a single-mode nulling rotating coronagraph for high...

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1 A Single-Mode Nulling Rotating Coronagraph for High Contrast Ground Based Imaging Bertrand Mennesson Gene Serabyn, Stefan Martin and Kurt Liewer Caltech / Jet Propulsion Laboratory Spirit of Lyot Conference Berkeley, June 4-8, 2007 “Batiment” Lyot at the Paris Observatory (Meudon site) Where COME-ON, FLUOR, NAOS etc were conceived, tested and partly assembled

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  • 1

    A Single-Mode Nulling RotatingCoronagraph for High Contrast

    Ground Based Imaging

    Bertrand MennessonGene Serabyn, Stefan Martin and Kurt Liewer

    Caltech / Jet Propulsion Laboratory

    Spirit of Lyot ConferenceBerkeley, June 4-8, 2007

    “Batiment” Lyot at the Paris Observatory(Meudon site)

    Where COME-ON, FLUOR, NAOS etc were conceived, tested and partly assembled

  • 2

    Current limits for high contrast / high resolutionground based imaging: single telescopes

    Classical Lyot coronagraphs: central 4-5 λ/D is not accessible

    Apodized coronagraphs and phase mask coronagraphs: cantheoretically image companions at λ/DHigh dynamic range inside 3-4 λ/D only accessible with very highStrehl (> 90% restricted to small D or future ExAO systems)

    Speckle interferometry: imaging at λ/D, dynamic range of a few tens

    Aperture masking (Keck, Palomar): allows imaging within λ/D butwith dynamic range still limited by V accuracy (fibers would help)

    Current off axis point source detection limit:~1000:1 at 5λ/D, degrading to ~100:1 at λ/D

    Current limits of high contrast /high resolutionground based imaging: long baseline

    interferometers

    Very high angular resolution (down to ~1mas in thenear IR), but dynamic range limited to:

    20-30:1 for conventional (bulk optics) interferometers

    ~100:1 using single-mode waveguide recombination andphotometric calibration (FLUOR)

    ~100:1 or better using nulling in the mid–IR (MMT, KECK,LBTI). Nulling brings extra spatial resolution

    Contrast limit for detection of off-axis sourcesis ~100:1

  • 3

    Bridging the gap: near IR fiber nulling ona single-telescope

    Principle: rotating nuller feeding a single-mode fiber

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    FIBER NULLER POSSIBLE IMPLEMENTATIONS

    Multi-Axial Co-Axial

  • 4

    Possible Nulling Beam Combinations

    Co-axial recombination:+ Variety of solutions provide achromatic nulls:RSI: rooftops, periscopes, LSI: dielectric plates + MMZ+ Proven techno (Wallace, Serabyn, Mennesson etc)

    Multi-axial recombination:Beam combiner = focusing element + fiber+ Easier to implement on telescope+ Adaptability to a large number of sub-beams- Deep nulls unproven before 2005- Fiber injection efficiency lower

    “A la FLUOR or IONIC” Would need zero dispersion waveguides e.g. photonic fibers

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    The Multi-axial (Fiber) Combiner

    SM Fiber provides 2 in 1: Beam Combination and Spatial Filtering

  • 5

    Lab results: visible LASER

    Lab results: visible LASER

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  • 6

    Lab results: visible LASER

    Best nulls are 1.3x10-6 (from Haguenauer & Serabyn, Applied Optics, 2006

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    Lab results: white lightDielectric Plates

  • 7

    Lab results: white light

    Dual Polarization Stable White Light (1.5 to 1.8 microns) Null Level: ~6x10-5

    Multi-axial recombination (Mennesson et al. 2007 in prep)

    Key Advantages High contrast accessible without high Strehl (fiber corrects

    individual wavefronts)

    Ultimate contrast fixed by OPD rms over unit integration time K band Nulls of 1e-3 readily accessible using 10ms sampling

    Spatial resolution = λ/2B (56 mas in K with B=4m), half transmissionpoint is λ/4B =28 mas

    Null level is constant over FOV. Achievable detection limit is fixedby fringe pattern Tr, not by field dependent residuals

    Can theoretically achieve 500:1 detection at λ/D in the near IR

    Much simpler to implement than long baseline interferometry;baseline can rotate much faster

  • 8

    Limitations• FOV limited to diffraction limit of sub-aperture λ/d ~ 3-4λ/D. Really

    tailored to high angular resolution.Could work in conjunction with conventional coronagraph accessinglarger separations

    • Sensitivity loss wrt to full telescope• Both limitations reduced when using more small sub-apertures

    Injection efficiency into a singlemode fiber using b/d =3.5m/1.5m(Multi-axial combination, nodensification, Palomar 200 inch) at2.2 microns. Plain curve:constructive case. Dotted curve:nulling case. A denser pupil, asavailable on Keck or Subaru, willallow better on-axis couplingefficiency, up to 62% in the idealcase where b=d Dotted curve:nulling case.

    Simulated Performance of Palomar system:two 1.5x3m sub-apertures 3.5m apart

    K band signal detected over 60 baseline rotations (5s each, sampled at 100Hz)

    Left: mK=3 star with 500 times dimmer companion 40 mas away

    Right: same but with companion 180 mas away

  • 9

    Objectives of Fiber Nuller Set-up atPalomar 200”

    Technical goals:- Prove feasibility of the approach on the sky- Demonstrate detection of companion at the 500:1 level within100 mas of primary (e.g. composite spectrum stars)- Test TPF-I companion detection approach on the sky underfavorable conditions

    Science goals:- Stellar diameters, atmospheric layers, asymmetries (evolvedstars easily resolved)- Survey of hot material around mK

  • 10

    Palomar layout

    Palomar Layout

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    r

    Palomar 1st Engineering run (May 07)

    • Mounted FN bread-board in 200” Cassegrain cage,behind PALAO system

    • Injected starlight from both beams into K band SM fiber

    • Checked angle tracker (quad cells), photometriccalibration wheel and K photometer sensitivity (presentlylimited to mK=5 at constructive peak)

    • Under Jet Stream: strong winds, bad/fast seeing (~2”)made fiber injection unstable

  • 12

    Future Developments• November 07 engineering run goals:

    - Measure first nulls- Enable aperture rotation

    • Key upgrades (2008 = present limit of funding):- Low noise fast read IR camera- Enable fringe tracker to further decrease opd

    residuals left after AO (larger sub-apertures than AO)- Install refraction corrector- Use dispersion and spectral differential nulling- Use >2 sub-apertures (deeper central nulls, or try nulling + DP)

    • > 2008: Get to larger telescope at a prime astronomical site. Southhemisphere preferred to survey nearby young stars

    • Possible FN in space on a 1.5m vis/near IR astrometric telescope(Pravdo et al. 2007)

    Related presentations:

    • Talk by M. Shao (Tuesday 11:30 am):Visible nulling coronagraphy

    • Poster by G. Perrin et al. :Diffraction limited high dynamic range imaging from thevisible to the infrared

  • 13

    Back up slides

    Advantages

    • High contrast accessible without highStrehl (fiber corrects individual wavefronts)

    • Ultimate contrast fixed by rms of opticalpath difference over unit integration time:

    • N=1/4 (t2 + σ2φt) N=1e-3 readilyaccessible with 10ms sampling in K

  • 14

    Palomar layout

    Palomar Layout

  • 15

    Multi-axial Beam Combination

    • After densification, can adapt to the case fmany-sub-apertures:

  • 16

    Expected performance at Palomar