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VSI / MATISSE
Sebastian WolfUniversity of Kiel, Germany
Circumstellar Disks and Planets – Science cases for the second generation VLTI instrumentation26-28 May, 2010 - University of Kiel
Perfect combination of observing wavelength (~10µm) and spatial resolution (VLTI baselines 10-20mas)
regions with hot dust can be spatially resolved
since 2002observations of the hot dust in circumstellar disks, AGB stars,
winds of hot stars, massive star forming regions, tori of AGNs, debris disks, solar system objects
Results:Very successful in interferometric spectroscopy(chemical composition of dust on different spatial scales)
Concept of mid-infrared long-baseline interferometry proven to work
but …
MATISSE[The Progenitor: MIDI]
MIDI
a) Small number of visibility pointsb) Lack of Phase Information
Investigation of small-scale structures (= main goal of MIDI) and quantitative analysis of spectroscopic observation strongly limited
c) Interpretation of MIDI data:Comparison between modeled and observed visibility points,
using 2D models with point-symmetry (usually even rotation symmetry)
Approach justified only by large-scale (if at all existing) symmetries, but expected to be strongly misleading or simply wrong
on size scales investigated with MIDI
MATISSE[MIDI’s limitations]
MIDI
[MIDI] Mid-IR Interferometry
Schegerer, Wolf, et al., 478, 779, 2008, „The T Tauri star RY Tauri as a case study of the inner regions of circumstellar dust disks “
Schegerer, Wolf, et al. 2009, A&A, 502, 367 „Tracing the potential planet-forming region around seven pre-main sequence stars“
Mid-Infrared Interferometric Instrument (MIDI)
Spatial resolution: λ/B ≥ 1AU @ 140pc with B ≤ 130m
Spectrally resolved (R=30) data in N band:• Silicate feature + (relative) radial distribution• Inner disk region ≤ 40 AU
General results(1) SED (global appearance of the disk) + spectrally
resolved visibilities can be fitted simultaneously(2) Best-fit achieved in most cases with
an active accretion disk and/or envelope(3) Decompositional analysis of the 10µm feature
confirms effect of Silicate Annealing in the inner disk (~ few AU)
Limitation of 2-beam interferometers[Example]
True surface brightness profile in circumstellar disks around TTauri / HAe/Be stars
Two-telescope interferometers: “mean” disk size & approximate inclination of the diskAssumption: Iso-brightness contours are centered on the location of the central star
Simulated 10μm intensity map of the inner 30AU×30AU region of a circumstellar T Tauri disk at an assumed distance of 140 pc; inclination angle: 60◦.
Left: VISIR false-color image of the emission from the circumstellar material surrounding the HAe star HD97048. The emission is widely extended, as compared with the point spread function (inset) obtained from the observation of a pointlike reference star. Right: Same image as in the middle, but with a cut at the brightness level and a fit of the edge of the image by an ellipse (Lagage et al. 2006).
Goal: Thermal reemission images with an angular resolution of 0.003“
MATISSE @ Very Large Telescope Interferometer
Multi-AperTure Mid-Infrared SpectroScopic Experiment
2nd generation VLTI beam combiner• L, M, N bands: ~ 2.7 – 13 µm• Improved spectroscopic capabilities:
Spectral resolution: 30 / 100-300 / 500-1000• Simultaneous observations in 2 spectral bands
MATISSE
Successor of MIDI:Imaging capability in the entire mid-IR accessible from the ground
Extension to AMBER / VSI:Extension down to 2.7µm + General use of closure phases
Complement to ALMA + TMT/E-ELT
Ground Precursor of DARWINWavelength range 6-18µm
Multi-AperTure Mid-Infrared SpectroScopic Experiment
High-Resolution Multi-Band Image Reconstruction+ Spectroscopy in the Mid-IR
MATISSE[overview]
Key features
• Imaging in N band
(general use of closure phases)
• L&M band extension
(simultaneous observations in L&M and N band)
Science Cases for MATISSE
1. Star and Planet Formation
2. Evolved Stars
3. Solar System Minor Bodies
