The Giant Magellan Telescope AAS San Diego January 11, 2005 Matt Johns.

Slides:



Advertisements
Similar presentations
TheEuropean Extremely Large Telescope. The E-ELT 40-m class telescope: largest optical- infrared telescope in the world. Segmented primary mirror. Active.
Advertisements

GLAO Workshop, Leiden; April 26 th 2005 Ground Layer Adaptive Optics, N. Hubin Ground Layer Adaptive Optics Status and strategy at ESO Norbert Hubin European.
Telescope Projects at Steward Observatory Work in Progress Astronomical Society of New York Union College Saturday, 24 October 2009 Peter Wehinger Steward.
Thomas Stalcup June 15, 2006 Laser Guidestar System Status.
“Riding the Hub”: The MMT Adaptive Secondary Douglas Miller University of Arizona The AO System Current Performance of the MMT AO System Ongoing Development.
George Angeli 11 September, 2001 Current Concepts and Status of GSMT Control Systems.
Géraldine Guerri Post-doc CSL
The Project Office Perspective Antonin Bouchez 1GMT AO Workshop, Canberra Nov
Alt.Aperturer 0 (m)FWHM(")  0 (")  0 (sec) 4 kmCFHT 3.8m km2.4 m~ ~600~5 35km10 m~ ~600~5 h (km)P (mbars)T (K)  (gm m.
Intro to Stellar Astrophysics L21 The tools of astrophysics ä Virtually all information about the external Universe is received in the form of electromagnetic.
PILOT: Pathfinder for an International Large Optical Telescope -performance specifications JACARA Science Meeting PILOT Friday March 26 Anglo Australian.
Light and Telescopes Chapter 5. Traditional Telescopes The 4-m Mayall Telescope at Kitt Peak National Observatory (Arizona)
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.
AURA New Initiatives Office S.C. Barden, M. Liang, K.H. Hinkle, C.F.W. Harmer, R.R. Joyce (NOAO/NIO) September 17, 2001 Instrumentation Concepts for the.
Telescope Design The W.M. Keck (I & II) Telescopes Jana Hunt & Kent Van ME250 Precision Machine Design April 8, 2003.
GSMT Committee, Los Angeles, Oct. 20, Giant Magellan Telescope.
Extremely Large Telescopes and the Epoch of Reionization Xiaohui Fan(Arizona) with help from Pat McCarthy and GMT Science Working Group July 11, 2008,
PSWG March Adaptive Optics Systems Engineering on GMT Peter McGregor.
An Introduction to Adaptive Optics Mike Hein PH 464 – Applied Optics Winter 2005.
Figuring large off-axis segments to the diffraction limit Hubert Martin Steward Observatory University of Arizona.
Providing Access for US Astronomers to the Next Generation of Large Ground Based OIR Telescopes 1.Scientific Potential 2.Current Design Efforts 3.Complementarity.
Some large-telescope design parameter considerations: Distributed pupil telescopes J.R.Kuhn Institute for Astronomy, UH How to “distribute the glass” in.
Next generation wide field AO (GLAO) and NIRMOS for Subaru Telescope.
July 2001Zanjan, Iran1 Atmospheric Profilers Marc Sarazin (European Southern Observatory)
MCAO Adaptive Optics Module Mechanical Design Eric James.
Center for Astronomical Adaptive Optics Ground layer wavefront reconstruction using dynamically refocused Rayleigh laser beacons C. Baranec, M. Lloyd-Hart,
A visible-light AO system for the 4.2 m SOAR telescope A. Tokovinin, B. Gregory, H. E. Schwarz, V. Terebizh, S. Thomas.
OWL Instrument Concept Studies Within the OWL Conceptual Design to be completed by ESO in 3Q 2005, ESO collaborates with external institutes in the study.
AO4ELT - Paris Giant Magellan Telescope Project Science Drivers & AO Requirements Patrick McCarthy - GMT Director Phil Hinz & Michael Hart - GMT.
Telescope Technologies
Telescopes & recent observational techniques ASTR 3010 Lecture 4 Chapters 3 & 6.
2013 Survey Science Group Workshop, Feb High-1 Resort.
1 The LOFT group Who we are Where we came from Where we are going Large Optics Fabrication and Testing ?
Adaptive Optics Nicholas Devaney GTC project, Instituto de Astrofisica de Canarias 1. Principles 2. Multi-conjugate 3. Performance & challenges.
Adaptive Optics1 John O’Byrne School of Physics University of Sydney.
European Extremely Large Telescope - Status April ESO.
Viewing the Universe through distorted lenses: Adaptive optics in astronomy Steven Beckwith Space Telescope Science Institute & JHU.
Tomographic reconstruction of stellar wavefronts from multiple laser guide stars C. Baranec, M. Lloyd-Hart, N. M. Milton T. Stalcup, M. Snyder, & R. Angel.
Early scientific goals for the MMT’s multi-laser-guided adaptive optics Michael Lloyd-Hart, Thomas Stalcup, Christoph Baranec, N. Mark Milton, Matt Rademacher,
February 2013 Ground Layer Adaptive Optics (GLAO) Experiment on Mauna Kea Doug Toomey.
Future Plan of Subaru Adaptive Optics
ATLAS The LTAO module for the E-ELT Thierry Fusco ONERA / DOTA On behalf of the ATLAS consortium Advanced Tomography with Laser for AO systems.
ASTR 3010 Lecture 18 Textbook N/A
1 High-order coronagraphic phase diversity: demonstration of COFFEE on SPHERE. B.Paul 1,2, J-F Sauvage 1, L. Mugnier 1, K. Dohlen 2, D. Mouillet 3, T.
Australia’s Path to a Giant Telescope Matthew Colless MNRF Symposium 7 June 2003.
SITE PARAMETERS RELEVANT FOR HIGH RESOLUTION IMAGING Marc Sarazin European Southern Observatory.
1 Design and analysis for interferometric measurements of the GMT primary mirror segments J. H. Burge a,b, L. B. Kot a, H. M. Martin a, R. Zehnder b, C.
Technology Development for ELTs Doug Simons GSMT SWG April 28, 2003.
March 31, 2000SPIE CONFERENCE 4007, MUNICH1 Principles, Performance and Limitations of Multi-conjugate Adaptive Optics F.Rigaut 1, B.Ellerbroek 1 and R.Flicker.
Mega Telescopes of the 21 st Century Evolution in the Ground-Space Synergy Dr. Marc Postman (STScI) & Richard Ellis (Caltech) James Webb Space Telescope.
Na Laser Guide Stars for CELT CfAO Workshop on Laser Guide Stars 99/12/07 Rich Dekany.
Some Thoughts on Ground Layer Adaptive Optics & Adaptive Secondary Mirrors for Keck P. Wizinowich 9/15/14 1.
Pre-focal wave front correction and field stabilization for the E-ELT
A monitor of the vertical turbulence distribution MASS: Victor Kornilov a, Andrei Tokovinin b, Olga Vozyakova a, Andrei Zaitsev a, Nicolai Shatsky a, Serguei.
Science with Giant Telescopes - Jun 15-18, Instrument Concepts InstrumentFunction range (microns) ResolutionFOV GMACSOptical Multi-Object Spectrometer.
Wide field telescope using spherical mirrors Jim Burge and Roger Angel University of Arizona Tucson, AZ Jim
Opening New Frontiers with the GMT, Seoul, October Giant Magellan Telescope How does an adaptive secondary mirror support the unique qualities of.
GMT’s Near IR Multiple Object Spectrograph - NIRMOS Daniel Fabricant Center for Astrophysics.
Giant Magellan Telescope Project Status and Relationship with the NSF Astronomy and Astrophysics Advisory Committee February 8, 2007 Patrick McCarthy -
Theme 2 AO for Extremely Large Telescopes Center for Adaptive Optics.
François Rigaut, Gemini Observatory GSMT SWG Meeting, LAX, 2003/03/06 François Rigaut, Gemini Observatory GSMT SWG Meeting, LAX, 2003/03/06 GSMT AO Simulations.
J. H. Burgea,b, W. Davisona, H. M. Martina, C. Zhaob
Optomechanical Technologies for Astronomy, SPIE 6273 (2006)1 Manufacture of a 1.7 m prototype of the GMT primary mirror segments Buddy Martin a, Jim Burge.
A Tour of the Largest Ground-Based Telescopes Being Developed
The GMT Project The Giant Magellan Telescope (GMT)
Pyramid sensors for AO and co-phasing
The Giant Magellan Telescope
Theme 2 AO for Extremely Large Telescopes
Theme 2 AO for Extremely Large Telescopes
Theme 2 AO for Extremely Large Telescopes
Presentation transcript:

The Giant Magellan Telescope AAS San Diego January 11, 2005 Matt Johns

The GMT Institutions Carnegie Observatories Harvard University Smithsonian Astrophysical Observatory Massachusetts Institute of Technology University of Arizona University of Michigan University of Texas, Austin Texas A&M University + …OTHERS TBD

The GMT Organization Memorandum of Understanding Conceptual design phase funding. Work toward GMT incorporation agreement Governing bodies GMT Board: each institution has two members Science Working Group Project Scientists’ Working Group AO & Instrumentation Groups Project Office

GMT Design Alt-az structure Seven 8.4-m primary mirrors Cast borosilicate honeycomb 25.3-m enclosed diameter 24-m diffraction equivalent 21.5-m equivalent aperture 3.2-m adaptive Gregorian secondary mirror Instruments mount below M1 at the Gregorian focus

GMT Optical Design Primary Mirror D1 = 25.3 meter R1 = 36.0 meters K = f/0.7 primary mirror overall Gregorian secondary mirror D2 = 3.2 meter R2 = 4.2 meter K2 = Segments aligned with primary mirrors Combined Aplanatic Gregorian focus f/8.2 final focal ratio Field of view: arc-min. BFD = 5.5 meters M2 conjugate = 160 m above M1

GMT Structure Design goal: Compact, stiff Structure Low wind cross-section Maximize modal performance Minimum swing radius -> cost Model parameters Analysis includes telescope structure, optics, & instrument load Height = 36.1 meters Moving mass = 991 metric tons Lowest vibration mode = 5.1 Hz

Exploits 8.4 m experience Large 8.4m diameter subapertures of well-corrected wavefront. –Co-phasing not needed for seeing-limited imaging at  m Thick cross section (0.7m) resists surface deflection under wind loading. Developed technology –Active supports maintain figure accuracy & alignment in the telescope. –Thermal Control  Settling time: 1/e < 1 hour Existing production facilities & technology exists within the consortium at SOML. 8.4 m, f/1.14 LBT surface, 24 nm rms

Preparations for Casting GMT m off-axis segment Primary mirror production Pacing item for GMT completion Requires development of off-axis technology Modification of test tower Prototype mirror Casting contract signed December 2004 Projected casting date: July ‘05

Stressed Lap Polishing Machines at SOML LPM LOGTest tower Stressed lap

3.2-m Segmented Adaptive Gregorian Secondary Mirror Technology developed for MMT & LBT 7 ~2-mm thick facesheets aligned with Primary mirror segments attached to a single reference body. ~4700 voice coil actuators total Laser projector rides on top. 64 cm MMT AO secondary mirror

Adaptive Optics Modes First Generation AO Capabilities Ground layer AO (GLAO) Laser tomography AO Second Generation capabilities Extreme (high contrast) AO (ExAO) –Ref. J. Codona, SPIE Multi-conjugate AO (MCAO) Adaptive secondary mirror is the first deformable element in all AO systems.

Ground Layer AO (GLAO) with GMT Emerging technology. Low altitude turbulence correction. Secondary conjugation at 160m above primary. Natural guide stars or lasers. Performance goals: – > 0.8  –Field of view: > 10’ –Factor of reduction in image size. GLAO test at Magellan (A. Athey, SPIE ) GLAO at MMT Modeled using Cerro Pachon turbulence profile. (M-L Hart 2003)

LTAO Laser Tomography AO –Single conjugate AO with the AO secondary mirror & multiple lasers. –Diffraction limited imaging over full sky in the NIR. –Fields of view limited by tilt anisotropy Prototype systems under development at 1.5m telescope & MMT –Rayleigh beacons with dynamic re-focusing (DR) (Stalcup,SPIE ). –Sodium lasers will be required to scale up to GMT (Angel, SPIE ). Figure 89. (Left) Five beams projected on a 1 arcmin radius from a single 15–Watt laser using a custom hologram. The beams are seen here on the bottom of cloud. (Center) Images of the Rayleigh beacons gated between 20 – 30 kilometers without dynamic refocus. The streaking is caused by perspective elongation as seen through the off-axis 1.5-meter telescope. (Right) With dynamic refocus, the images become nearly circular. FWHM 6.4 arcsec H 2.7 arcsec V FWHM 2.8 arcsec 15w laser km DR off20-30 km DR on

Radial average of GMT diffraction-limited PSFs with a bandpass of 1.57 to 1.73 microns. Blue dash is the normal profile. Red line is with apodization of individual segments. Green line is 150-degree average of the PSF formed by phase compensation applied to the adaptive secondary. Extreme AO

Candidate First Generation Instruments #InstrumentWavelength (µm) Resolution R FOVAO ModeObserving Modes * 1Optical MOS ( ) ( ) 50 (150) sq. arcmin (GLAO)MOS/IFU/TF/Imager 2Near-IR MOS ( ) (250-10K) 25 (100) sq. arcmin GLAOMOS/IFU/TF/Imager 3Echelle k-50K3” slitNatural seeing Single Obj/Fiber-fed MOS/I cell 4MIR Spectrograph (3-25) 30K (100K)3” slitLTAOSingle Object 5NIR AO imager (3500)20” (30”)LTAO (ExAO, MCAO) Coronagraph/IFU/TF/ Imager 6MIR AO- Imager ”LTAOCoronagraph/IFU/TF Concepts under development

GMT Instrument Platform (IP) Rotator GLAO Guider Folded port instruments Gregorian instruments capacity 6.4 m Dia. 7.6 m high 25 ton Optical MOS Near-IR MOS Mid-IR Spectrograh Echelle NIR AO imager NIR Echelle Small-intermediate sized intstruments Rapid exchange

GMT Enclosure Concept

Enclosure Structure M3 Engineering Height: 60 m Diameter: 54 m Structure design & cost study complete 12/04 Thermal & flow studies On-site Facilities design mid-2005

Site Testing Northern Chile location GMT conducting tests at 4 LCO sites Coordinate/share data with other projects Test equipment Differential Image Motion Monitors (DIMM) Multi-aperture Scintillation Sensor (MASS) Meteorological stations Magellan (Manqui)Campanas Pk. Alcaino Pk. Ridge (Manquis)

Decadal Survey Key Problems 1.Large-Scale properties of the Universe, Matter, Energy, Expansion History 2.First Stars and Galaxies 3.Formation and Evolution of Black Holes 4.Formation of Stars and Planetary Systems 5.Impact of Astronomical Environment on the Earth “Astronomy & Astrophysics in the New Millennium”

GSMT Key Science Areas * Origin of Large-Scale Structure Building of the Milky Way and Other Galaxies Exploring Other Solar Systems * Frontier Science Enabled by a Giant Segmented Mirror Telescope

GMT Science Priorities * Physical Studies of Exoplanets Star Formation & the Origin of the IMF Stellar Populations & Chemical Evolution The Nature of Dark Matter and Dark Energy Galaxy Assembly Black Hole Growth First Light & Reionization of the Universe * The Giant Magellan Telescope: Opening a New Century of Cosmic Discovery

GMT Science & Technology in Context The GMT Scientific priorities and capabilities: Address the key decadal survey goals Are aligned with the GSMT science priorities The GMT design will readily Adapt to new discoveries & evolving priorities Enhance value of ALMA, JWST, & other existing and planned facilities

Schedule

The central peak of the GMT PSF contains 65% of the total incident flux, compared to 84% for a filled circular aperture. FWHM is the same as for 24 m filled aperture: 40 mas FWHM at 5  m 8 mas FWHM at 1  m Reaching the diffraction limit of the GMT with adaptive optics

Ground layer measured with laser at MMT 9/28/04 Telescope measurement of ground layer seeing (Michael Lloyd Hart et al) 5 Rayleigh beacons in 2 arcminute circle 30W 532 nm YAG laser Centered around natural star in 0.7” seeing

Rms wavefront error summed over all 6 orders. bavg = average of all 5 LGS signals

phase information for closed loop operation will come from a natural star. A single NGS can sense the 6 relative pistons in addition to regular tip/tilt. (Need 8 modes from 7x8.4 m mirrors; better than 2 modes from 1x8.4 m on current large telescope with LGS, so should not at all compromise sky cover.) Sub-pupil Quarter-wave piston error PSF MTFs Absolute piston measurement Piston misregistration has unique effects on the MTF of three partially non- redundant arrays made from the full pupil. Each M1 segment is used exactly twice. Ideal PSFs are shown in second column. A quarter wave of piston on either an edge or center segment will affect two of the three MTFs. (N.B. MTFs are shown at much higher resolution than would actually need to be sampled.) GMT cophasing of 7 segments (Lloyd Hart)

Test configuration

New test tower at Mirror Lab * Needed for 8.4 m off-axis segments * Long 36 m radius of curvature (LBT = 20 m) * Requires diffraction limited 4 m folding spherical mirror at top