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Adaptive Optics Facility
Calibrations
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Calibration Issues for the Adaptive Optics Facility
| Purpose of work: |
AO Facility DSM calibrations
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Studies conducted by:
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Sylvain
Oberti (soberti@eso.org)
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| Project Manager AOF: |
Robin Arsenault (rarsenau@eso.org) |
| Location: |
N/A |
| Status: |
Preliminary Studies &
Simulations
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Calibration
Requirements
A fundamental
limitation of AO
systems based on an adaptive secondary mirror like the VLT M2 is that
there is
no intermediate focus before the deformable mirror. Therefore, it is
not
possible to install an artificial calibration source, seen by the DM
and the Interaction
Matrix (IM) measurement in a conventional way is not possible. An
extensive
program has been initiated at ESO to study this limitation and explore
alternatives.

Figure 1: Left a Adaptive
secondary scheme; there is no intermediate focus where an artificial
star can be located upstream from the DSM. This is the case for an
conventional AO system (right) where a re-imaging optics system is
inserted before the final corrected focus.
Several solutions are
being
envisioned for the IM measurement.
First, Synthetic (simulated) IM using measured influence
functions of
the DSM in the laboratory and calibration of the WFS optical path and
second
several different methods of performing on-sky IM measurements.
Even if the synthetic
IM is the
most seductive solution (noiseless, simplicity, no calibration time
required),
it still has to be demonstrated that the accuracy of the models (DM and
WFS)
can be high enough to ensure the expected performances.
Regarding the
experimental
estimation of the IM, novel techniques are investigated in order to
deal with
the new issues that we have to face:
- There is turbulent noise either because the
calibration is performed on sky or because of the telescope internal
turbulence.
- The calibration time might dramatically increased
because of the larger number of degrees of freedom.
- Several methods are being investigated through
simulations and laboratory tests as well as on sky tests when possible.
The
different schemes aim at minimizing the noise and bias on the
measurement in
order to optimize the quality of the reconstructor.
Using various modal
bases (zonal,
Hadamard, system modes/mirror modes, Zernike or Karhuenen-Loeve),
several
techniques are foreseen and being compared:
- Open loop fast DM actuation, which allows
freezing the disturbances between modal push and pull and thus minimize
turbulent noise as well as any low frequency effect.
- Open loop DM modulation and demodulation by FFT
detection. The stimulus power is concentrated on a single frequency
beyond the
modal atmospheric bandwidth. Low frequency effects are cancelled out
and it
allows for multiplexing. This way, several modes can be measured at the
simultaneously,
reducing the total calibration time.
- Closed loop calibration. Dynamic bias is applied
as offset on the WFS signal. The DM command is measured as a response
to this
bias and therefore the reconstruction matrix (or control matrix) is
measured
directly.
Furthermore, there is
a key issue
related to calibration. A pupil offset may have a strong impact on the
system
performance and must be addressed properly. Indeed, for high order AO
systems
such as VLT with DSM, the tolerance is very tight. Dynamical pupil
alignment is
envisioned to minimize this effect.
Modal Basis
The choice of the modal basis to activate the DM actuator is extremely
important. Hadamard modes have the property to maximize the WFS signal
for a low voltage actuation of each electrode. A mathematical matrix
operation allows to recover the individual DM Influence function. The
figure 2 provides a comparison for the MACAO-VLTI 60 elements curvature
systems of the IM betwen zonal (one actuator at a time) and Hadamard
modes.

Figure 2: Zonal IM versus
Hadamard IM. The
Hadamard matrix have the property to exhibit the largest determinant
for a matrix made of 1 and -1. This reflects in the highest WFS signal
for a given voltage actuation.
Fast DM Actuation
Another ingredient to a high S/N ratio IM is a fast actuation of the DM
electrode. This has the advantage of freezing the turbulence and
therefore making the process independant of time dependant variations
(like turbulence). Care must be taken to leave a short delay after
actuation (by a square wave for instance) to let the DM stabilize (in
case of overshoot and/or vibration after actuation). The measurement is
repeated several time and measurement averaged.
The use of the above technique have proven very promising on MACAO-VLTI
where an interaction matrix has been obtained on the sky (August 2004)
in moderate seeing conditions and used to close the loop and correct
turbulence. The result is shown on figure 3.

Figure 3: IM obtained
conventionally on artificial star (left) and IM obtained on sky on a
turbulent source (right). The image on the right has been obtained
after AO correction using the IM obtained on sky.
Modulation Technique
This is a classical technique in optics and telecommunications. It
consists in modulating the input signal with a sinusoidal wave. The
demodulation is obtained by multiplying by the same function. The
useful signal is folded to DC, a low pass filter (averager) retrieves
signal amplitude and averaging cancels out the white noise term.
Synthetic IM
The advantage of this technique is that it is independant of noise and
bias such as turbulent noise, photon noise, read noise, telescope
drifts and deformable mirror limitation (hysterisis, creep,
non-linearity...).
On the other hand it doesn't account for realistic effects like optical
mis-alignment and its effect on static aberration (and/or pupil
misregistration). A very accurate DM model is required and WFS as
well; the calibrations or definition of the model is a critical
and not obvious process.
MAD for test bed

Conclusions
- Various techniques have been investigated to tackle the
calibration issues in the AO facility case
- This study is of major importance for ELT AO as well
- The most promising solutions are synthetic and modulation
techniques
- They have been validated in the low order case
- Simulations, the HOT experiment (+1000 actuators) and later
ASSIST will allow addressing the high order case
More Details...
The following work led by S. Oberti (AOD) has been presented to the
SPIE meeting Orlando (May 2006). It represents the most up-to-date
approaches and strategy for accurate calibration of high order AO
system like the AO Facility and its DSM.
"Large DM AO
systems: synthetic IM or calibration on sky?"