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Table 4

Summary of our detection limits for each target.

Target Sep. PA Ref. Mass Radius ΔHα LHα (L) Lacc (L) (Myr−1)
(mas) (°) (MJ) (RJ) (mag) (erg s−1 cm−2)
HD135344B 180 a 10.2b 1.6c >9.8 < 3.8 × 10−15 < 2.0 × 10−6 < 3.7 × 10−6 < 2.4 × 10−12
TW Hya 390 d 2e 1.3c >9.3 < 1.9 × 10−14 < 2.2 × 10−6 < 3.5 × 10−6 < 1.0 × 10−11
HD100546 480 ± 4 8.9 ± 0.9 f 15f 2g >11.4 < 1.1 × 10−14 < 4.7 × 10−6 < 1.1 × 10−5 < 6.4 × 10−12
                     
~140 ~133 h 15i 2c >9.3 < 7.9 × 10−14 < 3.3 × 10−5 < 2.0 × 10−4 < 1.1 × 10−10
                     
HD169142 ~340 ~175 j 0.6j 1.4c >10.7 < 5.7 × 10−15 < 2.5 × 10−6 < 4.3 × 10−6 < 4.4 × 10−11
                     
156 ± 32 7.4 ± 11.3 k 10k 1.7c >9.9 < 1.2 × 10−14 < 5.2 × 10−6 < 1.3 × 10−5 < 7.6 × 10−11
MWC 758 111 ± 4 162 ± 5 l 5.5m 1.7n >9.4 < 1.4 × 10−14 < 1.2 × 10−5 < 4.3 × 10−5 < 5.5 × 10−11

Notes. While for HD100546, HD169142, and MWC 758 we consider the specific locations (separation and PA) of previously claimed companion candidates, we focused our analyses for HD135344B and TW Hya on separations related to disk gaps(hence no specific PA). Columns 5 and 6 give the mass and radius assumed for the accretion rate calculations, Col. 7 gives the contrast magnitude at the specific location and Cols. 8–11 report the values for the Hα line flux, Hα line luminosity, accretion luminosity, and mass accretion rate ignoring any possible dust around the companion.

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