Lecture 7: Adaptive Optics Errors & Guide Stars Flashcards
(43 cards)
total residual phase variance is equal to
the sum of variance from all sources
wavefront reconstruction
individual slopes fitted together
wavefront reconstruction limited by
finite spacing between the actuators of the mirror
fitting error
small details of wavefront remain uncompensated
number of sub-apertures for a mirror diameter D
N=aperture area/grid spacing area
control or ‘servo’ system
adjusts shape of deformable mirror to match shape of wavefront
hundreds of adjustments made per second
the finite bandwidth of the control system (or servo) leads to
a residual phase error that limits the Strehl ratio
servo with bandwdth f3dB has associated time constant
t3dB = 1/f3dB
ie how fast corrections can be made
wavefront sensor needs bright point source to
provide sufficient signal to noise in a short exposure time
typically light from science target cannot be used as too faint, instead
use light from a reference source within the field of view
a suitable reference source should be
- point like - with small angular radius
- close proximity to science object - within the isoplanatic patch
- bright - need photons!
natural guide stars
bright stars
laser guide star
laser used to generate an artificial star
isoplanatic patch
area of sky over which a natural guide star is effective
angular radius of theta0, centered on target star
a sufficiently bright natural guide star is not always
available within the isoplanatic patch
artificial may be needed
theta0 prop to r0 prop to lambda^6/5 so
theta0 is few arc seconds in optical
few tens of arc seconds in IR
greater availability of natural guide stars when observing in the infrared
angular anisoplanatism
for an angle between guide star and target, the residual wavefront error is
<Eiso^2> = (theta / theta0)^5/3
errors are smaller the closer
the guide star is to the target
also less when observing in the IR
laser guide star - artificial star created
above turbulence
placed within isoplanatic patch
laser light is
monochromatic
dichroic beamsplitter used to
direct laser light onto wavefront sensor
remaining light passes through beamsplitter to science detector
Rayleigh beacon
focused altitude between 10 and 20km
rayleigh back scattering of light from molecules in lower atmosphere
produces artificial star at low altitude
rayleigh beacon - beacon observed off axis appearing as
an elongated ‘pencil’ of light
rayleigh beacon - use short wavelengths since
rayleigh scattering is proportional to 1/lambda^4