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Lecture 16 The applications of tomography: MCAO, MOAO, GLAO

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Title: Lecture 16 The applications of tomography: MCAO, MOAO, GLAO


1
Lecture 16The applications of tomographyMCAO,
MOAO, GLAO
  • Claire Max
  • AY 289C
  • UC Santa Cruz
  • March 6, 2008

2
Next week (the last week of class!)
  • Tuesday March 11th lecture
  • AO for imaging the living human retina.
  • Jason Porter, Univ. of Houston
  • Thursday March 13th lecture
  • Extreme AO for imaging planets around nearby
    stars
  • Bruce Macintosh, Lawrence Livermore National Lab
  • Final exam take-home, open-book
  • Distributed at lecture Thursday March 13th
  • Due in my office (or my computer) on or before
    Thurs March 20th at noon. This is a hard
    deadline.

3
The final homework assignment
  • Will be on web by end of this week
  • Due Thurs March 13
  • Will be intended to help you review the whole
    course and get ready for the exam
  • What approaches have you found useful in
    reviewing classes like this? What makes the
    material stick ?

4
Outline of lecture
  • Review of AO tomography concepts
  • AO applications of tomography
  • Multi-conjugate adaptive optics (MCAO)
  • Multi-object adaptive optics (MOAO)
  • Ground-layer AO (GLAO)

5
What is Tomography ?1. Cone effect
Credit Rigaut, MCAO for Dummies
6
What is Tomography ?2. Wider field of view, no
cone effect
Tomography lets you reconstruct turbulence in the
entire cylinder of air above the telescope mirror
90 km
Credit Rigaut, MCAO for Dummies
7
Ragazzonis Tomography Cartoon
Credit Ragazzoni, Nature 403, 2000
8
Concept of a metapupil
  • Can be made larger than real telescope pupil
  • Increased field of view due to overlap of fields
    toward multiple guide stars

9
How tomography works from Don Gavel
kZ
kX
Fourier slice theorem in tomography (Kak,
Computer Aided Tomography, 1988)
  • Each wavefront sensor measures the integral of
    index variation along the ray lines
  • The line integral along z determines the kz0
    Fourier spatial frequency component
  • Projections at several angles sample the kx,ky,kz
    volume

9
10
How tomography works from Don Gavel
kZ
kX
  • The larger the telescopes primary mirror, the
    wider the range of angles accessible for
    measurement
  • In Fourier space, this means that the bow-tie
    becomes wider
  • More information about the full volume of
    turbulence above the telescope

10
11
How tomography works some math
  • where
  • y vector of all WFS measurements
  • x value of d?OPD) at each voxel in turbulent
    volume above telescope

x
y
A is a forward propagator (entries 0 or 1)
  • Assume we measure y with our wavefront sensors
  • Want to solve for x value of d?OPD)
  • The equations are underdetermined there are
    more unknown voxel values than measured phases Þ
    blind modes. Need a few natural guide stars to
    determine these.

12
Solve for the full turbulence above the telescope
using the back-propagator
x
y vector of all WFS measurements x value of
d?OPD) at each voxel in turbulent volume above
telescope
y
AT is a back propagator along rays back toward
the guidestars
x
Use iterative algorithms to converge on the
solution.
y
13
LGS Related Problems Null modes
  • Tilt Anisoplanatism Low order modes (e.g.
    focus) gt Tip-Tilt at altitude
  • ? Dynamic Plate Scale changes
  • Five Null Modes are not seen by LGS (Tilt
    indetermination problem)
  • ? Need 3 well spread NGSs to control these modes

Credit Rigaut, MCAO for Dummies
14
Outline of lecture
  • Review of AO tomography concepts
  • AO applications of tomography
  • Multi-conjugate adaptive optics (MCAO)
  • Multi-object adaptive optics (MOAO)
  • Ground-layer AO (GLAO)

15
What is multiconjugate AO?
Deformable mirror
Credit Rigaut, MCAO for Dummies
16
What is multiconjugate AO?
Credit Rigaut, MCAO for Dummies
17
The multi-conjugate AO concept
Telescope
Turb. Layers
WFS
2
1
DM2
DM1
Atmosphere
UP
Credit Rigaut, MCAO for Dummies
18
Star Oriented MCAO
  • Each WFS looks at one star
  • Global Reconstruction
  • n GS, n WFS, m DMs
  • 1 Real Time Controller
  • The correction applied at each DM is computed
    using all the input data.

Credit N. Devaney
19
Layer Oriented MCAO
  • Layer Oriented WFS architecture
  • Local Reconstruction
  • x GS, n WFS, n DMs
  • n RTCs
  • Wavefront is reconstructed at each altitude
    independently.
  • Each WFS is optically coupled to all the others.
  • GS light co-added for better SNR.

