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Table 3:

Parameters of the models that simulate the measured SED and MIR visibilities best.

Object (model-no.)
$M_{\rm disk}$ [ $M_{\rm\odot}$] $R_{\rm out}$ [AU] $R_{\rm in}$ [AU] $\beta$ $h_{\rm 100}$ [AU] $\vartheta$ [$^{\circ}$] $\dot{M}$[ $M_{\rm\odot}$/a]

DR Tau (I)
    0.10       $2.0 \times10^{-8}_{\rm (det.)}$

DR Tau (II)
0.1 90 0.10 0.75 15 20 $8.0 \times 10^{-8}_{\rm (1)}$

DR Tau (III)
    0.05       $8.0 \times 10^{-8}_{\rm (det.)}$

GW Ori (I,II)
1.0 360 0.35 1.10 22 10 $2.5 \times 10^{-7}_{\rm (2)}$

HD 72106 B
0.005 40 0.50 1.30 8 60 No Accretion

RU Lup
0.1 100 0.10 0.90 20 28 $1.0 \times 10^{-8}_{\rm (3)}$

HBC 639
0.1 120 0.10 1.00 10 65 No Accretion

S CrA N (I)
0.03 120 0.05 1.10 9 10 $4.0 \times 10^{-8}_{\rm (det.)}$

S CrA N (II)
      0.90 12 45  

S CrA S
0.03 100 0.10 1.05 8 30 $4.0 \times 10^{-8}_{\rm (det.)}$

References: (1): Akeson et al. (2005); (2): Calvet et al. (2002); (3): Herczeg et al. (2005).


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