Op. Lay et al., CONSTRAINTS ON THE HL-TAURI PROTOSTELLAR DISK FROM MILLIMETER-WAVE AND SUBMILLIMETER-WAVE INTERFEROMETRY, The Astrophysical journal, 489(2), 1997, pp. 917-927
Millimeter and submillimeter interferometry is used to probe the dusty
accretion disks around young protostars. New 460 GHz (lambda = 650 mu
m) data from the Caltech Submillimeter Observatory and the James Cler
k Maxwell Telescope CSO-JCMT Interferometer are combined with previous
345 GHz (lambda = 870 pm) data from CSO-JCMT, 220 GHz (lambda = 1.4 m
m) data from the Owens Valley Radio Observatory (OVRO) Millimeter Arra
y, 110 GHz (lambda = 2.7 mm) data from the Berkeley-Illinois-Maryland
Association Array (BIMA), and 43 GHz (lambda = 7 mm) data from the VLA
, in order to constrain the nature of the protostellar disk around HL
Tau on size scales of 50 AU and above. A power-law disk model is fitte
d directly to the measured visibility data, and probability distributi
ons are derived for the parameters. The effects of instrumental uncert
ainties are included in a consistent way. The position angle of the ma
jor axis of the emission is determined to be 127 degrees +/- 5 degrees
and the inclination 42 degrees +/- 5 degrees (where 0 degrees is face
-on), assuming the disk is thin, flat, and circular. A strongly flared
disk that is close to edge-on cannot be ruled out, however. The CSO-J
CMT and OVRO data favor centrally concentrated distributions of the su
rface density Sigma, where Sigma chi r(-p), and p > 1. This is not com
patible with the relatively large sizes measured at lower frequency by
BIMA and the VLA. No simple power-law disk model can be found that re
produces all of the millimeter and submillimeter data well. Such a mod
el, with radial power laws in the surface density and temperature, and
a single dust component, is therefore unlikely to be a good represent
ation of the actual disk structure. One possibility that would help to
reconcile the model with the data is the existence of more than one d
ust component, i.e., a range of grain sizes or structures in the disk
and no unique value of the emissivity index beta. Future models should
allow for this as well as for disk geometries that are not thin and f
lat.