a new “radio era” for planet forming disks k. teramura uh ifa david j. wilner...
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![Page 1: A New “Radio Era” for Planet Forming Disks K. Teramura UH IfA David J. Wilner Harvard-Smithsonian Center for Astrophysics thanks to S. Andrews, C. Qi,](https://reader037.vdocuments.site/reader037/viewer/2022110209/56649e015503460f94aea959/html5/thumbnails/1.jpg)
A New “Radio Era” for Planet Forming Disks
K. Teramura UH IfA
David J. WilnerHarvard-Smithsonian Center for Astrophysics
thanks to S. Andrews, C. Qi, and many collaborators, www.cfa.harvard.edu/disks
SMA
ALMA
HIA, Victoria, March 2013
EVLA
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Stars Form with Protoplanetary Disks
Marois et al. 2010, Keck Observatory
McCaughren & O’Dell 1995
Silhouette Disks in Orion Nebula around ~1 Myr-old stars
planets orbiting HR 8799
How do disks evolve and form planetary systems?
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Relevance of Radio Astronomy
• low dust opacity mass, particle properties
• many spectral lines gas diagnostics, kinematics
• access cold material including disk mid-plane
• contrast with star planet-forming region
• low T, t low brightness imaging needs sensitivity
ALMA
EVLA
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1mm 1mm 1m 1km 1000km <1km
Planetesimal formation Planet formation
collisionalagglomoration
gravity-assistedgrowth
gascapture
radial driftfragmentation/
bouncing
Debris
From Dust to Planets
requires growth by 14 orders of magnitudes in size in a few Myr through several physical processes…
collisional destruction
collective
effects???
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Spectral Signatures of Grain Growth
• thermal dust emission Iν ∝ Bν(T) (1 - e-τν)
≈ ν2 T κν Σ Iν ∝ ν2+b
• index b is observable an diagnostic of the particle size distribution
b
amax =
1μm
1 mm
5 cm
1 m
Beckwith & Sargent 1991Miyake & Nakagawa 1993Draine 2006
see Draine 2006
ISM grains“pebbles”
2b
0
Rodmann et al 2006Ricci et al. 2010, 2011
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Disks@EVLA Key Project• PI Claire Chandler (NRAO) + 17 co-Is worldwide• grain growth and substructure in protoplanetary
disks• probe last observable link in chain from ISM dust
to planets- photometry of 60+ disks at 7/9/13/50 mm- imaging of subsets, some to 50 mas = few AUBirnstiel et al. 2010
95% confidence
Isella et al. 2010RY Tau: CARMA
• global b: weak model constraints- average level of grain growth only
• resolved colors, b(r), affected by- turbulence- particle collision model- materials- radial drift efficiency
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EVLA Taurus Disk Images
spectral indices
l = 9 mm (30.5 and 37.5 GHz)
θ ~ 0.7 arcsec = 100 AU
Chandler et al, in prep
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UZ Tau Resolved Millimeter Colors
• radiative transfer: tn(r)
• b(r) = d log tn(r) / d log n
amax ~ 10 cm (inner disk)
amax ~ 10 mm (outer disk)
radial drift limited growth?
• disk resolved at 0.9 -9 mm
100 AU
Harris et al. 2013, also Perez et al. 2012
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Isolating the Effects of Radial Drift
• thermal pressure: vgas < vKep
– small sizes: entrained by gas
– mid sizes: strong headwind– large sizes: drag is weakWeidenschilling 1977
• natural size-sorting of solids
• strong variation of gas:dust as a function of disk radius
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The TW Hya SystemH
ST
Weinberger et al. 2002
• closest gas-rich disk system (51 pc)– M = 0.6 M, age 3-10 Myr,
– southern, isolated, viewed nearly face-on
– many studies with SMA – good model of disk physical structure
Andrews et al. 2012
Qi et al. 2008
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Indirect Signature of Radial Drift1. RT model dust densities
2. assume constant gas:dust3. non-LTE model gas (CO)4. compare with data
Rosenfeld et al. 2013
Andrews et al. 2012
gas/dust size discrepancy
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Signatures of Grain Growth and Drift
• empirical dependence between dust disk extent and wavelength– emission becomes more compact at longer wavelengths
• power law index of opacity, b, decreases with disk radius– maximum particle size increases with disk radius
• CO gas disk extent much larger than millimeter dust disk– dust and gas surface density profiles are decoupled
observations naturally explained if growth and inward drift of solids concentrates large particles relative to molecular gas reservoir
• planet-disk interactions also make pressure bumps/particle traps
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Snow Lines and Planet Formation• “snow line” = boundary
where volatiles condense out of gas phase
• enhance planetesimal formation– dramatically increase available
solids– increase grain stickiness (icy
mantles)– influence bulk composition, e.g.
