Adaptive optics and wavefront correctors

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1 brice.leroux@oamp. fr Adaptive optics and wavefront correctors

description

Adaptive optics and wavefront correctors. stratosphere. tropopause. 10-12 km. wind flow over dome. Boundary layer. ~ 1 km. Heat sources w/in dome. Atmosphere from 0 to 20 km…. Measured from a balloon rising through various atmospheric layers. And what about spatial telescopes ?. - PowerPoint PPT Presentation

Transcript of Adaptive optics and wavefront correctors

Page 1: Adaptive optics and  wavefront correctors

[email protected]

Adaptive optics and wavefront correctors

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stratosphere

tropopause

Heat sources w/in dome

Boundary layer~ 1 km

10-12 km

wind flow over dome

Atmosphere from 0 to 20 km…

Measured from a balloon rising through various

atmospheric layers

[email protected]

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And what about spatial telescopes ?

• It is definitively a solution for some applications

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But extremely difficult and expensive to make large telescopes…

Telescope under study for first light around 2015-2020:USA : TMT diameter of 30 meterEurope : E-ELT diameter 42 meter

42 meter in space ???????? No !!!!

• Ground based telescopes necessary to get more photons & a better angular resolution with higher diameter … large telescope WITH adaptive optics • Space telescope will remain necessary anyway because of atmosphere absorption at certain wavelengths

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How does adaptive optics help?

Measure details of blurring from “guide star” near the object you want to observe

Calculate (on a computer) the shape to apply to deformable mirror to correct blurring

Light from both guide star and astronomical object is reflected from deformable mirror; distortions are removed

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Phase lag, noise

propagation

DM fitting error

Measurement error

Non-common path errors

Feedback loop: next cycle

corrects the (small) errors

of the last cycle

Adaptive optics system

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Classical Adaptive optics

Wave front sensor

control

astro.imaging

Deformablemiror

[email protected]

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Close loop / open loop AO

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RTCRTCWFSWFS

DMDM CAMCAM

WaveFront Sensor Real Time Computer

Deformable mirror Imaging camera

WFSWFS

CAMCAM

RTCRTC

DMDM

wav

efro

ntw

avef

ront

Open loop

Close loop

Main advantage of close loop :the WFS is working around 0, measuring small perturbations=> It is working in its linearity domain

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Adaptive optics increases peak intensity & width of a point source

Lick Observatory

No AO With AO

No AO With AO

Intensity

How is the Point Spread Functionafter adaptive Optics ?

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AO produces point spread functions with a “core” and “halo”

• When AO system performs well, more energy in core

• When AO system is stressed (poor seeing), halo contains larger fraction of energy (diameter ~ r0)

• Ratio between core and halo varies during night

Inte

nsity

x

Definition of “Strehl”:Ratio of peak intensity to that of “perfect” optical

system

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Correction quality ?

• Strehl ratio :

I[0,0] is the intensity of the Point Spread Functionat the center of the image

(Strehl, K., 1902, Zeit. Instrumenkde, 22, 213)

Post AO

Ideal case

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Other parameter might be more interesting, depending upon the objective:

• Full width half maximum (FWHM) resolution

• Ensquared/encircled energy spectroscopy• Indirect criterium:

- detection/signal to noise ratio- quality of image reconstruction

Correction quality ?

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Adaptive optics system elements

• Deformable mirror to correct the wavefront• Wavefront sensor to measure the distortion that has to

be corrected• Real time computer / control algorithm to calculate the

instructions to the DM from the WFS measurements

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Each of them brings specific limitations / error terms

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2ph & ron

+ 2aliasing

+ 2scintill.

= 2

miror

+ 2wfs

+ 2temp.

+ 2atm. res.

+ 2anisoplanatism

{

Residual phase variance2

OA residu

Classical Adaptive optics

Now, we are going to study each of these elements…

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DM caracteristics• Number of actuators and spatial arrangement

• Dynamic range: stroke (total up and down range)– Typical “stroke” for astronomy several microns. For vision science up to 10

microns

• Spectral range

• Temporal frequency response: faster than coherence time 0

• Influence function of actuators:– Shape of mirror surface when you push just one actuator

• Surface quality: Small-scale bumps can’t be corrected by AO

• Hysteresis of actuators:– Want actuators to go back to same position when you apply the same voltage

• Power dissipation:– Don’t want too much resistive loss in actuators, because heat is bad (“seeing”,

distorts mirror)

– Lower voltage is better (easier to use, less power dissipation)

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Influence function of deformable mirror

15Influence function and interactuator distance gives correlation coefficient

correlation coeffBetween two actuators

One actuator Two actuators

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Types of deformable mirrors: large• Segmented

– Made of separate segments with small gaps– Each segment has 1 - 3 actuators and can correct:

• Piston only (in and out), or • Piston plus tip-tilt (three degrees of freedom)

• “Continuous face-sheet” – Thin glass sheet with actuators glued to the back– Zonal (square actuator pattern), or– Modal (sections of annulae, as in curvature sensing)

• Bimorph– 2 piezoelectric wafers bonded together with array of

electrodes between them. Front surface acts as mirror.

