3.3.12.1 EPIC spectral quality

In Figs. 43-47 we display a series of Mekal model spectra at different energies, ranging from 0.1 to 10.0 keV, with successively increasing total photon numbers (from 500 to 20000 counts). Although these figures have been created using on-ground calibrations, they can be still used as a qualitative reference for the expected spectral quality. These show which data quality can be reached for a given total number of counts. All model spectra have been produced with XSPEC, faking a Mekal model spectrum and using the ready-made response matrices for MOS1 and pn for the thin filter and full window mode. Photon statistics was allowed and the faked spectra were rebinned in a way such that the 5 sigma significance criterion is fulfilled. For the 2.0 keV model, the MOS1 and pn cameras are compared directly (Figs. 45 and 46), while for all other energies only the MOS1 model spectra are displayed.

Note: These simulated spectra have been produced with a particular set of response matrices for MOS1 and pn. Some changes are expected if simulations are repeated with different versions (for latest info: check the XMM-Newton Calibration Portal).

**Figure 43:** Series of EPIC MOS1 model spectra of a Mekal thermal plasma with a temperature of 0.1 keV. From the bottom to the top, the total number of counts in the XMM-Newton passband (0.15-15 keV) increases from 500 to 20000.
$\begin{figure}\begin{center} \leavevmode \epsfig{height=0.76\hsize, file=figs/mos_mekal_00_1kev.eps} \end{center} \end{figure}$

**Figure 44:** Series of EPIC MOS1 model spectra of a Mekal thermal plasma with a temperature of 0.5 keV. From the bottom to the top, the total number of counts in the XMM-Newton passband (0.15-15 keV) increases from 500 to 20000.
$\begin{figure}\begin{center} \leavevmode \epsfig{height=0.76\hsize, file=figs/mos_mekal_00_5kev.eps} \end{center} \end{figure}$

**Figure 45:** Series of EPIC MOS1 model spectra of a Mekal thermal plasma with a temperature of 2.0 keV. From the bottom to the top, the total number of counts in the XMM-Newton passband (0.15-15 keV) increases from 500 to 20000.
$\begin{figure}\begin{center} \leavevmode \epsfig{height=0.76\hsize, file=figs/mos_mekal_02_0kev.eps} \end{center} \end{figure}$

**Figure 46:** Series of EPIC pn model spectra of a Mekal thermal plasma with a temperature of 2.0 keV. From the bottom to the top, the total number of counts in the XMM-Newton passband (0.15-15 keV) increases from 500 to 20000.
$\begin{figure}\begin{center} \leavevmode \epsfig{height=0.76\hsize, file=figs/pn_mekal_02_0kev.eps} \end{center} \end{figure}$

**Figure 47:** Series of EPIC MOS1 model spectra of a Mekal thermal plasma with a temperature of 10.0 keV. From the bottom to the top, the total number of counts in the XMM-Newton passband (0.15-15 keV) increases from 500 to 20000.
$\begin{figure}\begin{center} \leavevmode \epsfig{height=0.76\hsize, file=figs/mos_mekal_10_0kev.eps} \end{center} \end{figure}$

XMM-Newton Users Handbook

3.3.12.1 EPIC spectral quality