4. Extrasolar Planets
5. Active Galactic Nuclei
6. Galactic Center
MATISSE[requirements / observing strategy]
Requirements: Spectroscopic Resolution
Number of Combined Beams
2/3 T Mode : Highest sensitivity measurements; Preparatory studies
4 T Mode : Image reconstruction and Model fitting studies
Observing Strategies
a) Image reconstruction mode (3-5 nights)
b) Model fitting mode (single measurements)
~
MATISSE[ATs / UTs]
ATs
Goal Image reconstruction
Requirement Optimized coverage of the u-v plane
Consequence Majority of key science programmes must be executable using the relocatable Auxilliary Telescopes (ATs)
UTsRequired to reach the sensitivity limits demanded by selected science programmes
(e.g. AGNs)
Size ScalesSolar System
Angular diameter of the orbits of selected Solar System planets as seen from the distance of the nearby star-forming region in Taurus (140pc) :
Neptune - 0.43” Jupiter - 0.074”Earth - 0.014”
What is possible? – TODAY
AMBER / VLTI ~ a few mas [near-IR]MIDI / VLTI ~ 10 – 20 mas [N band: ~8-13µm]SMA ~ 0.3” (goal: 0.1”) [~submm]
Size scales
IRAS 04302+2247 „Butterfly Star“
Size ScalesSolar System
Angular diameter of the orbits of selected Solar System planets as seen from the distance of the nearby star-forming region in Taurus (140pc) :
Neptune - 0.43” Jupiter - 0.074”Earth - 0.014”
What is possible? – WITHIN THE NEXT DECADE (examples)
VSI / VLTI ~ a few mas [near-IR]MATISSE / VLTI ~ 3 – 20 mas [L/M/N bands: ~3-13µm]ALMA ~ 20 mas [~submm]
Size scales
IRAS 04302+2247 „Butterfly Star“
4-6 telescopes;image reconstruction
AB Aurigae
Spiral arm structure: H band(Herbig Ae star; Fukagawa et al. 2004; SUBARU)
Distance: ~140 pc
MATISSE[Exemplary science case]
Low/Intermediate mass star formationPlanet formation
Complex outer disk structure observed
Complex inner disk structure expected
FU Ori outbursts -- Variability in general (flux, polarization),
Expected influence from the formation of Jets/Outflows
AB AurigaeAsymmetry (Color: 24.5µm, Contours: H Band)
(Herbig Ae star; Fujiwara et al., 2006, SUBARU)
Distance: ~140 pc
Complex outer disk structure observed
Complex inner disk structure expected
FU Ori outbursts -- Variability in general (flux, polarization),
Expected influence from the formation of Jets/Outflows
MATISSE[Exemplary science case]
Low/Intermediate mass star formationPlanet formation
AB AurigaeSpiral (345 GHz, continuum)
(Herbig Ae star; Lin et al., 2006, SMA)
Distance: ~140 pc
MATISSE[Exemplary science case]
Low/Intermediate mass star formationPlanet formation
Complex outer disk structure observed
Complex inner disk structure expected
FU Ori outbursts -- Variability in general (flux, polarization),
Expected influence from the formation of Jets/Outflows
Example #1 HH30
[Guilloteau et al. 2008]
Observation• IRAM interferometer, 1.3mm, beam size ∼0.4”
Result• Disk of HH30 is truncated at an inner radius of 37 ± 4 AU
Interpretation• Tidally truncated disk surrounding a binary system (two stars on a low eccentricity, 15 AU semi-major axis orbit)
• Additional support for this interpretation: Jet wiggling due to orbital motion
• The dust opacity index, β ≈ 0.4, indicates the presence of cm size grains (assuming that the disk is optically thin at 1.3mm)
Example #2 Disk in the Bok Globule CB26
[Sauter et al., 2009]
Observations considered
• HST NICMOS NIR imaging• (Sub)mm single-dish: SCUBA/JCMT, IRAM 30m• Interferometric mm cont. maps:SMA (1.1mm), OVRO (1.3/2.7mm)• SED, including IRAS, ISO, Spitzer
Inner disk radius: ~ 45 AU
constraints on radial + vertical disk structure in the potential planet-forming region (r~80-120AU)
1360µm
894µm
[Wolf et al. 2008]
Example #3 The Butterfly Star in Taurus
Example #4 Face-on disks
• AB Aurigae (Lin et al. 2006)Emission gap observed in gas and dust distribution
• GM Aurigae (Dutrey et al. 2008)Inner disk radius: 19 +/-4 AU
Example #4 Face-on disks
340 GHz dust continuum images of LkHα 330 (top), SR 21N (middle), and HD 135344B (bottom).The crosses mark the literature coordinates of the central star.
