Adaptive Optics: Concepts & Key Numbers Jean-Marc Conan

ONERA - Optics Dept (France) [email protected]

Adaptive Optics: Concepts & Key Numbers ‰

FAWSA – JM Conan – Nov. 2016

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3

Adaptive Optics Principle ‰

Correcting for turbulence with adaptive optics

‰

Key components & System specification

‰

Closing the loop & Corrected Images

New Developments in Adaptive Optics ‰

eXtreme Adaptive Optics: the search for exoplanets

‰

Wide Field Adaptive Optics : origin of the universe

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From VLT (10 m class) to ELT (30 m class) telescopes

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Beyond astronomical applications ?

Astronomical Imaging Through Turbulence •

Astronomy often implies high angular resolution imaging of distant objects: solar system bodies, stars, galaxies…

FAWSA – JM Conan – Nov. 2016

Loss in resolution and sensitivity

4

D/r0 key parameter gives resolution ratio seeing over diffraction

FAWSA – JM Conan – Nov. 2016

λ/D

D = 10m

λ/D = 10 mas λ/D = 45 mas 1 mas = 10-3 arcsec

In IR, large telescopes (10m for instance) give same resolution as amateur 60cm instrument 5

400 Years of Ground Based Astronomical Instrumentation •

From few centimeters in 1609…

…to 39 meters… in 2024 (?)

D=39 m Isaac Newton D=0.15 m 1671

Galileo Galilei

FAWSA – JM Conan – Nov. 2016

1953 Concept Optique Adaptative par Babcock

2024 ?

1990 Optique Adaptative COME-ON @ 3.6m ESO

Angular Resolution 4 ” [arcsec]

1”

1”

1”

1” 0.100”

λ/D diffraction limited case

0.040” VLTs

0.010” ELTs

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Adaptive Optics Principle

Incoming Plane Wave

Object

Atmospheric turbulence Turbulent wavefront Deformable Mirror

Uncorrected Image

Reconstruction & Control

WaveFront Sensor

FAWSA – JM Conan – Nov. 2016

Corrected wavefront

Corrected Image

Imaging Camera

¾ Adaptive Optics allows to reach near diffraction limited angular resolution ¾ Main components: Turbulence ; Def. Mirror ; Wave-Front Sensor ; Rec. & Control 7

Adaptive Optics: Concepts & Key Numbers ‰

‰

Correcting for turbulence with adaptive optics

‰

Key components & System specification

‰

Closing the loop & Corrected Images

New Developments in Adaptive Optics ‰

eXtreme Adaptive Optics: the search for exoplanets

‰

Wide Field Adaptive Optics : origin of the universe

‰

From VLT (10 m class) to ELT (30 m class) telescopes

‰

Beyond astronomical applications ?

FAWSA – JM Conan – Nov. 2016

‰

Adaptive Optics Principle

8

AO Performance: Main Contributors to Residual Phase Residual phase variance

σ2 φ residual = Incoming Plane Wave

σ2fitting 䊽 spatial sampling

Atmospheric turbulence

(Deformable Mirror pitch) Turbulent wavefront Deformable Mirror

+ σ2wfs-noise 䊽 number of photons (guide star magnitude)

Reconstruction & Control

+ σ2tempo 䊽 temporal sampling WaveFront Sensor

FAWSA – JM Conan – Nov. 2016

Corrected wavefront

'ŽŽĚŝŵĂŐŝŶŐƋƵĂůŝƚLJƌĞƋƵŝƌĞƐ͗ Imaging Camera

㼼ϯ

σ φ residual << λim

Is it a perfect plane wave?

9 9

FAWSA – JM Conan – Nov. 2016

PSD alias Energy versus spatial frequency

Residual Phase after AO Correction Turbulent Phase PSD Kolmogorov Spectrum α f -11/3

Rejection by AO

Corrected Phase

σ2wfs-noise & σ2tempo

Low Frequencies partially corrected by AO

σ2fitting High Frequencies non corrected by AO

Spatial Frequencies (1/m)

fc = 1/(2 pitch)

10

IR Adaptive Optics: Key numbers

Incoming Plane Wave

Object

Atmospheric turbulence

Turbulent Phase Amplitude PV 10 à 50 µm

Turbulent wavefront Deformable Mirror

Uncorrected Image

Reconstruction & Control

WaveFront Sensor

FAWSA – JM Conan – Nov. 2016

Corrected wavefront

Corrected Image

11

Imaging Camera

Objective: Residual Amplitude PV < 1 µm (fraction of λim)

Implies a precise wave-front sensing precision : °spatial resolution ~ 50 cm ~ r 0 @ λim °temporal resolution ~ 2 ms ∝ (r0 @ λim / Vwind) °« bright » guide star > 100 photons / m ² / ms (0~12)

What if VIS AO ? r0 ÷ 6 !

