The HRI was a digital X-ray camera which provided high spatial and temporal resolution over the central 25 arcmin of the Einstein focal plane. The instrument had no inherent spectral resolution, but spectral studies could be performed using interchangeable broad band filters and Objective Grating Spectrometers (OGS). When operated with the OGS, the HRI had an energy resolution of 10-50. There were 3 HRI detectors onboard, identical except for the UV opaque shade material. The HRI had a 25´ diameter FOV, with a spatial resolution of 2" within 5´ of the axis. The effective area was 20 cm2 at 0.25 keV; 10 cm2 at 1 keV; and 5 cm2 at 2 keV. The time resolution was 8 msec. The energy range was 0.15-3.0 keV. The background was ~5 x 10-3 cts/arcmin2/ sec.
The SSS consisted of a cryogenically cooled lithium-drifted Si(Li) detector at the focus of an X-ray imaging telescope. It subtended a six arcminute diameter circular aperture, and was slightly defocused so that a point source was blurred to a radius of ~1 arcmin. The spectral resolution was noise-limited, with a 160 eV FWHM, and was nearly energy independent over the detector range 0.5-4.5 keV. There was 128 energy channel resolution, with each channel being about 45 eV wide. A time-dependent build-up of ice (water) on the detector surface occurred because of cryopumping of ambient outgassing material onto the 100 K detector. It was periodically defrosted by heating to 220 K at the beginning of a series of three days of observations. Each defrost reduced the total amount of ice that returned, such that after 9 months the ice covering was almost gone. A model had been developed that predicted the ice parameter as a function of time, and was used to obtain the correct response matrix for any given observation. The cryogen keeping the SSS at its operational temperature of 100 K ran out, as expected, in October 1979, between Day 276 (Oct 3) and Day 286 (Oct 13).
The Focal Plane Crystal Spectrometer (FPCS) was a Bragg crystal spectrometer with 6 different crystal diffractors and two redundant position-sensitive detectors which were multiwire proportional counters. The FPCS had a set of 4 apertures to select from, with dimensions of 1´ x 20´, 2´ x 20´, 3´ x 30´, and 6´ diameter, respectively. Only the latter three were actually used in observastions. The effective area of the FPCS was of order 0.1-1.0 cm2, and its energy resolution was 50-1000. In a typical FPCS observation, a small segment (20-80 eV) of spectrum would be obtained centered on a specific spectral feature by stepping the orientation of the selected crystal: features in the energy range from 0.42-2.6 keV were observed.
The MPC was a non-focal plane instrument that monitored the 1-20 keV X-ray flux of the source(s) being observed simultaneously by the operational focal plane instrument. The MPC was a collimated proportional counter filled with argon and carbon dioxide. It had a circular field of view, 1.5° in diameter (FWHM), which was co-aligned with the telescope. A 1.5 mil Be window sealed the gas in the detector and shielded the detector from ultraviolet radiation. The active area of the MPC was 667 cm2. Each photon detected by the MPC was pulse-height analyzed into one of 8 bins, the size of which increased logarithmically with energy from 0.41 keV, for the lowest energy bin, to 6.72 keV for the highest energy bin. The MPC had an energy resolution of ~20% at 6 keV. The MPC obtained useful data from 1978 November 19 until 1981 April 17, with the exception of a 3-month period from 27 Aug 1980 to 8 Dec 1980 when operation was intermittent, due to Einstein Observatory attitude control problems.
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