As a measure of the RGS sensitivity the detection threshold for a few prominent lines in the 0.35-2.5 keV range has been modeled using SciSim. As examples, the following lines were chosen: the O VII line complex (at 0.57 keV), the Ne X line (at 1.022 keV) and the Si XIII line (at 1.86 keV). The RGS line sensitivity plots displayed in Figs. 55-57 provide an estimate of the exposure time necessary to detect a line above a certain underlying continuum at a significance level of 5-. The calculations were performed for one RGS. It is in all cases assumed that the line emission emanates from a point source.
The calculations are based on the line flux integrated over the HEW of the line profile, assuming Gaussian error propagation. For such an estimate, four contributing components must be considered:
The X-ray background varies over the sky. In order to provide a graphical representation of RGS's sensitivity which is independent of the source coordinates on the sky, the X-ray background was not considered directly. However, at the discussed energies the extragalactic X-ray background can well be reproduced by a power-law spectrum. This allows us to consider the X-ray background simply by adding an additional component to the continuum flux of the source. In general, the ``continuum flux'' in the plots can therefore be assumed to contain in practice a contribution from both the source continuum and the X-ray background at the position of the source.
The particle-induced background, which depends on the design of the instruments, is considered in the calculation of the curves. We assume a particle-induced background of counts mm-2 s-1 keV-1. This is a mean number, which accounts for the normal fluctuation in solar activity. For the given lines we assumed a geometrical area for particle hits of 7.2, 10.8 and 12.5 mm2.
The plots allow a first estimate of the exposure time in the sense that unreasonable sources can be rejected during a pre-selection of possible targets. They give a basic idea of whether or not it is possible to detect lines. They are not intended to (and cannot) substitute detailed simulations with realistic spectra with SciSim for sources where a detection and/or separation of one or more emission lines is the main scientific goal.