Deformable Mirrors (DMs): Small Post-Focal DMs ‰ ‰

‰ ‰

Thin optical plate with aluminum coating Piezo-electric / Magnetic / Electrostatic actuators often on Cartesian grid Distance between actuators = pitch Typical size of DM: few cms to few decimeters implies optical conjugation between DM & Tel. pupil

FAWSA – JM Conan – Nov. 2016

pitch

Piezo DM (CILAS Orléan) Magnetic DM (ALPAO Grenoble)

pitch = spatial resolution ~ 50 cm ~ r0 @ λim 12

Deformable Mirrors (DMs): Adaptive Secondary Mirrors ‰ ‰

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Thin optical plate (1-2 m) Magnetic actuators (voice coil + magnets) driven by Nact control signals (generally current) Distance between actuators = pitch

MMT Deformable Secondary

FAWSA – JM Conan – Nov. 2016

typical diameter 1 or 2 meters ! Included in the telescope itself

Shack-Hartmann Wave-Front Sensor (WFS) d: sub-aperture size

FAWSA – JM Conan – Nov. 2016

WFS data are called “slopes”

« bright » guide star > 100 photons / m² / ms (0~12) 14

Typical design for VLT class IR Adaptive Optics : NAOS since 2001 on ESO VLT @ Paranal (Chile)

Beta Pictoris

FAWSA – JM Conan – Nov. 2016

‰ NAOS (coupled to CONICA IR Camera)

16

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15x15 actuators

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500 Hz sampling frequency (alias 2 ms temporal resolution)

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Guide star magnitude for good performance 0 ” 12

Faint companion: brown dwarf

Adaptive Optics: Concepts & Key Numbers ‰

‰

Correcting for turbulence with adaptive optics

‰

Key components & System specification

‰

Closing the loop & Corrected Images

New Developments in Adaptive Optics ‰

eXtreme Adaptive Optics: the search for exoplanets

‰

Wide Field Adaptive Optics : origin of the universe

‰

From VLT (10 m class) to ELT (30 m class) telescopes

‰

Beyond astronomical applications ?

FAWSA – JM Conan – Nov. 2016

‰

Adaptive Optics Principle

18

We can now close the loop ! ONERA AO bench Analyseur de surface d’onde (Shack-Hartmann)

miroir déformable SAM

caméra d’imagerie

FAWSA – JM Conan – Nov. 2016

RTC: PC-Linux (Shaktiware)

19

FAWSA – JM Conan – Nov. 2016

Observation of Io (Jupiter satellite) with AO@Keck

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Adaptive Optics: Concepts & Key Numbers ‰

FAWSA – JM Conan – Nov. 2016

‰

21

Adaptive Optics Principle ‰

Correcting for turbulence with adaptive optics

‰

Key components & System specification

‰

Closing the loop & Corrected Images

New Developments in Adaptive Optics ‰

eXtreme Adaptive Optics: the search for exoplanets

‰

Wide Field Adaptive Optics : origin of the universe

‰

From VLT (10 m class) to ELT (30 m class) telescopes

‰

Beyond astronomical applications ?

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)RUPDWLRQGHVpWRLOHVGDQVOHVJDOD[LHV Ö *DOD[LHVSURFKHV DNSF

1 à 100 light-years

103 à 107 light-years

)RUPDWLRQGHV*DOD[LHV Ö*DOD[LHVORLQWDLQHV j 0SF

FAWSA – JM Conan – Nov. 2016

108 light-years

1010 light-years eWXGHGHVJDOD[LHVSULPRUGLDOHV Ö QDLVVDQFHGHO·XQLYHUV *SF 

23

Adaptive Optics: Concepts & Key Numbers ‰

FAWSA – JM Conan – Nov. 2016

‰

24

Adaptive Optics Principle ‰

Correcting for turbulence with adaptive optics

‰

Key components & System specification

‰

Closing the loop & Corrected Images

New Developments in Adaptive Optics ‰

eXtreme Adaptive Optics: the search for exoplanets

‰

Wide Field Adaptive Optics : origin of the universe

‰

From VLT (10 m class) to ELT (30 m class) telescopes

‰

Beyond astronomical applications ?

19 30

18 46

eXtreme Adaptive Optics: SPHERE since 2014 on ESO-VLT

‰ Objective :

FAWSA – JM Conan – Nov. 2016

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detection of exo-planets around nearby stars

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flux ratio between star / exo-planet ~ 1 million !