[Brown et al. 2009]
rin=27AUrin=37AU rin=40AU
MATISSEDisk clearing
10µm image of a circumstellar disk with an inner hole; radius 4AU (inclination: 60°; distance 140pc;
inner 60AU x 60AU)
Sublimation radius ~ 0.1-1AU (TTauri HAe/Be stars)
but:
Observations: Significant dust depletion >> Sublimation Radii
TW Hydrae : ~ 4 AU (Calvet et al. 2002)
GM Aur : ~ 4 AU (Rice et al. 2003)
CoKu Tau/4 : ~10 AU (D’Alessio et al. 2005, Quillen et al. 2004)
[ MATISSE Science Cases ]
Planetary signatures in the near-IR?
Artist impression of the disk around LRLL 31. A planet in the innermost regioninfluences the disk to cast a large shadow on the outer region. The orbit of theplanet, and thus the shadow, causes the disk to be variable in the nearinfrared on timescales on the order of one week. Picture credits: NASA.
ObservationVariability of T Tauri stars
on time scales < 1 year
Various interpretations• Clumpy inner circumstellar shell/disk structure
• Variable stellar accretion rate⇒ variable net luminosity⇒ variable inner disk structure / disk illumination
• Embedded stellar or planetary companion => dynamical perturbation (short-term)
Example Transitional disk LRLL 31 in the 2-3Myr old star-forming region IC 348: Variations of the near-IR and N band spectra on a few months timescale[Muzerolle et al. 2009]
Observational basis: Spitzer/IRS 5-40µm observations, 6 months (Houck et al. 2004); further Spitzer/MIPS observations (Muzerolle et al. 2009) + SpeX/IRTF, SPOL (Spectro-polarimeter; Steward observatory) spectroscopic measurements
ALMA: Gaps
Jupiter in a 0.05 Msun disk
arounda solar-mass star
as seen with ALMA
[ Wolf et al. 2002 ]
d=140pc
Baseline: 10km
λ=700µm, tint=4h
Planetary Accretion Region
[ D’Angelo et al. 2002 ]
[ Wolf & D’Angelo 2005 ]
Density Structure
Stellar heating
Planetary heating
Prediction of Observation
Proc
edur
e
Close-up view: Planetary Region[ Wolf & D’Angelo 2005 ]
Maximum baseline: 10km, 900GHz, tint=8h
Mplanet / Mstar = 1MJup / 0.5 Msun
Orbital radius: 5 AUDisk mass as in the circumstellar disk around the Butterfly Star in Taurus
50 pc
100 pc
Random pointing error during the observation: (max. 0.6”);Amplitude error, “Anomalous” refraction;
Continuous observations centered on the meridian transit;Zenith (opacity: 0.15); 30o phase noise;
Bandwidth: 8 GHz
Influence on SED?
[ Wolf & D’Angelo 2005 ]
Planet
Planetary Environment
Inner Disk Planetary radiation significantly affects the dust reemission SED only in the near to mid-infrared wavelength range.
This spectral region is influenced also by the warm upper layers of the disk, the inner disk structure, and the planetary contribution.
Planetary Contribution / Disk reemission (within the inner 12 AU ~ 0.1” in Taurus) < 0.4%
(depending on the particular model)
The presence of a planet + its basic characteristics (temperature, luminosity)
cannot be derived from the SED of the disk alone.
Complementary Observations: Mid-IR
Hot Accretion Region
around the Planet
inclination: 0° inclination: 60°
10µm surface brightness profile of a T Tauri disk with an embedded planet
(inner 40AUx40AU, distance: 140pc)
[ Wolf et al. 2007 ]
Shocks & MRI
Strong spiral shocks near the planet are able to decouple the larger
particles (>0.1mm) from the gas
Formation of an annular gap in the dust, even if there is no gap
in the gas density.
