Title: Constraining TW Hydra Disk Properties
1Constraining TW Hydra Disk Properties
- Chunhua Qi
- Harvard-Smithsonian Center for Astrophysics
Collaborators D.J. Wilner, P.T.P. Ho, T.L.
Bourke, N. Calvet (CfA)
G.A. Blake(Caltech), M. Hogerheijde(Leiden),
N. Ohashi(ASIAA),
E. Bergin (U. Michigan)
2TW Hya disk in scattered light
Weinberger et al. 2002
- Closest classical T Tauri star, 56 pc in
distance - Nearly face on disk around.
- Strong X-ray, UV radiation
- Age variable from 6 -20 Myr, highly evolved
system
3Outline
- SMA observations
- Dust continuum emission (220-355 GHz)
- Molecular line emission (cool gas 20-40 K)
- 2D radiative transfer calculation and Chi-square
analysis on disk properties - Temperature profile (surface heating)
- Outer radius
- Vsini at 100 AU
- Depletion
- Summary
4SMA Observations
5TW Hya Continuum
- 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.
6TW Hya Images I
CO 2-1
CO 3-2
13CO 2-1
7TW Hya Images II
HCN 3-2
HCO 3-2
CN 2-1
8Aikawa et al. 2002 Van Zadelhoff et al. 2003
- (Sub)mm molecular emission typically from cool
gas 20-40 k - Some common lines are optically thick like CO
- Physical and chemical processes ( freeze out,
photodissociation etc.) add the complexity of
analysis.
9Data Analysis
- We use a 2-D accelerated Monte Carlo model
(Hogerheijde van der Tak 2000) to calculate the
radiative transfer and molecular excitation. - Chi-square analysis
10CO 2-1
CO 3-2
Blue Canonical Model (Calvet et al. 2002, Qi et
al. 2004 ) Black SMA data
11The Effects of X-Rays
Mean heating energy per ionization
Glassgold Najita 2001
Mean dust radius
12CO 2-1
CO 3-2
CO 6-5
Blue Canonical Model (Calvet et al.
2002, Qi et al. 2004 ) Black SMA
data Red Model with X ray heating
13Constaining Outer Radius
- Rout 172 2 AU
- Vsini at 100 AU 0.27 0.01km/s
- Turbulence velocity 0.12 0.01 km/s
- Uncertainty can be limited by the velocity
resolution.
CO
CO
14Smaller outer radius photochemical effect ?
CO/13CO60
- Rout 110 5 AU
- Isotope-selective photodissociation of CO
- Rout 120 10 AU
- HCN large cross sections which absorb Lya
radiation
1513CO 2-1
Model (Rout 110 AU)
Model (Rout 172 AU)
Data
16Depletion
- Dc constant depletion factor
- Dj jump depletion factor where the kinetic
temperature falls below 22K - Dc 10-1.2 Dj 10-2.2
17Summary
- Dust emission follows closely the predictions of
the irradiated accretion disk model of Calvet et
al. 2002. - Higher gas temperature vs dust temperature on the
disk surface is needed to explain the line
intensity, probably due to X-ray heating. - Outer radius can be well constrained, given the
resolution small enough. We have the first clear
evidence of the isotope-selective
photodissociation of CO in the disk. - Substantial CO depletion, by an order of
magnitude or more, is required to explain the
line emission.
18Constraining inclination
(Vsini)0.27 km/s
- We can resolve the disk at radii where most of
the disk mass resides. Can place strong
constraints on vsini at 100AU. - Very hard to use the kinematics to disentangle M
from inclination. Better spectral resolution is
needed.
19CO 2-1
Model vsini 0.273 (i6o)
Model vsini0.273, (i13.5o)
Data