Like the G230L
grating, the G230M
grating is used with the NUV-MAMA
; it has a spectral range from 1650-3100 Å, however, with a resolving power R~10,000 a single exposure with the G230M
grating covers only 90 Å, and the grating must be scanned, with a series of exposures taken at 18 distinct settings to cover the full spectral range.
The G230M
grating mode is designed for observations where spatially resolved, long slit, spectroscopy is desired at relatively high spectral resolution covering a limited region of the near-ultraviolet spectrum.
Notice that the CCD G230MB
grating mode also covers the near-ultraviolet with comparable resolution. See Comparison of G230MB and G230M for a detailed comparison of these two grating modes in that wavelength regime.
Point source sensitivity assumes full transmission (zero slit losses). Diffuse source sensitivity assumes a 0.1" wide slit. To convert point source sensitivities to diffuse source sensitivities multiply the point source values by the grating spatial (cross dispersion) plate scale in units of arcseconds per pixel and by the width of the desired slit in units of arcseconds.
The top axis displays constant F values corresponding to the STMAG units (V+STMAG) on the bottom axis. Recall that STMAG=0 is equivalent to F = 3.63E-9 erg cm-2 s-1 Å-1. The curves are labeled with exposure times in seconds.
Figure 13.36: Diffuse Source Signal-to-Noise as a Function of STMAG for G230M
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