(PaardeKooper & Mellema 2004)
MHD simulations - Magnetorotational instability
• gaps are shallower and asymmetrically wider
• rate of gap formation is slowed
Observations of gaps will allow to constrain the physical
conditions in circumstellar disksLog Density in MHD simulations after 100 planet orbits for planets with relative masses of q=1x10-3 and 5x10-3 (Winters et al. 2003)
Gas Dust
Shadow – Astrometry
Conditions for the occurrence of a significantly large / strong shadow still have to be investigated
[ Wolf & Klahr, in prep.]
Space Interferometry Mission (SIM)
Wavelength range0.4-0.9µm
Baseline: 10m
Narrow Angle Field: 1°
Narrow Angle Astrometry1µas mission accuracy
StrategyCenter of Light Wobble
[ G. Bryden, priv. comm.]
K band, scattered light
5 AU
Giant Planets in Debris Disks
• Decreased Mid-Infrared SED
[ Rodmann & Wolf ]
Planet Resonances and gravitational scattering
Asymmetric resonant dust belt with one or more clumps, intermittent with one or a few off-center cavities
+
Central cavity void of dust.
• Resonance Structures: Indicators of Planets
[1] Location
[2] Major orbital parameters
[3] Mass of the planet
[ Wolf & Hillenbrand 2003, 2005 ]
www1.astrophysik.uni-kiel.de / dds
Scattered Light Image
Young binaries
Binaries are the rule and not the exception• Nearby solar-type main-sequence stars show that about 53% of the stars are binary or multiple
systems• Taurus-Auriga star forming region: 80-100% (Ghez et al. 1993; Leinert et al. 1993; Reipurth &
Zinnecker 1993)
Science Cases• Gap between the close binaries detected by spectroscopic measurements and the companions at
larger separations detected on single dish telescopes by imaging with adaptive optics or by speckle interferometryMATISSE: Can close the gap
• Dynamical mass determination: Calibration of pre-main sequence evolutionary models• Characterization of infrared companions• Evolution of young binary systems
(Note: binary /= two independent stars)• Circumbinary disks: Structure, Alignment
The ‘miniclusters’ UZ Tau (the sources are separated by 0.4 and 3.6 arcsec) as seen in the Ks band with
NAOS/CONICA at the VLT.
High-mass star forming regions are much more distant (in average)than those of low-mass stars (high-mass: 3-7kpc vs. low-mass: 0.1-0.3 kpc)
JHK composite of NGC 3603 from ISAAC data, dimension 25'' x 25''
OB stars- form preferentially in the centre of dense star clusters- seem to live pref. in (tight) binary and higher order systems
The Orion BN/KL region at 12.5µm,dimension 10'' x 10'' (distance 450 pc)
[Shuping et al. 2004]
High number density of objects
Enhanced outflow activity
Strong stellar winds from the massive stars after ignition
Massive Star Formation
Observations in different bands
• … trace regions with different characteristic temperatures / physics / chemistry
• … provide image with different spatial resolution
• … allow a comparison with lower-resolution images obtained at large telescopes with adaptive optics – tracing the large scale structure of the targets – in different wavelength regions (L/M: NACO, N: VISIR)
L M N
Multi-wavelength imaging
Depending on the individual band
• … unique spectral features (dust/gas) are accessible
• … spectral features can be investigated that correspond to dust species which can also be observed in N band
L band
• H2O ice broad band feature (2.7-4.0µm)
• PAHs: 3.3µm, 3.4µm
• Nanodiamonds: 3.52µm
• Highest Sensitivity in the MIR (reduced background emission)
M band
• CO fundamental transition series (4.6-4.78µm)
• CO ice features (4.6-4.7µm)
• Recombination lines, (e.g., Pfβ at 4.65µm)
Spectroscopy[Gas]
Prominent gas/dust features
Dust / Gas spectroscopy: Applications
• Mineralogy of proto-planetary disks– Dust grain coagulation– Modification in innermost (hottest) disk regions (silicate annealing), Radial mixing
• Environment of massive stars– Spatial distribution of CO, H2O ice– CO absorption lines: Distribution of warm / cold gas– Pfund β and Br α emission lines (?): Disk kinematics
M–band spectrum of the massive star forming region W33A (taken from Pendleton et al. 1999) as a compelling example for the occurrence of the 4.62 μm feature commonly attributed to OCN−.