SPHERE system : ‰

XAO system : 41x41 actuators ; sampling frequency 1200 Hz ; wave-front sensing on star 0 ” 10

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+ Coronagraph to suppress star photons

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+ spectro-imaging instruments

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+ smart post-processing

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Hence direct detection & analysis of exo-planet photons

25

SPHERE … from concept to reality Premières idées 2002 Design final 2008

Intégration à Grenoble (2011-13)

FAWSA – JM Conan – Nov. 2016

Sur VLT 2014

27

SPHERE compared with american competitor GEMINI-GPI GPI

*3

20 minutes in H band

15 minutes in H2 band

HD 165054, G4V, V=8.5 28

Preliminary reduced data © A. Vigan (LAM)

Adaptive Optics: Concepts & Key Numbers ‰

‰

Correcting for turbulence with adaptive optics

‰

Key components & System specification

‰

Closing the loop & Corrected Images

New Developments in Adaptive Optics ‰

eXtreme Adaptive Optics: the search for exoplanets

‰

Wide Field Adaptive Optics : origin of the universe

‰

From VLT (10 m class) to ELT (30 m class) telescopes

‰

Beyond astronomical applications ?

FAWSA – JM Conan – Nov. 2016

‰

Adaptive Optics Principle

31

FAWSA – JM Conan – Nov. 2016

Anisoplanatism issue

BAD NEWS : Guide star has to be bright and close to object of interest (within few arcsec) !

32

FAWSA – JM Conan – Nov. 2016

FAWSA – JM Conan – Nov. 2016

2 arcmin

33

10 arcsec

36

FAWSA – JM Conan – Nov. 2016

Laser Guide Star for Adaptive Optics

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Lasers for each and every telescope Gemini Sud

Sodium : λ = 589 nm Continuous Laser ~20 W

Subaru

(Keck)

WHT

FAWSA – JM Conan – Nov. 2016

VLT ESO

laser guide stars delivering the required few 100 ph/m²/ ms & low order aberrations (tip-tilt, focus...) measurement on very faint natural guide stars ~ 1 photon / m² / ms 38

Rayleigh : λ = 532 nm Pulsed @ 10kHz ~ 20 W

Multiplication of the Laser Guide Stars

FAWSA – JM Conan – Nov. 2016

There must be a smarter way...

44

Tomographic AO : think collective !

FAWSA – JM Conan – Nov. 2016

This should do!

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5 Sodium Laser Guide Stars

+ Tomographic AO GEMS

GEMINI South Chile 8m telescope

47

+ GSAOI IR Camera

5 Etoiles Laser

x3

+ 3 Etoiles Naturelles très faibles

49

Crédit Benoit Neichel AO4ELT3

Adaptive Optics: Concepts & Key Numbers ‰

‰

Correcting for turbulence with adaptive optics

‰

Key components & System specification

‰

Closing the loop & Corrected Images

New Developments in Adaptive Optics ‰

eXtreme Adaptive Optics: the search for exoplanets

‰

Wide Field Adaptive Optics : origin of the universe

‰

From VLT (10 m class) to ELT (30 m class) telescopes

‰

Beyond astronomical applications ?

FAWSA – JM Conan – Nov. 2016

‰

Adaptive Optics Principle

50

Extremely Large Telescopes are BIG ! European ELT 39 m telescope 798 individual segments (1.45m) to be cophased Up to 6 Laser Guide Stars 2.5 m deformable mirror with ~ 5316 actuators (2 mm thick, 6 petals)

fusion of ~30000 wave-front sensing data for tomographic AO !

51

FAWSA – JM Conan – Nov. 2016

Pupils through the ages

52

Adaptive Optics: Concepts & Key Numbers ‰

FAWSA – JM Conan – Nov. 2016

‰

53

Adaptive Optics Principle ‰

Correcting for turbulence with adaptive optics

‰

Key components & System specification

‰

Closing the loop & Corrected Images

New Developments in Adaptive Optics ‰

eXtreme Adaptive Optics: the search for exoplanets

‰

Wide Field Adaptive Optics : origin of the universe

‰

From VLT (10 m class) to ELT (30 m class) telescopes

‰

Beyond astronomical applications ?

High Resolution Imaging @ Onera Optics Dpt (DOTA) more than 100 researchers @ DOTA ; ~15 on High Resolution Imaging ‰

Earth-Space Observations (astronomy, earth obs...) Propagation through turbulence, adaptive optics, active optics

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Earth-Space Optical Links Turbulence effects on high data rate links and clock transfer

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Ophtalmology Aberrometry, adaptive optics assisted retinal imaging and surgery

FAWSA – JM Conan – Nov. 2016

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Microscopy Optical wave control for 2-photon microscopy and 3D imaging

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54

Beam shaping for high power lasers

more than 10 docs and post-docs on these research activities

54

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