C/O
• key evaporation temperatures– H2O: 170 K (R = a few AU)
– CO: 20 K (R = a few 10’s of AU)
Hayashi 1981
Ciesla & Cuzzi 2006
Oberg et al. 2011
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• disks are 3D objects: “snow line” = “snow surface” – very difficult to discern in (optically thick) CO emission
• use chemical selectivity to advantage• N2H+ abundant only where CO highly depleted
– CO inhibits N2H+ formation
– CO speeds up N2H+ destruction
– CO freezes out at 20 K– observed in pre-stellar cores
CO Snow Line and N2H+ Chemistry
Qi et al. 2012
H3+ HCO+
N2H+
CO
N2
CO
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TW Hya SMA Obs ALMA Prediction
SMA N2H+
data
model
simulation
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TW Hya ALMA Cycle 0 N2H+ Imaging
• N2H+ shows a ring
• 2012 November 18• l = 0.8 mm (band 7)• 26 antennas, 2 hours• beam 0.6 x 0.6 arcsec • rms = 25 mJy (0.1 km/s)
>20x better sensitivity, >20x smaller beam area than SMA N2H+ obs
- rim radius (27 AU) matches prediction for CO snow line
- N2H+ abundant where T drops below 20 K
2011.0.00340.S PI Qi
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Planetesimal Belts in Debris Disks• sister stars in the 12 Myr-old b Pic Moving Group• surrounded by dusty disks, cleared of gas, viewed
edge-on
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b PicA6
19.4 pc
Rdisk > 800 AU
AU MicM1
9.9 pc
Rdisk > 200 AUKalas 2004
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Scattered Light Midplane Profiles
both disks show broken power-law profiles with similar slopes
Liu 2004
Golimowski et al. 2006
R-4R-1
b Pic break at R ~120 AUR-1
R-4
AU Mic break at R ~35 AU
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The “Birth Ring” Paradigm• a collisional ring of dust-producing planetesimals
– small grains blown out by stellar radiation (b Pic) and winds (AU Mic)
– large grains stay close to birth ring– size-dependent dust dynamics explains scattered light
profile
b = F*/Fgrav
Krivov 2010 (see Wyatt 2006)
Strubbe & Chiang 2006 (also see Augereau & Beust 2006)
scattered light
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SMA: 1.3 Millimeter Emission Belts
Wilner et al. 2011
b Pic
contours: ±2,4,6,8 x 0.6 mJy
Wilner et al. 2012
AU Mic
contours: ±2,4,6 x 0.4 mJy
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Emission Models and Belt Locations b Pic
R = 94±8 AUDR = 34+44 AU
F = 15±2 mJy
-32
AU Mic
R = 36+7 AUDR = 10+13 AU
F = 8.2±1.2 mJy
-16
-8
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MacGregor et al. 2013
AU Mic ALMA Cycle 0 Observations
>10x better sensitivity, >10x smaller beam area than SMA study
2011.0.00142.S PI Wilner2011.0.00274.S PI Ertel
• 4 SB executions in 2012 April and June
• l = 1.3 mm (band 6)• 16 to 20 antennas• beam 0.8 x 0.7 arcsec (8 x 7 AU)• rms = 30 μJy
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Millimeter Emission Model Fitting
contours: ±4,8,12,.. x 30 μJy
outer belt
+central peak
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AU Mic Outer Dust Belt Properties• extends to R=40 AU, to the break in scattered light
profile– consistent with model based on size-dependent dust
dynamics
• appears sharply truncated– reminiscent of the classical Kuiper Belt– initial condition? or result of dynamical interaction?
• surface density profile rises with radius, S(r) ~ r2.8 – collisional depletion of inner disk by ongoing planet
formation?
• no detectable asymmetries in structure or position– no significant clumps, e.g. due to resonances with orbiting
planet– centroid offset limit compatible with presence of Uranus-like
planet
Kennedy and Wyatt 2010
Mustill and Wyatt 2009
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AU Mic Central Peak Emission
• stellar photosphere and additional unresolved emission– measure 320 mJy in central component– a NextGen stellar model (3720 K, 0.11 L 0.6 M) 52 mJy
• stellar flares? – no detectable variability, hours to months
• stellar corona? – low radio flux density limits in quiescence from VLA (in early
1990s)– requires turnover frequency > 40 GHz, or time evolution – would be detectable by EVLA at centimeter wavelengths
• asteroid-like belt at a few AU?– compatible with absence of excess emission < 25 μm– would be easy for ALMA to resolve in future Cycles
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A new “Radio Era” for Disk Studies• planets form in circumstellar disks• major unknown is
distribution/evolution of cold dust and gas at Solar System scales: key observables for ALMA and EVLA
• entering a new regime of decoupled gas and dust, size-dependent dust dynamics
• three examples- resolving grain growth and drift - imaging snow lines- revealing planetesimal belts• expect surprises!
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END
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Next Generation Radio Telescopes
• 66 moveable 12m/7m antennas 5000 m site in northern Chile l = 300 mm to 7 mm
• global collaboration (NA, EU, EA) to fund >$1B construction
• 27 moveable 25 m antennas 2000 m site in New Mexico l = 7 mm to 4 m
• modern electronics and signal processing, c. 1980 infrastructure
Atacama Large Millimeter Array Expanded Very Large Array
10-100x better sensitivity, spectral capabilities, resolution
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Planet-Disk Interactions• viscous/tidal
interactions make waves
• consequences– open a gap– create pressure
bumps – planet migrationGoldreich & Tremaine 1980; e.g., Bryden et al 1999
Andrews et al 2011aMathews et al 2012 Brown et al 2008 Hughes et al 2009 Andrews et al 2011a
Andrews et al 2011b
Andrews et al 2009
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Transition Disk Issues • mass flow across gap
– gas: regulated by Mp + viscosity
– dust: size-dependent filtration
• particle trapping (and growth)– location of ring vs. planet orbit– azimuthal asymmetries
Lubow and D’Angelo 2006, Zhu et al. 2012, Dong et al. 2012
Pinilla et al. 2012, Birnstiel et al. 2013
ALMA Cycle 0 HD142527
Casassus et al. 2013
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A New “Radio Era” for Planet Forming Disks
K. Teramura UH IfA
David J. WilnerHarvard-Smithsonian Center for Astrophysics
thanks to S. Andrews, C. Qi, and many collaborators, www.cfa.harvard.edu/disks
SMA
ALMA
HIA, Victoria, March 2013
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Planetary Systems Form from Disks
Marois et al. 2010, Keck Observatory
McCaughren & O’Dell 1995
Silhouette Disks in Orion Nebula around ~1 Myr-old stars
planets orbiting HR 8799