Field of View - full angle, circular |
2.0 deg |
2.0 deg |
2.0 deg |
| Spatial resolution at nadir |
25 km |
25 km |
25 km |
| Center Wavelength |
427.8 nm |
630 nm |
629.4 nm |
| Spectral Bandwidth |
5.0 nm |
0.3 nm |
0.3 nm |
| Optic diameter |
0.5 inch |
2 inch |
2 inch |
| Pixel Integration Time |
1.0 sec |
1.0 sec |
1.0 sec |
| Sensitivity (cnt/sec/Rayleigh) |
5 |
30 |
30 |
| Maximum count per pixel |
500,000 |
100,000 |
100,000 |
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Table 6. Photometer Detector Characteristics |
| Parameter |
Unit #1 |
Unit #2 |
Unit #3 |
| Photocathode |
Bi-Alkali |
Tri-Alkali |
Tri-Alkali |
| Input Window |
Glass |
Glass |
Glass |
| Cathode diameter |
7 mm |
7 mm |
7 mm |
| Wavelength |
427.8 nm |
630 nm |
629.4 nm |
| Output signal |
pulse |
pulse |
pulse |
| Maximum count per sec |
500,000 |
100,000 |
100,000 |
| Dark count (maximum) |
40 cps |
40 cps |
40 cps |
| HV inhibit |
100 millisec |
100 millisec |
100 millisec |
| Power |
0.5 Watts |
0.5 Watts |
0.5 Watts |
| Operating Temperature (in spec) |
-30°C to -20°C |
-30°C to -20°C |
-30°C to -20°C |
Each photometer unit contains an interference filter
in front of a collimator lens. The filter characteristics for the
three units are listed in Table 6. The interference filter temperature
coefficient must not exceed 0.03 nm/°C in order for the bandpass
to remain constant and controllable for Units 2 and 3. The filters
in all three units are mounted in a thermal control fixture to maintain
wavelength stability. Each photometer filter employs a thermostatically
controlled heater to maintain an operating temperature range of
+25°C ± 1°C and the heater can be commanded on or off. .
The temperature gradient from the center to the edge of the filter
will not exceed 1° C. The filter temperature is monitored with
an accuracy of 1° C. Passive cooling is used to maintain an
operating flight range of -30 °C to -20 °C in order to reduce
the dark count rate.
The photometer baffle design received a good deal
of attention because the NPS may operate in a near-dusk environment,
. This environment is particularly difficult to model. In order
to be able to function at a solar zenith angle of 98deg, a two-dimensional
model of the twilight Rayleigh scattering radiation field was developed
10,11. The photometer has a glint zone of ±25 degrees and is located
on the shaded side of the spacecraft GLOB. The NPS has dual, redundant
illumination sensors. The illumination sensor triggers on earth
albedo and inhibit the photometer detectors by gating the HVPS.
The illumination sensor field of view is 10 degrees which provides
an adequate margin for the near-terminator orbits.
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