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Types of deformable mirrors: small

• Liquid crystal spatial light modulators– Technology similar to LCDs for computer screens

– Applied voltage orients long thin molecules, changes index of refraction

– Allows large number of pixels DM (typically LCD : 512x512 pixels)

– Only problem… response time slow…

• MOEMS (micro-Opto-electro-mechanical systems)– Fabricated using microfabrication methods of the integrated circuit

industry

– Many mirror configurations possible

– Potential to be very inexpensive

– Very large number of actuators possible

– No problem of response time

Electrostaticallyactuateddiaphragm

Attachmentpost

Membranemirror

Continuous mirror

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Continuous face-sheet deformable mirrors

Anti-reflection coating

Glass face-sheet

PZT or PMN actuators: get longer and shorter as

voltage is changed

Cables leading to mirror’s power supply (where voltage is applied)

Light

• DMs generates a wavefront fitting DMs generates a wavefront fitting error due to its limited degree of error due to its limited degree of freedom freedom

fittingfitting2 2 = a= aFF ( d / r ( d / r00 ) )5/3 5/3 radrad22

•Characteristics:Characteristics: actuator separation, actuator separation, temporal response, influence temporal response, influence function, surface quality, hysteresisfunction, surface quality, hysteresis

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• Range from 13 to > 900 actuators (degrees of freedom)

Xinetics

About 12”

Continuous face-sheet DM’s: Xinetics product line

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Influence functions for Xinetics DM

• Push on four actuators, measure deflection with an optical interferometer

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Bimorph mirrors

Bimorph mirror made from 2 piezoelectric wafers with an electrode pattern between the two wafers to control deformation

Front and back surfaces are electrically grounded.

When V is applied, one wafer contracts as the other expands, inducing curvature

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Micro deformable mirror in poly-Silicium (continuous membrane)

Influence function of the deformable mirror

600µm

MOEMS

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Fitting error

fitting2 = aF ( d / r0 )5/3 rad2

• Physical interpretation: If we assume the DM does a perfect correction of all modes with spatial frequencies < 1 / r0 and does NO correction of any other modes, then aF = 0.26

• Equivalent to assuming that a DM is a “high-pass filter”:

– Removes all disturbances with low spatial frequencies, does nothing to correct modes with spatial frequencies higher than 1/r0

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Fitting error and number of actuators

fitting2 = aF ( d / r0 )5/3 rad2

DM Design aF Actuators / segment

Piston only, 1.26 1square segments

Piston+tilt, 0.18 3Square segments

Continuous DM 0.28 1

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Consequences: different types of DMs need different actuator counts, for same

conditions• To equalize fitting error for different types of DM, number of

actuators must be in ratio

• So a piston-only segmented DM needs ( 1.26 / 0.28 )6/5 = 6.2 times more actuators than a

continuous face-sheet DM

• Segmented mirror with piston and tilt requires 1.8 times more actuators than continuous face-sheet mirror to achieve same fitting error:

N1 = 3N2 ( 0.18 / 0.28 )6/5 = 1.8 N2

N1

N2

d2

d1

2

aF1

aF2

6/ 5

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Adaptive secondary mirrors• Make the secondary mirror into the “deformable mirror”• Curved surface ( ~ hyperboloid) tricky• Advantages:

– No additional mirror surfaces • Lower emissivity. Ideal for thermal infrared.• Higher reflectivity. More photons hit science camera.

– Common to all imaging paths except prime focus

• Disadvantages:– Harder to build: heavier, larger actuators, convex.– Difficult to control mirror’s edges (no outer “ring” of actuators outside

the pupil)

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MMT-Upgrade: adaptive secondary

• Magnets glued to back of thin mirror, under each actuator.

• On end of each actuator is coil through which current is driven to provide bending force.

• Within each copper finger is small bias magnet, which couples to the corresponding magnet on the mirror.

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Adaptive secondary for the MMT

U. Arizona +

Arcetri Observatory

> 300 actuators