Lecture 6: Wavefront Sensing & Correction Flashcards
(40 cards)
active optics compensates for other long-term dirfts in the telescope such as
mechanical relaxation of flexures
thermal expansion of truss
active optics counteracts effect of
gravity and other deformations of the telescope mirros
active optics acute on
large primary mirror (plus tip-tilit of secondary mirror)
active optics operate on timescales of
tens of seconds
rate about 0.05Hz
common adaptive optics
segemented mirror
deformable mirror
bimorph mirror
piezoelectic / electrostrictive actuators
displacement/curvature proportional to applied voltage
bimorph mirror
two thin plates of piezoelectric material bonded over a configuration of electrodes
applied voltage causes mirror to bend in response
wavefront sensing
light from reference star picked off by dichroic beamsplitter
focused on wavefront sensor
info used to adjsut shape of adaptive optic
independent of wavelength
most common wavefront sensing concepts
Shack-Hartmann
Curvature
Shack-Hartmann WFS senses
SLOPE
applies corrections to segmented mirror than produces variable tilt in response to a control signal
Shack-Hartmann WFS best for
large number of sub-apertures
N>50
curvature WFS senses
CURVATURE
applies corrections to bimorph mirror that produces variable curvature in response to a control signal
simple scheme
curvature wfs is competitive with S-H for
a relatively small number of sub-apertures
N< or =50
S-H WFS - wavefront divided into
portions
one to each sub-aperture
S-H WFS - light from each sub-aperture focussed onto
CCD camera/detector array
S-H WFS - PLANE WAVEFRONT
regular series of spots in the focal plane
S-H WFS - corrugated wavefront
irregularly spaced spots
S-H WFS - slope of each portion of the wavefront determined from
the displacement of the spot from the central position
measurements used to reconstruct wavefront
S-H WFS - distorted wavefront has
local gradient, a, at a particular lenslet
tilt of the wavefront is measured in two directions:
ax and ay
with sub-aperture size, d, angular size of image (FWHM) will be
for d<ro - aSA=lambda/d
for d>ro - aSA = lambd/r0
the overall centroid of the image is estimated from
the average of the displacement within each sub-aperture
this info is then used for tip-tilit correction
photon counting noise leads to
an uncertainty in the measurement of the centre of the spot
Fractional error in determining the angle corresponding to
the centre of the image
sigma a / aSA = 1/root n