For EPIC users must check that any neighbouring bright sources are not in the same CCD row/column as the desired object by selecting an appropriate position angle, if necessary, in order to avoid contamination of the target data.
If high time resolution is required, the RGS HIGH TIME RESOLUTION mode
should be chosen (see UHB section on RGS modes
). Fastest readout (on
part of the spectrum) is achieved if only one CCD is read out.
For each of the science instruments as prime there is one OM fast mode default configuration. The user should consider whether the time resolution of OM fast mode data is important for the observations and choose the time slice duration accordingly. In case of OM grism observations with a fast mode window on the zeroth order image, OM should be declared prime.
If the observation is long compared with the visibility window (as
reported by the online XMM Target Visibility Tool), the user must consider how best to
split it up, e.g., into multiple observations that fit into continuous
visibility periods. Other criteria for the split of an observation
could be optimal filling of gaps between CCDs, or a calculation to
fit in a certain sequence of OM filters
observed with one of the
OM default configurations
(i.e., with exposure multiples of five per filter).
Users must check the visible magnitude of in-field or nearby optical
sources and the science target itself. If the soft X-ray response is
important, one should choose the thinnest filter compatible with the
brightest visible objects, as described in the UHB section on
EPIC filters
.
In case of HIGH TIME RESOLUTION mode observations it must be decided whether one or all nine CCDs shall be read out.
For the OM it must be decided if specific filter coverage is necessary
for the science or if the recommended filter sequence is adequate (see
UHB section on OM default configurations
).
Telemetry and onboard memory limits place upper and lower boundaries on the duration of single OM exposures as listed in § 5.3.3.5.