AOLI-- Adaptive Optics Lucky Imager: Diffraction Limited Imaging in the Visible on Large Ground-Based Telescopes Craig Mackay, Rafael Rebolo-López, Bruno.

Slides:



Advertisements
Similar presentations
The Adaptive Optics Lucky Imager High-resolution imaging in the visible on large ground-based telescopes Jonathan Crass Institute of Astronomy, University.
Advertisements

Optics and Telescopes Chapter Six. Telescopes The fundamental purpose of any telescope is to gather more light than the naked eye can In many cases telescopes.
Astronomy and the Electromagnetic Spectrum
Extragalactic AO Science James Larkin AOWG Strategic Planning Meeting September 19, 2004.
© 2011 Pearson Education, Inc. Lecture Outlines Astronomy Today 7th Edition Chaisson/McMillan © 2011 Pearson Education, Inc. Chapter 5.
Optics and Telescopes Chapter Six.
PILOT: Pathfinder for an International Large Optical Telescope -performance specifications JACARA Science Meeting PILOT Friday March 26 Anglo Australian.
Imaging Science Fundamentals Chester F. Carlson Center for Imaging Science Astronomical Imaging Telescopes and Detectors.
Aug-Nov, 2008 IAG/USP (Keith Taylor) ‏ Instrumentation Concepts Ground-based Optical Telescopes Keith Taylor (IAG/USP) Aug-Nov, 2008 Aug-Sep, 2008 IAG-USP.
Astronomy 101 Section 020 Lecture 6 Optics and Telescopes John T. McGraw, Professor Laurel Ladwig, Planetarium Manager.
5 Telescopes How big is yours?. 5 Goals Telescopes Angular Sizes “Seeing” Magnitudes.
Telescopes (Chapter 6). Based on Chapter 6 This material will be useful for understanding Chapters 7 and 10 on “Our planetary system” and “Jovian planet.
NGAO Science Instruments Build to Cost Status February 5, 2009 Sean Adkins.
The Imaging Chain for Optical Astronomy. Review/overview The imaging chain typically includes the following elements: –energy source –object –collection.
Diffraction-limited imaging in the visible at the WHT Craig Mackay, Institute of Astronomy, University of Cambridge. 22 March 2010: Science with WHT.
Telescopes Collect more light than eye More detailed images than human eye Larger aperture is better –Aperture refers to the diameter of the primary lens.
Telescopes and Astronomical Instruments The 2 main points of telescopes are 1)To make images with as much angular information as possible 2)To gather as.
Astronomical Spectroscopy
Optics and Telescopes Chapter Six.
Diffraction Limited Imaging from the Largest Ground-Based Telescopes in the Visible Craig Mackay, Jonathan Crass, David L. King Institute of Astronomy,
Page 1 AO in AO A daptive O ptics in A stronomical O bservations Diana R. Constantin ASTRONOMICAL INSTITUTE OF THE ROMANIAN ACADEMY.
Issues with the use of telescopes
4. Telescopes Light gathering power and resolution Optical and radio telescopes Limitations of Earth’s atmosphere and satellite missions. Instruments (prism.
A visible-light AO system for the 4.2 m SOAR telescope A. Tokovinin, B. Gregory, H. E. Schwarz, V. Terebizh, S. Thomas.
STATUS REPORT OF FPC SPICA Task Force Meeting March 29, 2010 MATSUMOTO, Toshio (SNU)
Telescopes & recent observational techniques ASTR 3010 Lecture 4 Chapters 3 & 6.
© 2004 Pearson Education Inc., publishing as Addison-Wesley Telescopes.
Adaptive Optics Nicholas Devaney GTC project, Instituto de Astrofisica de Canarias 1. Principles 2. Multi-conjugate 3. Performance & challenges.
“Twinkle, Twinkle Little Star”: An Introduction to Adaptive Optics Mt. Hamilton Visitor’s Night July 28, 2001.
15 October Observational Astronomy Direct imaging Photometry Kitchin pp ,
Astronomy 1020-H Stellar Astronomy Spring_2015 Day-21.
Issues with the use of telescopes Magnification Magnification determines how much larger the image is as compared to the size of the source of the light.
NORDFORSK Summer School, La Palma, June-July 2006 NOT: Telescope and Instrumentation Michal I. Andersen & Heidi Korhonen Astrophysikalisches Institut Potsdam.
February 2013 Ground Layer Adaptive Optics (GLAO) Experiment on Mauna Kea Doug Toomey.
TELESCOPES Astr 221 Lec 3 Spring 2015 (Ch. 5 in Nightwatch)
ASTR 3010 Lecture 18 Textbook N/A
Hubble Space Telescope Coronagraphs John Krist JPL.
Observing Venus (and Mars) with Adaptive Optics
SUNYAEV-ZELDOVICH EFFECT. OUTLINE  What is SZE  What Can we learn from SZE  SZE Cluster Surveys  Experimental Issues  SZ Surveys are coming: What.
SITE PARAMETERS RELEVANT FOR HIGH RESOLUTION IMAGING Marc Sarazin European Southern Observatory.
Telescopes. Light Hitting a Telescope Mirror huge mirror near a star * * * small mirror far from 2 stars In the second case (reality), light rays from.
Adaptive Optics for Astronomy Kathy Cooksey. AO Basics Photons –Travel in straight lines Wavefront –Line perpendicular to all photons’ paths Atmospheric.
Astronomy 1010-H Planetary Astronomy Fall_2015 Day-22.
Mega Telescopes of the 21 st Century Evolution in the Ground-Space Synergy Dr. Marc Postman (STScI) & Richard Ellis (Caltech) James Webb Space Telescope.
Telescopes Lecture. Standards Understand how knowledge about the universe comes from evidence collected from advanced technology (e.g., telescopes, satellites,
HLA WFPC2 Source List Photometric Quality Checks Version: August 25, 2008 Brad Whitmore 1.Introduction 2.Comparison with Ground-based Stetson Photometry.
Astronomy with cm – Mpc lenses Phil Marshall KIPAC – SLAC – Stanford University February 28 th 2004.
Surface Layer SLODAR J. Osborn, R. Wilson and T. Butterley A prototype of a new SLODAR instrument has been developed at Durham CfAI and tested at the Paranal.
Telescopes Resolution - Degree to which fine detail can be distinguished Resolution - Degree to which fine detail can be distinguished Fundamentally an.
Overview Science drivers AO Infrastructure at WHT GLAS technicalities Current status of development GLAS: Ground-layer Laser Adaptive optics System.
Robo-AO Overview: System, capabilities, performance Christoph Baranec (PI)
Theme 2 AO for Extremely Large Telescopes Center for Adaptive Optics.
Introduction of RAVEN Subaru Future Instrument Workshop Shin Oya (Subaru Telescope) Mitaka Adaptive Optics Lab Subaru Telescope Astronomical.
Page 1 Adaptive Optics in the VLT and ELT era François Wildi Observatoire de Genève Credit for most slides : Claire Max (UC Santa Cruz) Basics of AO.
Diffraction Limit What is the best angular resolution a telescope would achieve in idealised conditions? Circular aperture: θ min ≈ 1.22 λ/d For the HST:
Chapter 6 Telescopes: Portals of Discovery
Jeffrey R. Regester Greensboro Day School Greensboro NC
Telescopes.
Pyramid sensors for AO and co-phasing
Into to Telescopes Version for CSUEB (8” Celestron)
Telescopes & Detectors
Theme 2 AO for Extremely Large Telescopes
4. Telescopes Light gathering power and resolution
Telescopes (Optical Instruments)
Observational Astronomy
Optics and Telescopes Chapter Six.
Telescopes Lecture.
“Twinkle, Twinkle Little Star”: An Introduction to Adaptive Optics
Theme 2 AO for Extremely Large Telescopes
Theme 2 AO for Extremely Large Telescopes
Presentation transcript:

