ALMA Observations of the Disk Wind Source AS 205

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ALMA Observations of the Disk Wind Source AS 205 Keck/VLT ALMA 8 April 2013 Geoffrey A. Blake, Division of GPS, Caltech Transformational Science with ALMA: From Dust to Rocks to Planets

Folks doing the work: Colette Salyk, Goldberg Fellow, NOAO, Tucson Klaus Pontoppidan, Hubble Fellow, STScI Ke (Coco) Zhang, PMA Graduate Student (TW Hya snowline, 2013 ApJ 766, 100) Joanna Brown, SMA Fellow, CfA & the Leiden/Garching teams, especially Jeanette Bast and, of course, Ewine van Dishoeck.

Laplace 1796 What can the solar system tell us about The formation & evolution of planetary systems? Key insights: 1. Most of the mass is in the sun. 2. The major planets all orbit in the same sense. 3. Small bodies, especially comets, are very different (eccentric, not in one plane).

Angular momentum is key. How best to study disks? HH 30 G.J. van Zadelhoff (2002) ç Hotter Colder è Chiang & Goldreich (1997) IR disk surface within several 0.1 several tens of AU. (sub)mm disk surface at large radii, disk interior also. Need high spatial resolution to break model degeneracies.

The photospheres of stars & disks tell us what they are made of The Astronomer s Periodic Table H [O,C] ~10-4 [H] [N] ~10-5 [H] [Si,Fe]~10-6 [H] O C H, H 2, He very hard to see. Dust+Ice/Gas~1% He N Si Fe All Else and serve as beacons for exoplanet searches.

Arrays esp. critical at long wavelengths. ALMA? Gas in TW Hya (SV Data) Once completed, ALMA should be able to detect 1 AU wide gaps in its largest configurations via dust imaging, but for 3 AU pixels at 140 pc, VV Ser 1 km/s in CO 3-2 = 100 K rms in 8 hr Very difficult to see lines at <5 AU, does the grain emissivity change with radius? Wolf et al. 2002, ApJ 566, L97.

How can we test disk models with gas tracers @ 0.1-1 AU resolution? Even w/alma, the Theory size scales are too small even for the largest mm-wave arrays. Look where the inner disk is self-luminous, or, IR spectroscopy to the rescue Jupiter (5 AU): V doppler = 13 m/s V orbit = 13 km/s Observation?

Disk Photospheres: CO Line Width Trends inclination AB Aur Objects thought to be ~face on have the narrowest lines, highly inclined YSOs the largest. As the excitation energy increases, so does the line width (small effect). Consistent with disk emission, radii range from 0.5-5 AU. Low J lines also resonantly scatter 5 µm VV photons Ser to much larger distances. Asymmetries (VV Ser)? Blake & Boogert 2004, ApJL 606, L73, Herbig Ae stars (above) Najita et al. 2003, ApJ 589, 931 for clasical T Tauri stars

Spectro-Astrometry of Disks with CRIRES, NIRSPEC: IRS 48 Brown et al. (2012) T(CO)~650-700 K AO-fed echelle <200 µas Spectroastrometry @ 3 km/s! K. Pontoppidan et al. (2008)

CO Emission from Transitional Disks? S-A. SR 21 HD LkHα 135344B 330 Directly gives emitting radii (typically a few AU), but cannot sense the disk beyond >10 AU (need ALMA). Better than 0.1 AU precision for both Keck and the VLT. CARMA K. Pontoppidan et al. (2008)

Some confusing results: Many ctts show classic Keplerian line shapes and spectro-astrometric signatures, but Some profiles are single peaked even at 3 km/s (Bast et al 2011).

Likely answer? Not just a disk! Pontoppidan et al. (2011) Need a slow, wide angle, molecular wind. Does this gas escape or re-impact on disk (comets)?

What are the properties & fate of this molecular wind? Enter ALMA. AS 205 Two Cycle 0 sessions, 31 min. total. CO/ 13 CO/C 18 O 2-1. Binary well resolved, all lines nicely detected.

What are the properties & fate of this molecular wind? Enter ALMA. AS 205 Andrews et al. (2009), 12 CO 3-2, see also Oberg et al. (2011). 13 CO 2-1 yields a compact velocity pattern around AS 205A that is consistent w/keplerian rotation.

What are the properties & fate of this molecular wind? Enter ALMA. AS 205 CO 2-1 clearly more extended than 13 CO/C 18 O, patterns not consistent w/a Keplerian field, and as w/some other disks (esp. TW Hya), the gas/dust ratio must increase at large R.

Is there a disk wind in AS 205? Some thoughts. SR 21 13CO 2-1 Gas readily seen @ <0. 5 in disks w/alma. 13CO Keplerian, but 12CO asymmetric. Comp? Another component? Different gas/dust? To constrain this component, ALMA data on several CO transitions/isotopologues needed. Are breaks in the gas/dust ratios in disks signatures of disk winds? Could the remnant envelopes seen around older stars be, in fact, remnant disk winds? Might help explain ISO H2 detections.

At early times, does water aid grain growth? Do small grains remain lofted, ~mm/cm bodies settle quickly? That is, do we get: to accelerate planetesimal growth? If so, the radial location of the snow line is critical!

How does spectro-astrometry work? Relative astrometry measures the centroid of a point source image (ΔX, ΔY). In long-slit spectra (far right), there is only one spatial centroid, ΔX(n, PA), that is measured for each frequency, slit PA. ΔX(n, PA) can be determined to much better precision than the formal PSF width (~100 times better). DY DX n