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Table 1.

HST/STIS sample in this paper plus a system previously observed with this technique (HD 93 129 Aa,Ab).

Name ΔB d θ WDS ID Obs. date Res.?
(mag) (mas) (deg) (YYMMDD)
ζ Ori Aa,Ab 2.20* 39* 280 05407−0157 191118 N
ι Ori Aa,Ab 3.16 155* 98 05354−0555 191119 Y
15 Mon Aa,Ab 1.55 143 269 06410+0954 191129 Y
τ CMa Aa,Ab 0.90 95 310 07187−2457 200102 Y
τ CMa Aa,E 4.47 685† 310 07187−2457 200102 Y
HD 206 267 Aa,Ab 0.95 64 147 21390+5729 191206 Y
HD 193 443 A,B 0.26 138 250 20189+3817 191013 Y
HD 16 429 Aa,Ab 2.02 275 91 02407+6117 191126 Y
IU Aur A,B 2.04 138* 232 05279+3447 191003 Y
HD 93 129 Aa,Ab 1.23 36* 14 10440−5933 100407 Y

Notes. The position angle θ corresponds to the angle of the slit as measured from the first to the second component while d′ corresponds to the plane-of-the-sky separation between the two components along the slit. An asterisk is added for those cases where ΔB or d′ were fixed from the literature instead of measured from the data. The separation marked with a † was measured with the slit positioned far from the predicted position angle, making d and d′ significantly different (see text). Measured uncertainties are typically 0.01 mag in ΔB and 1 mas in d′.

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