The adaptive optics (AO) subsystem is the heart of GPI. It is responsible for making fast visible-light
measurements of the wave front external to GPI (primarily atmospheric phase errors) and correcting that
wave front using its deformable mirrors. It is tightly integrated with other subsystems.
The AO subsystem optical path begins at the entrance window. A steering mirror is available to align
GPI’s pupils with the Gemini entrance pupil. The beam is then collimated and relayed to the first
deformable mirror. This high-stroke low-actuator count piezo DM (referred to as the “woofer”) reduces
the residual wave front error to a level controllable by the finer “tweeter” mirror. This DM will also
serve as the tip/tilt mirror, mounted on a commercial FSM mount.
A pair of optics relays the beam to the
“tweeter” DM. This is a 4096-actuator MEMS device (with a 45-actuator-diameter region illuminated).
Two more conic optics produce a converging F/64 beam with a finite pupil for input into the
coronagraph path. A 0.95-micron dichroic splits the visible light into the fast spatially-filtered wave
front sensor (SFWFS). The visible light passes through a variable-size spatial filter, used to remove
uncontrollable spatial frequency components that would be aliased into incorrect wave front
measurements. Relay optics then reform the pupil on a lenslet array, and the resulting dot pattern is in
turn relayed to a high-speed CCD. The final CCD downselect has not been made (in part because of the
developmental status of several attractive CCD options, but it will operate at 1-2 kHz
with each subaperture corresponding to a 2x2 quad-cell. A bandpass or short-cutoff filter limits the
wavelength range seen by the SFWFS (nominally to 0.7-0.9 microns), since spatial filter performance
improves with increasing Strehl at the sensing wavelength, and since the spatial filter size can only be
precisely matched to spatial frequency cutoff at a single wavelength.
The baseline AO control algorithm is the Optimized-gain Fourier Controller (OFC) algorithm developed
by Poyneer and Veran. This is an adaptive modal gain algorithm using the Fourier modes as its basis set,
allowing both efficient reconstruction and a direct match to sensor geometry and the PSF. We have also
explored a predictive controller algorithm. Although this is not yet the baseline, it has
the potential to improve performance by a factor of 2 on dim stars, and/or allow performance at 1 kHz
comparable to OFC performance at 2 kHz. We are specifying the AO control computer (AOC) with
sufficient capability to support this predictive algorithm should we decide to implement it.
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