AOLI-- Adaptive Optics Lucky Imager: Diffraction Limited Imaging in the Visible on Large Ground-Based Telescopes Craig Mackay, Rafael Rebolo-López, Bruno Femenia Castellá, Jonathan Crass, David L. King, Lucas Labadie, Peter Aisher, Antonio Pérez Garrido, Marc Balcells, Anastasio Díaz-Sánchez, Jesús Jimenez Fuensalida, Roberto L. Lopez, Alejandro Oscoz, Jorge A. Pérez Prieto, Luis F. Rodríguez-Ramos, Isidro Villó. (AOLI team: IAC La Laguna, ING La Palma and Universities of Cartagena, Cologne and Cambridge) 5 July, 2012: SPIE

Our understanding of the Universe has been transformed by the Hubble space telescope that has freed us from the limitations of atmospheric turbulence on ground. We can build telescopes on the ground with extraordinary angular resolution but the atmosphere limits us to ~1 arcsec. AO now works in the near-IR, but less successful in the visible. Our science programmes emphasise distant, compact and faint targets over the whole sky. Our goal is to allow large telescopes to produce near diffraction limited images over much of the sky using natural guide stars. To do this we really have to rethink many of the assumptions conventionally made about how this might be achieved. Introduction and Outline 5 July, 2012: SPIE

High Resolution Imaging from the Ground in the Visible The only technique that can routinely deliver Hubble resolution images on Hubble size (~2.4m) telescopes in the visible on the ground is Lucky Imaging. It is our shared experiences with Lucky Imaging that brought our team together. High-speed photon counting CCD cameras freeze the motion due to atmospheric turbulence. A moderately bright ( I<16.5 mag ) reference star in the field allows image sharpness to be measured. By shifting and adding the best images we can produce near diffraction limited resolution in the visible. 5 July, 2012: SPIE