Note: While this solid state feature is present toward several massive YSOs, W33A is an extreme example where it attains an even larger optical depth than the neighbouring CO ice feature at 4.67 μm.
FWHM(W33A) @ 8µm: 30mas [Wit et al. 2007]
MATISSE in the context of Star and Planet formation
Star and Planet FormationLow-mass Star and Planet FormationMineralogy of proto-planetary disks, dust grain growth and sedimentationTransitional objects: Status of inner disk clearingNature of outbursting young stellar objectsBinary mode of star formation: Inner structure and conditions for planet formation in circumbinary vs. circumstellar disks. Disk alignment.Characteristic structures in disks: Tracing giant proto-planets
Late stage of planet formation - Debris disksPlanetesimal collisions and exo-comets evaporation, grain properties and disk geometry.Complex spatial inner disk structure – direct indicators for the presence of planetsCharacterization of Darwin/TPF targets
Massive Star Formation: Link between low and high-mass star formation?Search and characterization of accretion disks around young massive (proto)starsSpatial distribution of the gas (carbon monoxide and hydrogen) and dust (silicates/graphite and CO ice) in the typically complex and distant high-mass star-forming regions
Summary
Phase-referenced imaging
Phase-referenced imaging allows one to reconstruct
∼ 4× fainter targets than closure-phase imagingPhase-referenced imaging can yield acceptable reconstructions of the T Tauri disk (∼ 90 masdiameter) down to a flux of 5.7 Jy (restoration error ∼ 21%), and closure-phase imaging can yield acceptable reconstructions down to a flux of 19.7 Jy (restoration error ∼ 15%).
∼ 1.5−2× larger targets than closure phase imaging.Reconstruction of T Tauri disks (average SNR ≈ 20 of the squared visibility) up to diameters of 180-210 mas (restoration errors ∼ 28-42%), and closure-phase imaging can reconstruct disks up to a diameter of 120 mas (restoration errors ∼ 16%).
VSI: VLTI Spectro-Imager
Second generation general purpose VLTI instrument
Near infrared• Immediate access to emission/absorption lines that probe the gas in a wide variety of conditions
and chemical states• Sublimation temperatures of dust peaks in the NIR
Full use of existing infrastructure• Eight telescopes and six delay lines are currently installed at Paranal • Use of 4T at a time can provide excellent science, but the full use of the existing infrastructure is
the key to maintain VLTI as the top optical interferometric facility in the world.
Complementarity• Imaging capabilities / High angular resolution:
Highly complementary to both the AO imaging instrumentation available at the VLT but also to ALMA imaging
• Spectral resolutions: considerable overlap with existing VLT instrumentation (which have much coarser angular resolution)
• Complementary to MATISSE: Probes the inner dust sublimation surface as well as the gas motions, while MATISSE probes the outer “colder” dust
VSI: VLTI Spectro-Imager
Instrument design:
ImagingYoung star disks and winds; Evolved stars; Stellar surfaces; AGN torus.
High dynamic range imagingDebris disks.
Parametric visibilitiesBinaries, AGN BLRs and massive black holes.
High dynamic range parametric visibilitiesExtrasolar planets.
PRIMA operationAdditional science in AGN torus, BLR and massive-black holes
Target of opportunity + PRIMAMicrolensing (additional science)
VSI: VLTI Spectro-Imager
Scientific requirementsSpectroscopic requirements. lowest resolution: 20 … 100.. intermediate spectral resolution: 1500–2500. high spectral resolution: 12000.
. lower scientific priority: mode with spectral resolution of 5000 is recommended.
. On average the spectral position of each pixel should be determined with an error no lessthan 0.20 of the pixel wavelength width
. lowest boundary of accessible instrument wavelengths: 1.08 μm.
. accessible J band in intermediate spectral resolution: at least 1.08 μm as its lower limit.
. K band accessible to the instrument should range from 1.95 μm to 2.37 μm; ideally upto 2.40 μm.
. spectral bands (J, H or K) does not necessarily have to be observed simultaneously.
VSI: VLTI Spectro-Imager
Scientific requirementsFringe tracker requirements
. A fringe tracker is required for the science case.The fringe tracker can operate at a different band than the science channel, except for the Kband. A mode where part (exact amount TBD) of the K band light is used to fringe trackand part to do science should be available.