Credit N. Devaney
20
MCAO Predicted Performance
1
1
0
  • Surface plots of Strehl ratio over a 1.5 arc min
    FoV.
  • 13x13 actuator system, K band, Cerro Pachon
    turbulence profile.

Credit Rigaut, Le Louarn
21
MCAO Performance PredictionsNGS, Mauna Kea
Atmospheric Profile
2 DMs / 5 NGS
1 DM / 1 NGS
165
320 stars / K band / 0.7 seeing
Stars magnified for clarity
Credit Rigaut, MCAO for Dummies
22
MCAO Simulations, 3 laser guide stars
Strehl at 2.2 ?m 3 NGS, FoV 1 arc min
Strehl at 2.2 ?m 3 NGS, FoV 1.5 arc min
Average Strehl drops, variation over FoV
increases as FoV is increased
Credit N. Devaney
23
Results from ESOs Multiconjugate AO Demonstrator
(MAD)
Single Conjugate
Multi Conjugate
24
Gemini South MCAO
Credit Eric James Brent Ellerbroek, Gemini
Observatory
25
Outline of lecture
  • Review of AO tomography concepts
  • AO applications of tomography
  • Multi-conjugate adaptive optics (MCAO)
  • Multi-object adaptive optics (MOAO)
  • Ground-layer AO (GLAO)

26
Distinctions between multi-conjugate and
multi-object AO
  • Only one DM per object, conjugate to ground
  • Guide star light doesnt bounce off small MEMS
    DMs in multi-object spectrograph
  • DMs conjugate to different altitudes in the
    atmosphere
  • Guide star light is corrected by DMs before its
    wavefront is measured

27
Science with MOAO multiple deployable spatially
resolved spectrographs
  • A MEMS DM underneath each high-redshift galaxy,
    feeding a narrow-field spatially resolved
    spectrograph (IFU)
  • No need to do AO correction on the blank spaces
    between the galaxies

28
Why does MOAO work if there is only one
deformable mirror in the science path?
  • Tomography lets you measure the turbulence
    throughout the volume above the telescope

90 km
29
Why does MOAO work if there is only one
deformable mirror in the science path?
  • Tomography lets you measure the turbulence
    throughout the volume above the telescope
  • In the direction to each galaxy, you can then
    project out the turbulence you need to cancel out
    for that galaxy

90 km
30
Outline of lecture
  • Review of AO tomography concepts
  • AO applications of tomography
  • Multi-conjugate adaptive optics (MCAO)
  • Multi-object adaptive optics (MOAO)
  • Ground-layer AO (GLAO)

31
Ground layer AO do tomography, but only use 1 DM
(conjugate to ground)
GLAO
GLAO uses 1 ground-conjugated DM, corrects
near-ground turbulence
Credit J-M Conan
32
Correcting just the ground layer gives a very
large isoplanatic angle
  • Strehl 0.38 at ? ?0
  • ?0 is isoplanatic angle
  • ?0 is weighted by high-altitude turbulence (z5/3)
  • If turbulence is only at low altitude, overlap is
    very high.
  • If you only correct the low altitude turbulence,
    the isoplanatic angle will be large (but the
    correction will be only modest)

Common Path
Telescope
33
Ground Layer AO (GLAO) typically decreases
natural seeing by a factor of 1.5 to 2
  • Example GLAO calculation for Giant Magellan
    Telescope (M. Johns)
  • Adaptive secondary conjugation at 160 m above
    primary mirror.
  • Performance goals
  • ? gt 0.8 mm
  • Field of view gt10
  • Factor of 1.5-2 reduction in image size.

Modeled using Cerro Pachon turbulence profile.
(M-L Hart 2003)
34
Many observatories have ambitious GLAO projects
planned
  • Near term on medium sized telescopes SOAR
    (4.25m), William Herschel Telescope (4.2m), MMT
    (6.5m)
  • Medium term on VLT (8m), LBT (2x8m)
  • Longer term on Giant Magellan Telescope etc.
  • Is it worth the large investment just to
    decrease seeing disk by factor of 1.5 to 2 ?
  • Depends on whether existing or planned large
    spectrographs can take advantage of smaller image
  • Potential improved SNR for background-limited
    point sources

35
time
Credit A. Tokovinin
36
Credit A. Tokovinin
37
Summary
  • Tomography a way to measure the full volume of
    turbulence above the telescope
  • Once you have measured the turbulence and know
    its height distribution, there are several ways
    to do the wavefront correction to get wider field
    of view
  • Multi-conjugate AO multiple DMs, each optically
    conjugate to a different layer in the atmosphere.
  • Multi-object AO correct many individual objects,
    each over a small field.
  • Ground-layer AO correct just the turbulence
    close to the ground. Gives very large field of
    view but only modest correction. Should work in
    both the visible and the IR.
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