The optical design is based upon two parabolic mirrors, a plane mirror and a spherical concave grating, all made of silicon carbide. The first off-axis telescope parabola mirrors the Sun on the spectrometer entrance slit. The second off-axis parabola collimates the beam leaving the slit. This beam is then deflected by the plane mirror onto the grating. Two detectors, located in the focal plane of the grating, collect the monochromatic images of the spectrometer entrance slit. Coverage of the full spectral range of the instrument requires a wavelength scan performed by rotating the plane mirror. A baffle system, consisting of an entrance aperture, light traps, an aperture stop, a pre-slit and a Lyot stop, completes the design.
The Telescope: Focal length 1302.77 mm at 75°C Off-axis angle 4.5° Equivalent f-number 10.67 Plate scale in slit plane 6.316 µm/arcsec Total dynamic field-of-view 64 × 64 arcmin² Smallest step sizes 0.38 arcsec (N-S and E-W) The Slits: 1 × 300, 1 × 120, 0.3 × 120, 4 × 300 arcsec² The Rear-Slit Camera: Wavelength range 5770 - 6520 Å Array size 512 (spatial) pixels Pixel size 25 µm The Spectrometer: Wavelength ranges Detector A 390 - 805 Å (2nd order) * 780 - 1610 Å (1st order) Detector B 330 - 750 Å (2nd order) * 660 - 1500 Å (1st order) Collimator focal length 399.60 mm Off-axis angle 7° Grating radius 3200.78 mm Grating ruling 3600.42 lines/mm Magnification factor ** 4.092 at 800 Å in detector plane 4.407 at 1600 Å The Detectors: Array size 1024 (spectral) × 360 (spatial) pixels Pixel size (mean value) 26.5 × 26.5 µm² Angular scale 1.03 arcsec/px at 800 Å 0.95 arcsec/px at 1600 Å Spectral scale 22.3 mÅ/px at 500 Å (2nd order) * 21.0 mÅ/px at 800 Å 45.2 mÅ/px at 800 Å (1st order) 41.9 mÅ/px at 1600 Å* In the range below 500 Å the sensitivity is very low, because of three normal-incidence reflections. Strong lines have, however, been observed in this regime during the calibration phase and under operational conditions. Some lines have been observed in 3rd order.
** The magnification factor is the ratio of the effective grating focal length and the collimator focal length.