The image on the left is from the Hubble Space Telescope Advanced Camera for Surveys (ACS) while the image on the right is the lucky image taken on the NOT in July 2009 through significant amounts of dust. The central slightly fuzzy object is the core of the nearby Zwicky galaxy, ZW that gives four gravitationally lensed images of a distant quasar at redshift of 1.7 The Einstein Cross 5 July, 2012: SPIE

Lucky Imaging on Large Telescopes On telescopes larger than Hubble (4-10 meter diameter), the chance of a sharp image becomes negligible. There are too many turbulent cells of size ~r 0 over the telescope aperture. Most of the turbulent power is on the largest scales. If they are removed, the effective turbulent cell size, r 0, is increased, and the number over the aperture is reduced. This increases the chance of a sharp Lucky Image. Demonstrated 5 years ago on the Palomar 5 m telescope with our lucky camera behind the PALMAO AO system. 5 July, 2012: SPIE

Globular cluster M13 on the Palomar 5m. Seeing ~650 mas. PALMAO system and our EMCCD Camera. Achieved 17% Strehl ratio in I-band, giving ~35 mas resolution. This is the highest resolution image ever taken in the visible. Large Telescope Lucky Imaging. 5 July, 2012: SPIE

22 March, 2012: Open University Compare Lucky/AO and Hubble Advanced Camera (ACS) is quite dramatic. The Lucky/AO images have a resolution ~35 milliarcseconds or nearly 3 times that of Hubble. Large Telescope Lucky Imaging.

22 March, 2012: Open University AOLI (Adaptive Optics Lucky Imager) AO usually needs a bright reference star. We will use a non-linear curvature wavefront sensor (Guyon). Much more sensitive than S-H sensors for low-order AO (Racine). We use 4 out-of-pupil images, and fit the wavefront curvature. Reference star x fainter than S/H, ~achromatic in low order. Wavefront fit quality gives Lucky Image selection and full PSF info. (From Olivier Guyon, Subaru telescope, Hawaii).

AOLI Layout. AOLI uses a 97 element long stroke ALPAO deformable mirror. The reference star is always on the optical axis, and the science field may be offset by up to 2 arc minutes. It feeds the science camera, 4 EMCCDs, optically butted to give 2048 x 2048 pixel field of view. 22 March, 2012: Open University

Curvature Sensor Layout. The reference star light is split 4 ways using two beam splitters. Two photon counting EMCCDs running at 100 Hz, in sync with the science EMCCDs record a pair of near pupil images. Each set of 4 images allows the wavefront to be reconstructed and the deformable mirror driven quickly. Reference star limiting I-band magnitude should be mag for the WHT 4.2 m, and mag for the GTC 10.4 m 22 March, 2012: Open University

Science Camera Layout. EMCCDs are not optically buttable so we follow the original Hubble WF/PC concept of using a shallow angle prism to split the beam giving a contiguous 2048 x 2048 pixel field of view. 22 March, 2012: Open University The magnification is variable: from 6-60 milliarcseconds per pixel. Each CCD may have a different filter.

Enhanced Efficiency Lucky Imaging With Lucky Imaging, the sharpest images come from the smallest fraction of images. Often the less good images are smeared in one direction only yet still showing excellent resolution in other directions. Garrel et al (PASP, 2012) suggested making the lucky selection in Fourier space rather than image space. Results below: Globular cluster M13,770nm : HST/ACS, lucky selection of 10% in image space, 20% and 50% in Fourier space. FOV 2.0 x 1.5 arcseconds, 35 mas resolution.

Enhanced Efficiency Lucky Imaging With Lucky Imaging, the sharpest images come from the smallest fraction of images. Before & after plots from the globular cluster field. Left-hand image very near reference star, right-hand image 12 arcseconds away. Profiles show different selection percentages. These curves show selection percentages from 1% (top) to 50%. 1-50% seln.

Conclusions The combination of Lucky Imaging behind a low order non- linear curvature wavefront sensor based AO system looks to be particularly powerful. It should allow near-diffraction limited imaging on large ground-based telescopes in the visible over much of the sky. The key technology is the availability of high-speed, high quantum efficiency photon counting EMCCD detectors. AOLI has the potential to feed not only an imaging camera but also an integral field spectrograph or other instruments. AOLI offers astronomers the opportunity to carry out entirely new kinds of research at the very faintest signal levels with near diffraction limited image resolution. 5 July, 2012: SPIE

Instrumentation Group Institute of Astronomy University of Cambridge, UK 5 July, 2012: SPIE