Focussing UCLES
The depth of focus for UCLES is substantial and it will be rare
that focus changes are required, but it should nevertheless be checked.
Configure spectrograph to wavelength of interest.
CCD: use a narrow unbinned window ( e.g. TEK1K_SETUP or
THOMSON_SETUP)
IPCS: use ND filters over the arc lamps ( i.e. LF1 8 and
LF2 3) and gradually remove them until the maximum countrate is below
1 Hz. Because of the large IPCS window used with UCLES the countrate
limitations are severe and it is advised that the countrate should not
exceed 0.5 Hz in any of the measured lines.
Focussing UHRF
First focus on the red laser line at 6328.160 Å and inspect
the instrumental profile. It should have a Gaussian FWHM of approximately
48
m, plus a low asymmetric tail to higher wavelengths.
Tests with a green laser yielded the same value. Note that UHRF resolves the
ThAr lines, so these cannot be used to assess the instrumental profile, but
they are used to refocus UHRF for each wavelength setting, which is essential.
Configure spectrograph to wavelength of interest.
CCD: use a narrow binned window ( e.g. UHRF_X4)
IPCS: use ND filters over the arc lamps ( i.e. LF1 8 and
LF2 3) and gradually remove them until the maximum countrate is below
1 Hz.
to help
estimate a new collimator value. In the latter case, for every +1 pixel shift
resulting from
the cross correlation SCROSS hp_down hp_up, move UFC/UFF by
-50 ADU at R = 1.0M, -80 ADU at R = 0.6M, and -170 ADU at R = 0.3M.
that UFC and UFF
read the same encoder, but differ in their positioning accuracy, so UFF
must be used for setting within 50 ADUs. Moreover, UFF will position
poorly for motions less than about 20 ADUs, so should be driven away by 50 ADUs
and back again if necessary.
m,
= 2 Tek pixels or 2.6 Thomson pixels.
Note that the HP UP configuration produces brighter spectra than the HP DOWN configuration.
The geometric structure of the image slicer modulates the signal
in the spatial direction. This is clearly visible in the UHRF laser, ThAr,
and quartz lamp exposures (see Figs
and
). Observers may find it useful to take flat field
exposures not only through the image slicer but also through the slit, using
the maximum slit length ( SL MAX). These will provide more uniform
illumination in the spatial direction which makes it easier to identify
pixel--to--pixel variations. (Reminder: SLIT SLIT and SLIT SLICER
swap between the image slicer and slit assembly.)
Figure: UHRF, 10 sec ThAr lamp @ 6328 Å, SLICER, UHRF_X4, XMEM orientation.
Figure: UHRF, 10 sec quartz lamp, SLICER, UHRF_X4, XMEM orientation.
Wavelength placement:
Even after doing a CONFIG, further adjustment of the spectrum
positioning may be desired, especially with UHRF for which the spectrum
coverage is so small, or for UCLES if partial orders are being recorded
at one or both sides of the detector,
in which case it might be desirable to shift the spectrum in the
cross-dispersion direction to obtain a better coverage of one of these.
With UHRF, observers may wish to force the VAX to use encoder units, rather than
transformed units ( e.g. mm), by specifying RAW. To return to
transformed units, specify REAL.
The most likely parameters to change are:
Once satisfactory grating and focus settings are obtained, they can be locked into the control files with
Other useful commands: