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New Technologies for Exoplanet Detection with Mid-IR Interferometry
Peter R. Lawson
Oliver Lay, Stefan Martin, Robert Peters, Andrew Booth, Robert Gappinger, Alexander Ksendzov, and Daniel Scharf
Jet Propulsion LaboratoryCalifornia Institute of Technology
New Technologies for Probing the Diversity of Brown Dwarfs and Exoplanets
Shanghai, ChinaThursday, 23 July 2009
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 2
Overview
Spectra of Earth-like exoplanets Architecture & Design Team Studies Technology Demonstrations Future Prospects Summary and Conclusion
Terrestrial Planet Finder
May 1999
McKee–Taylor Report: Decadal Survey 2000
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 3
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 4
Frank Selsis (Lyon)
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 5
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 6
Architecture Trades
and
Design Team Studies
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 7
TPF-Darwin Architecture Studies
Linear DCB
TPF-I Darwin
Bow-Tie
X-Array Planar TTN
Emma TTN
Emma X-Array
TPF-Darwin
Stretched X-Array
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 8
Properties of a TPF-I Observatory
Illustrative Properties of a TPF-I Observatory Concept
Parameter 4-Telescope Chopped X-Array Emma Design
Collectors Four 2-m diameter spherical mirrors, diffraction limited at 2 μm operating at 50 K
Array shape 6:1 rectangular array
Array size 400 × 67 m to 120 × 20 m
Wavelength range 6–20 µm
Inner working angle 13–43 mas (at 10 m, scaling with array size)
Angular resolution 2.4 mas to 8.2 mas (at 10 μm, scaling with array size)
Field-of-view 1 arcsec at 10 µm
Null depth 10-5 at 10 m (not including stellar size leakage)
Spectral resolution Δλ/λ 25 (for planets); 100 for general astrophysics
Sensitivity 0.3 µJy at 12 µm in 14 hours (5)
Target Stars 153 (F, G, K, and M main-sequence stars)
Detectable Earths 130 (2 year mission time, 1 Earth per star)
Exozodiacal emission Less than 10 times our solar system
Biomarkers CO2, O3 , H2O, CH4
Field of regard Instantaneous 45° to 85° from anti-Sun direction, 99.6% of full sky over one year.
Orbit L2 Halo orbit
Mission duration 5 years baseline with a goal of 10 years
Launch vehicle Ariane 5 ECA or equivalent
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 9
Mass estimates and launch packaging
3 m design = 6900 kg (w 30% reserve) Mass saving of 30% over previous
design Compatible with medium lift LV
– Delta IV M+
– Ariane 5 ECA
Scaling to smaller diameters– 3.0 m 6900 kg
– 2.0 m 4800 kg
– 1.5 m 4100 kg
– 1.0 m 3700 kg
Inspired by a design by Thales Alenia Space
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 10
Technology Demonstrations
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 11
Technology for a Mid-IR Interferometer Starlight suppression
– Null depth & bandwidth– Null stability
Formation flying– Formation control– Formation sensing– Propulsion systems
Cryogenic systems– Active components– Cryogenic structures– Passive cooling– Cryocoolers
Integrated Modeling– Model validation and testbeds
Science Requirements Architecture trade studies
Technology forStarlight and Noise Suppression
Spatial FilteringAdaptive Nulling
Array Rotation, Chopping, and AveragingSpectral Filtering
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 13
Single-Mode Mid-Infrared Fibers
Chalcogenide Fibers (NRL)– A. Ksendzov et al., “Characterization of mid-
infrared single mode fibers as modal filters,” Applied Optics 46, 7957-7962 (2007)
– Transmission losses 8 dB/m
– Suppression of 1000 for higher order modes
– Useable to ~11 microns
Silver-Halide Fibers (Tel Aviv Univ)– A. Ksendzov et al. “Modal filtering for mid-
infrared nulling interferometry using silver halide fibers,” Applied Optics 47, 5728-5735 (2008).
– Transmission losses 12 dB/m
– Suppression of 16000 possible with a 10-20 cm fibre, with aperturing the output.
– Useable to ~18 microns (?)
Example Chalcogenide Fibers, produced on contract by the Naval Research Laboratory
http://planetquest.jpl.nasa.gov/TPF-I/spatialFilters.cfm
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 14
Broadband Intensity and Phase Compensation
Parabolic mirror~ 10 x 14 cm
Uncompensatedbeam in (~4 cm)
Dispersive elementsplits wavelengths
Birefringent elementsplits polarizationsPupil
Stop
Compensatedbeam out (~4 cm)
PupilStop Birefringent element
re-combines polarizations
Dispersive elementre-combines wavelengths
S-polarization
Deformablemirror
P-polarization
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 15
TPF-I Milestone #1 and #3: Adaptive Nuller
Adaptive Nuller
– TPF-I Milestone #1 completed, July 2007
• Demonstrated 0.09% intensity compensation and 4.4 nm phase compensation
– TPF-I Milestone #3 completed, February 2009
• Demonstrated 1.0×10-5 mean null depth with a 34% bandwidth in three 6-hour experiments.
“Broadband phase and intensity compensation with a deformable mirror for an interferometric nuller,” R. D. Peters, O. P. Lay and M. Jeganathan, Applied Optics 47, 3920-3926 (2008).
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 16
100,000:1 with 34% Bandwidth, = 10 m
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 17
Chop, Rotate, Average, Spectral Fit
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 18
– Demonstrate array rotation, chopping, and averaging
– Detect planet signal at a contrast of ≤ 10-6 relative to the star
– Show residual starlight suppression from phase chopping and rotation ≥ 100.
– Tests run for a total duration of 10,000 s, with one or more rotations at timescales of ≥ 2000 s.
Planet Detection Testbed
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 19
Technology forFormation Flying
Guidance, Navigation & Control
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 21
Precision Formation Flying
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 22
Precision Leader-Follower Maneuver
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 23
TPF-I Milestone #2: Formation Control Testbed
TPF-I Milestone #2 experiments for the formation precision performance maneuver were completed 30 September 2007
Goal:Per axis translation control < 5 cm rmsPer axis rotation control < 6.7 arcmin rms Demonstrated with arcs having 20 and 40 degree chords. Experiments repeated three times, spaced at least two days apart.
Milestone Report published 16 January 2008
Formation Control Testbed
Example Milestone Data: Rotation maneuver with 20 degree chord segments
x axis 2.66 arcmin rmsy axis 2.93 arcmin rmsz axis 1.67 arcmin rms
x axis 4.77 arcmin rmsy axis 5.14 arcmin rmsz axis 2.70 arcmin rms
x axis 1.39 cm rmsy axis 2.41 cm rms
Relative path of robots for an arc with 20 degree chords
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 24
Recent Advances in Formation Flying
Orbital Express (DARPA) May-July 2007– Demonstrated in-orbit servicing of satellites
– Relative maneuvers of two satellites
– Transfer of liquids and batteries
Autonomous Transfer Vehicle (ESA) April 2008– Unmanned transport to the International Space
Station
– 10.3-m long and 4.5-m diameter
– GPS, video, and human supervision
– Two days of demos, and rendezvous and docking
– 30 September 2008, completed a destructive re-entry
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 25
Prisma (2009) and Proba-3 (2012) Prisma (Swedish Space Corporation) launch 24 November 2009
– Rendezvous and docking demonstrations
– Prototype “Darwin” RF metrology
Proba-3 (ESA) 2012– 30-150 m separation for demonstrations
– Millimeter-level range control
– RF Metrology & Optical metrology
– AO for the provision of the coronagraph now out
• http://sci.esa.int/proba_3_AO
Prisma
Proba-3
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 26
Related New Technologies
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 27
Large Light-Weight Optics
Herschel Primary Mirror
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 28
CryocoolersAdvanced Cryocooler Technology
Development Program
JWST Cryocooler (NGST)
Technology Development in Europe Infrared Nulling testbeds (ESA)
– Thales Alenia Space
– EADS Astrium
– University of Delft
– Institut d’Astrophysique Spatiale Cryogenic Delay Line (ESA)
– TNO, The Netherlands
Integrated Optics and Fiber Optics (ESA)– LAOG, Université Joseph Fourier, Grenoble
– Thales Alenia Space
– EADS Astrium / TNO
– Université de Rennes
– Université de Montpellier Breadboard demonstrator for PEGASE (CNES) Cryogenic mid-IR testbed, Inst. Astrophysique Spatiale
(under design) RF Metrology for formation flying (Thales Alenia Space)24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 29
Thales Alenia Space
Inst. Astrophysique Spatiale
TNO
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 30
Interferometer Technology Metrics
Technology Specs Performanceto date
Performance target prior to
Phase A
FlightPerformance(preliminary)
Nulling
Averagenull depth
9.9x10-6 (34%BW)Milestone #3 1.0x10-5 1.0x10-5
Intensity control
0.09%Milestone #1 0.2% 0.13%
Phase control
4.4 nmMilestone #1 5.0 nm 1.5 nm
Stability timescale
21,600 sMilestone #1 5,000 s > 50,000 s
Bandwidth8.4-11.6 µm
(34%)Milestone #1
8.3 to 10.7 µm(25%) 7 to 17 µm
FormationFlying
Number of S/C 2 Robots 3 Robots 5 S/C
Relative control
1.4 - 4.6 cm range, 1σ(formation rotation)
Milestone #2
5 cm range, 1σ(formation rotation)
2 cm range
Accomplished1999–2009
31
Room-temperature experiments & ground-based
• Broadband mid-infrared starlight suppression has been demonstrated at flight performance levels using the adaptive nuller
• System-level planet detection has been demonstrated using the Planet Detection Testbed
• Formation Flying algorithms demonstrated with traceability to flight.
Related cryogenic technology
• Herschel mirror development
• Cryocooler work for JWST
• Cryogenic delay line development for ESA
3124 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers
Remaining2010–2020
Cryogenic engineering & space-based testing
• Demonstrate component, subsystem, and system performance in a cryogenic environment
• Demonstrate the detection of biosignatures
• Validate models of the observatory
• Complete integration and test plans
• Demonstrate space-based interferometry
• Demonstrate space-based formation flying
Further Reading
32
R. D. Peters, O. P. Lay, and M. Jeganathan, “Broadband phase and intensity compensation with a deformable mirror for an interferometric nuller,” Applied Optics 47, 3920–3926 (2008)
A. Ksendzov, et al., “Modal filtering for mid-infrared nulling interferometry using single-mode silver halide fibers,” Applied Optics 47, 5728–5735 (2008)
A. Ksendzov, et al., “Characterization of mid-infrared single mode fibers as modal filters,” Applied Optics 46, 7957–7962 (2007)
R. O. Gappinger, et al. “Experimental evaluation of achromatic phase shifters for mid-infrared starlight suppression,” Applied Optics 48, 868–880 (2009)
32
http://planetquest.jpl.nasa.gov/TPF-I/
This work was conducted at the Jet Propulsion Laboratory, California Institute of Technology, under contract with the National Aeronautics and Space Administration.
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 33
Backup Slides
24 July 2009 - Shanghai, China P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers 34
Terrestrial Planet Finder Interferometer
Salient Features• Formation Flying Mid-IR nulling
Interferometer • Starlight suppression to 10-5 • Heavy launch vehicle• L2 baseline orbit• 5 year mission life (10 year goal)• Potential collaboration with
European Space Agency
Science Goals• Detect as many as possible Earth-like planets in the “habitable zone” of nearby stars via
their thermal emission• Characterize physical properties of detected Earth-like planets (size, orbital parameters,
presence of atmosphere) and make low resolution spectral observations looking for evidence of a habitable planet and bio-markers such as O2, CO2, CH4 and H2O
• Detect and characterize the components of nearby planetary systems including disks, terrestrial planets, giant planets and multiple planet systems
• Perform general astrophysics investigations as capability and time permit
State of the Art in Nulling Interferometry
24 July 2009 - Shanghai, China 35P. R. Lawson, New Technologies for Exoplanet Detection with mid-IR Interferometers