Proposed
Approach to the OMC/ WFS Integration at the ATC
wht-naomi-98
Document number
AOW/GEN/RAH/10.0/02/98/OMC/WFS Integration Approach
Version date: 2 March 1998
An earlier document (Number
AOW/GEN/RAH/9.0/02/98/OMC/WFS Integration) presented four possible approaches
to the integration of the OMC and the WFS at the ATC. As a result of further
discussions between the project scientist (PS) and the project engineer a new
approach is now proposed.
The minimum level of integration testing presented in the earlier
document was rejected as it provided little information, presented high risk
and it did not characterise the performance of the integrated subsystems. There
appears to be little evidence that the shortest route to system integration at
Durham provided any significant overall benefit to the project. At the other
extreme, the highest level of testing requires a significant level of proven
software as well as part of the RTCS. We strongly advise against tests at this
stage that involve considerable real-time or interpretative software. The risk
here is that we might be making the implicit assumption that the software was
reliable whereas we need an integrated system to verify its reliability.
The proposed approach
outlined below does not match exactly any of the four levels described earlier.
It lies between the second intermediate level and the maximum level except that
we recommend tests with the DM to be carried out at Durham. We believe that
Durham will be better equipped to perform these tests, e.g. the availability of
the Electra system and a suitable interferometer. Furthermore, the project would
save on shipping, installation and operating costs. The PS estimates that 3
staff from Durham would be required at the ATC for at least one week. If this
approach is followed the DM x-y stage would be shipped to Durham together with
accelerometers, if needed, supplied by
the ATC. An optical flat would be substituted for the DM for the integration
tests at the ATC. The one disadvantage of this approach is that the DM/FSM
interaction would not be evaluated until system integration. However, as
additional time and effort required to carry this evaluation at the ATC, we do
not view this as a significant disadvantage.
We propose that the ATC be
provided with the capability to acquire, process and display diagnostic frames
from the WFS. Processing would be limited primarily to a determination of spot
centroids and a non-real-time wavefront reconstruction using Electra software.
The objective is to allow simple but
useful tests to be performed, e.g. mapping of distortions over the field, a
measurement of spot offsets, etc. There is no intent to provide a dynamic,
real-time capability. We also suggest that a WFS camera/controller be provided
to Durham, when convenient for both the ATC and Durham, for preliminary
integration, interface checkout and
software testing. We view this approach as a risk-reduction measure that
could significantly reduce the problems encountered during both the OMC/WFS
integration and the system integration.
The test sequence given below
is preliminary and it may not be optimum. Note that an optical flat will be
substituted for the DM. The mechanical DM interface with the x-y stage will be
checked at Durham.
3.1 Determine that all
mechanical interfaces are satisfactory and that there are no mechanical
interferences.
3.2 Perform a safety audit to
verify that the equipment does not
present any hazards. This operation
should include the NCU laser, all moving components and all electrical equipment
that may present a potential hazard.
3.3 Verify all basic OMC and
WFS functions using engineering level software and the WFS independent control
module. Verify that images are received by the pre-correction camera,
IR/optical science ports and the WFS. Note that quantitative measurements of
wavefront quality are performed later in the integration process.
3.4 Perform open-loop tests
of both the FSM and the NCU tip/tilt injector. The suggested approach would be
to use a calibrated position-sensing detector at the f/16.8 focus and monitor
the drive signals (sinusoidal input) and the detector output. We anticipate
that the NCU laser source would be required to provide adequate signal/noise
and resolution from the detector. Comparison of the input/output signals could
provide information on vibration effects but it is suggested that
accelerometers are also used to assess vibration effects.
3.5 Measure the non-dynamic
transfer function of the WFS using both the WFS calibration source and the NCU.
Note that “non-dynamic” indicates that one is unable to make a proper phase-lag
measurement at this time, i.e. the real-time processing latency would not be
included.
3.6 Determine the Hartmann
spot offsets with both the WFS calibration source and the on-axis NCU point
source. The former provides a measure of the WFS internal aberrations and the
latter includes both the WFS and on-axis OMC aberrations. Wavefront reconstruction would be performed, possibly
off-line, using Electra software.
3.7 Measure simple static
wavefronts, i.e. tilt, defocus and
low-order aberrations from the aberration generator, using the WFS and
NCU. The WFS performance variation with light level would be investigated.
3.8 Perform distortion
mapping of the WFS field using the NCU’s array of point sources. The Hartmann
spot offsets would be determined at selected field points and wavefront
reconstruction performed to assess the off-axis aberrations.
3.9 Assess the proposed
technique to align the DM to the WFS. This test would be carried out by placing
a mask over the optical flat to simulate a single segment of the DM. The entire
flat would be moved using the x-y stage until the “segment” is centred in a WFS
subaperture. The sensitivity and repeatability of this alignment operation
would be determined. Note that this test would involve open-loop operation with
manual input; an automated procedure is not proposed at this stage.
3.10 Evaluate the OMC/NCU/WFS
sensitivity and repeatability when subjected to temperature cycling. This test
will be restricted to the limits set by the laboratory environment.
3.11 Limited measurements of
non-common-path aberrations are suggested, subject to an evaluation of technical feasibility and the evaluation of
equipment and resources.
The wavefront aberrations at
the IR and optical science ports could be measured at selected field points
using a self-referencing interferometer, e.g. a Smartt interferometer (aka a
point-diffraction interferometer). The interferometer would need to be mounted
on an x-y stage to cover the field of view. Concerns include the required
source brightness and the choice of sensor to be used with the interferometer.
We note that the NCU’s array of point sources, as currently proposed by ROE,
will only be diffraction limited as seen by the WFS subapertures and thus this
array is not suitable for use with a Smartt interferometer at visible
wavelengths, i.e. the pinholes are too large. The wavefront errors seen by the
WFS would be determined as outlined in section 3.6 above.
3.12 Verify that any special
handling equipment performs satisfactorily and that components fit properly in their shipping containers to insure
safe transport.