Ge/Ay133

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Ge/Ay133 ED studies of disk “lifetimes” & Long wavelength studies of disks

description

SED studies of disk “lifetimes” & Long wavelength studies of disks. Ge/Ay133. IR disk surface within several 0.1 – several tens of AU (sub)mm disk surface at large radii, disk interior. Details next!. Characterizing large disk samples? SED Models:. - PowerPoint PPT Presentation

Transcript of Ge/Ay133

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Ge/Ay133

SED studies of disk “lifetimes” & Long wavelength studies of disks

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Characterizing large disk samples? SED Models:

IR disk surface within several 0.1 – several tens of AU(sub)mm disk surface at large radii, disk interior. Details next!

G.J. vanZadelhoff2002

Chiang &Goldreich 1997

HH 30

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Use SED surveys to probe disk evolution w/time, accretion rate, etc.

Find very few objects with moderate IR excesses, most disk systems are optically thick out to 24 m.

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Disk Fraction Correlations

Cieza et al. 2006

For wTTs sample projected on clouds, disk fraction increases with H Equivalent Width (EW), declines with age.

wTTs

cTTs

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Disk Timescales

Some wTTs do have disks, not seen before w/IRAS.But, only the young ones (age < 3 to 6 MYr)The ages are uncertain due to models, but ~half the young wTTs lack disks (even at 0.8 to 1.5 Myr).Thus, time is NOT the only variable. How might disks evolve?

Padgett et al., 2006; Cieza et al., 2006

Big RED circle: has disk

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Class III

That is, are there multiple paths from optically thick to optically thin disks?

Class II Star

Disk

Class II

Class II

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Mapping evolutionary paths?

• Evolutionary sequence: cTTs wTTs Debris

is theslope ofthe IRexcess,t-o wherethe starand diskcontributeequally tothe SED.

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Statistically, how long do dust grains in disks “survive”?

Basic result: Disks dissipate within a few Myr, but with a large disp. for any SINGLE system. When they go, however, the dissipation is FAST in comparison w/ disk “lifetime.”

Gas???

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With modern mm-detectors, can sense beyond SED “knee”:

Can this long wavelength photometry help us understand disk evolution and dissipation? (Images later)

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)( )( rrTRr do Measure, must know distance.

derive

AssumeUNLESS thedisk is spatiallyresolved.

Disk modeling of (sub)mm-wave flux measurements:

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optically thin, near peak of blackbody:

optically thin, R-J limit

0

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For “typical” assumptions, what do you find?

Current studies are flux limited at ~10 mJy:

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Submm Continuum Imaging – TW Hya

• The SMA continuum measurements agree well with the predictions of the physically self-consistent irradiated accretion disk model for TW Hya (Calvet et al. 2002)

• The radial brightness distribution of the disk observed at 345 GHz is also consistent with the Calvet model.

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So, we CAN measure many disk parameters, but only for a handful of sources for now. Use these results to guide continuum surveys:

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Only substantial correlation is with overall SED and/or accretion rate indicators, otherwise LARGE scatter!

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Other “factoids”:

Submm flux highly correlated with the presence or absence of IR excess. Almost no disks w/weak IR but strong submm.

Very little dependence of MAXIMUM disk mass on age (that is, some fairly OLD stars have >MMSN disks).

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Other “factoids”:

Submm flux highly correlated with the presence or absence of IR excess. Almost no disks w/weak IR but strong submm.

Very little dependence of MAXIMUM disk mass on age (that is, some fairly OLD stars have >MMSN disks).

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Gas? CO/Good Dynamical, T Tracer

M. Simon et al. 2001, PdBI

The CO line shape isSensitive to:Rdisk ,Mstar, Inc.

These can bemeasured w/resolved images:

Dent et al. 2005, JCMT

vLSR (km/s)

TM

B (K

)

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CO 3-2

With multiple CO lines T gradients:

Qi et al. 2004, ApJ 616, L7.TW Hya w/SMA

M.R. Hogerheijde code

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13CO 2-1/TW HyaData

Model (Rout 110 AU)

Model (Rout 172 AU)

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Blue: Canonical Model (Calvet et al. 2002, Qi et al. 2004 )Black: SMA data

CO 2-1 CO 3-2Temperature Contour

Tau=1 Surfaces

CO 3-2CO 2-1

Only sensitive to disk surface layers, hard to get mass.

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Calvet et al. 2005, ApJ, 630, L185

Also, very few“transitional”disks are found(that is, disks w/ inner holes):

Statistics are ~a few of many hundreds of young stars.

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Calvet et al. 2005, ApJ, 630, L185

At least some disks evolve “from the inside out.” Does this apply more generally, or can disks dissipate in a variety of ways?

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Are there other examples? The case of LkH 330.

1´´

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For dust sublimation alone, the lines from T Tauri disks should be broader than those from Herbig Ae stars+disks. Often observed, but…

CO v =1-0 Emission from Transitional Disks?

The TW Hya lines are extremely narrow, with i~7° R≥0.37 AU. Similar for SR 9, DoAr 44, GM Aur. Rhot(KI) < R(CO) < Rdust(SED)

Good, hCO ≥ 11.09 eV to dissociate.