. The fringe tracker design should be driven by sensitivity.
. Interesting additional science would be allowed if the fringe tracker could fringe track onone of PRIMA’s dual beams, the other being reserved for the science channel.
VSI: VLTI Spectro-Imager
Scientific requirementsImaging requirements
. Telescope positions should remain fixed during the night.
. An imaging mode where three different combinations of four telescopes (3 x 4T) are availablewithin a time-span of weeks, is required.
. An imaging mode where the simultaneous combination of six telescopes (6T) is available in asingle night, would open new and unique science.
PRIMAThe star separator systems and differential delay lines of PRIMA allows off-axis fringe tracking
VSI: VLTI Spectro-Imager
Selected science casesYoung disks• Physical properties of the inner disk, Structure of gas / dust disk• Inner rim structure• Presence of planetary companion
• Disk census in star-forming regions
• Time-dependent phenomena:– VSI angular resolution of 1 mas => keplerian radius of 0.15 AU at 150 pc => keplerian period:
11.5 days => Disk evolution on timescales of weeks.
Complementary observations:Sub-mm interferometers (PdBI, ALMA): Cold, outer disk regions; different dust properties and different emission linesMATISSE:Obtaining images of protoplanetary disks at multiple infrared wavelengths will enable a global picture of these objects
VSI: VLTI Spectro-Imager
Reconstructed images: Case studies:[1] YSOs
3x4T [MIRA reconstruction]
1x6T [MIRA reconstruction]
VSI: VLTI Spectro-Imager
Reconstructed images: Case studies:[1] YSOs
3x4T [BSMEM reconstruction]
1x6T [BSMEM reconstruction]
VSI: VLTI Spectro-Imager
Selected science casesMultiplicity of young stars
Is the frequency of companions within 5AU of YSOs consistent with that observed amongnearby field stars or substantially higher, as for wider systems?
Among multiple systems, what is the frequency of quadruple and high-order systems and dothey show evidence of past dynamical re-arragements?
Are there some significant trends regarding this restricted multiplicity rate as a function ofstellar mass, age and/or environment?
Can the physics of core fragmentation and/or subsequent internal rearrangements account forthese differences? Alternatively, do these companions form through a distinct mechanism?
VSI: VLTI Spectro-Imager
Selected science casesExoplanets
Observation of hot Jupiters in J, H and K bands, with a low (R ~100) or medium (R ~1000) resolution.
Model fitting of low-resolution spectra => of their albedo and test the cloud-free assumption
Phase dependence of the measured signal shall constrain the heat redistribution (through the temperature across the surface) and the weather conditions.
At medium resolution: Measurement of the abundance of CO, testing of the presence of CH4
Approach: Differential closure phases:Hot Jupiters are very close to their parent star:In the wavelength domain of VSI, common hot Jupiters have a typical contrast of 10−4 and the best
targets reach a contrast of 10−3
Reconstructed images: Case studies:[3] Microlensing
VSI: VLTI Spectro-Imager1x6T(?) [MIRA reconstruction]
1x6T(?) [BSMEM reconstruction]
VSI: VLTI Spectro-Imager
Selected science casesDebris disks
Inner disk structure => indicative for embedded planets (planet/disk interaction)
Large survey to detect the presence of close-in dust down to a meaningful density level and derive statistics for this phenomenon
• Occurrence rate as a function of various stellar parameters. These mainly include age and spectral type, but also metallicity. Further parameters could be added to the list. One could investigate, for example, correlation with stellar rotation, which is closely related to the angular momentum budget of planetary systems
• Possible correlation with the presence of cold excesses. Statistical information on excesses across the spectrum — from near-IR (VSI) to sub-mm (SCUBA/SCUBA2) would allow one to better constrain the overall spatial distribution of dust material in the systems
• Possible correlation with the known (RV) giant planets, as done for outer discs.
VSI: VLTI Spectro-Imager
Reconstructed images: Case studies:[2] Debris disks
1x6T [MIRA reconstruction]
1x6T [BSMEM reconstruction]
Remark: High dynamic range requirements=> only the 6 AT × 1 night configuration was explored