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Table B.1

Best fit parameters for the multiple systems in this study: targets with no clear substructures.

Name Parameters
Single power law with exponential cutoff
log Fν Rc γ1 γ2 Inc PA ΔRA ΔDec

V710 Tau −1.076 0.320 0.482 8.819 48.912 84.345 −0.022 2.685
                 
DH Tau −1.555 0.139 0.381 5.734 16.946 18.870 −0.108 −0.113

Single power law with exponential cutoff (both components)
log Fν Rc γ1 γ2 Inc PA ΔRA ΔDec

T Tau N −0.690 0.150 0.680 49.623 28.251 87.493 −0.085 −0.000
                 
T Tau S −1.690 0.040 1.501 0.297 61.558 7.864 −0.249 −0.656
                 
RW Aur A −1.206 0.139 0.700 26.711 55.048 41.132 −0.080 −0.123
                 
RW Aur B −1.812 0.090 0.074 11.945 74.556 40.994 −1.515 −0.532
                 
DK Tau A −1.511 0.122 0.598 38.642 12.859 4.513 −0.034 0.164
                 
DK Tau B −1.929 0.069 −0.122 26.849 77.966 28.050 2.047 −0.995
                 
HN Tau A −1.449 0.142 0.651 16.148 69.768 85.299 0.217 −0.120
                 
HN Tau B −3.447 0.203 2.467 10.303 49.461 −2.690 −1.820 −2.535
                 
UY Aur A −1.659 0.043 0.235 8.616 23.502 −53.601 0.161 0.022
                 
UY Aur B −2.193 0.055 1.768 10.444 25.571 −35.043 −0.520 −0.546
                 
HK Tau A −1.217 0.229 0.919 21.220 56.882 −5.117 0.174 −0.702
                 
HK Tau B −0.871 0.499 −1.182 11.356 83.242 41.236 0.599 −2.982

Notes. Results of the fitting of the visibilities of the data. The reported uncertainties on the best fit paramters include the correction factor discussed in Sect. 3.

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