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SSUSI: Instrument

 

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


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.