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Table 6

Fluxes and equivalent widths of Balmer lines.

Name Hα Hβ Hγ Hδ H8 H9 H10 H11 10%Hα F360/F400
TWA9A 14.0 ± 1.1 4.7 ± 1.8 2.7 ± 1.5 2.2 ± 1.0 1.4 ± 0.2 1.0 ± 0.1 0.82 ± 0.07 0.91 ± 0.47 135.0 0.38
−1.48 −0.68 −0.62 −0.59 −0.80 −0.83 −0.43 −0.65
SO879 1.8 ± 0.2 0.52 ± 0.15 0.23 ± 0.08 0.20 ± 0.06 0.15 ± 0.01 0.11 ± 0.01 0.10 ± 0.00 0.078 ± 0.022 242.0 0.38
−2.08 −1.17 −0.70 −1.12 −1.62 −1.57 −1.74 −0.77
TWA6 36.4 ± 4.0 8.4 ± 2.1 5.1 ± 3.9 3.3 ± 0.7 2.0 ± 0.1 1.5 ± 0.1 1.4 ± 0.1 1.3 ± 0.7 362.0 0.41
−4.17 −1.68 −1.02 −1.43 −1.47 −1.54 −1.67 −1.36
TWA25 47.3 ± 3.7 18.8 ± 3.4 10.4 ± 2.6 7.5 ± 1.4 4.8 ± 0.2 3.4 ± 0.2 2.7 ± 0.2 2.2 ± 0.3 165.4 0.42
−2.69 −1.94 −1.86 −1.81 −2.26 −1.97 −1.14 −1.15
TWA14 15.4 ± 1.1 3.6 ± 0.5 2.1 ± 0.5 1.4 ± 0.2 0.87 ± 0.02 0.63 ± 0.02 0.50 ± 0.02 0.41 ± 0.07 262.2 0.45
−5.77 −3.18 −3.03 −2.91 −3.30 −2.73 −1.28 −1.87
TWA13B 23.8 ± 1.9 8.8 ± 1.4 4.8 ± 1.1 3.3 ± 0.5 1.9 ± 0.1 1.3 ± 0.1 0.95 ± 0.08 0.81 ± 0.12 121.9 0.39
−2.37 −1.94 −1.88 −1.75 −2.07 −1.65 −0.51 −0.94
TWA13A 85.7 ± 5.5 30.2 ± 4.0 17.0 ± 3.4 10.6 ± 1.3 4.8 ± 0.1 3.0 ± 0.1 2.3 ± 0.1 1.7 ± 0.2 287.8 0.45
−7.58 −6.07 −5.48 −5.11 −4.30 −3.41 −1.28 −1.68
TWA2A 42.0 ± 5.0 13.9 ± 2.1 6.6 ± 1.5 4.4 ± 0.8 2.8 ± 0.1 2.0 ± 0.1 1.4 ± 0.1 1.3 ± 0.2 154.7 0.38
−2.25 −1.88 −1.56 −1.36 −1.64 −1.38 −0.43 −0.84
Sz122 6.4 ± 0.8 3.2 ± 0.3 2.3 ± 0.6 1.5 ± 0.4 1.2 ± 0.1 1.0 ± 0.1 0.86 ± 0.05 0.59 ± 0.08 660.3 0.74
−6.76 −8.67 −10.00 −8.02 −11.57 −11.69 −10.02 −6.27
TWA9B 5.9 ± 0.6 2.0 ± 0.1 1.0 ± 0.1 0.71 ± 0.06 0.37 ± 0.01 0.24 ± 0.01 0.18 ± 0.01 0.16 ± 0.01 137.6 0.39
−4.81 −4.83 −4.20 −3.50 −3.09 −2.49 −0.71 −1.54
TWA15B 6.8 ± 0.3 2.0 ± 0.1 1.1 ± 0.1 0.72 ± 0.06 0.38 ± 0.01 0.27 ± 0.02 0.19 ± 0.01 0.16 ± 0.01 157.7 0.45
−8.96 −7.94 −7.19 −6.48 −6.20 −5.18 −1.60 −3.11
TWA7 46.7 ± 3.9 13.3 ± 0.9 6.8 ± 0.6 4.5 ± 0.4 2.6 ± 0.1 1.8 ± 0.1 1.4 ± 0.1 1.1 ± 0.1 111.6 0.41
−4.73 −4.53 −3.82 −3.36 −2.97 −2.36 −0.48 −1.68
TWA15A 10.4 ± 0.6 3.0 ± 0.2 1.8 ± 0.1 1.3 ± 0.1 0.62 ± 0.02 0.47 ± 0.02 0.33 ± 0.02 0.25 ± 0.03 250.3 0.55
−12.43 −10.34 −10.80 −9.68 −6.33 −8.07 −3.36 −4.06
Sz121 5.9 ± 0.8 1.1 ± 0.1 0.50 ± 0.10 0.28 ± 0.06 0.15 ± 0.01 0.12 ± 0.01 0.10 ± 0.01 0.087 ± 0.020 377.9 0.38
−7.01 −5.06 −3.79 −2.90 −2.33 −2.39 −2.32 −2.02
Sz94 2.3 ± 0.2 0.75 ± 0.05 0.42 ± 0.04 0.27 ± 0.02 0.14 ± 0.01 0.087 ± 0.006 0.064 ± 0.006 0.047 ± 0.008 188.9 0.39
−5.67 −5.79 −5.49 −4.43 −3.91 −2.73 −2.66 −1.18
SO797 0.16 ± 0.02 0.035 ± 0.003 0.016 ± 0.002 0.0099 ± 0.0015 0.0057 ± 0.0006 0.0037 ± 0.0011 0.0030 ± 0.0011 0.0022 ± 0.0007 149.3 0.43
−6.85 −6.83 −5.23 −3.89 −5.95 −3.71 −3.47 −1.48
SO641 0.090 ± 0.009 0.019 ± 0.001 0.0097 ± 0.0010 0.0053 ± 0.0006 0.0033 ± 0.0003 0.0025 ± 0.0003 0.0018 ± 0.0003 0.0012 ± 0.0002 131.2 0.38
−8.04 −9.08 −8.38 −5.42 −6.91 −5.98 −5.97 −1.74
Par−Lup3−2 1.1 ± 0.2 0.26 ± 0.03 0.14 ± 0.02 0.080 ± 0.011 0.041 ± 0.003 0.026 ± 0.003 0.019 ± 0.005 0.017 ± 0.005 138.7 0.36
−4.97 −4.88 −4.07 −2.67 −1.90 −1.38 −0.65 −1.39
SO925 0.081 ± 0.009 0.012 ± 0.001 0.0050 ± 0.0011 0.0030 ± 0.0013 <0.0012 <0.0011 <0.000975 <0.000877 142.2 0.68
−8.55 −6.81 −5.59 −4.29 ... ... ... ...
SO999 0.20 ± 0.02 0.031 ± 0.003 0.016 ± 0.002 0.0091 ± 0.0020 0.0050 ± 0.0011 0.0036 ± 0.0006 0.0024 ± 0.0005 0.0021 ± 0.0007 147.1 0.45
−8.70 −7.99 −7.80 −5.31 −4.23 −4.18 −2.43 −1.35
Sz107 1.8 ± 0.2 0.40 ± 0.03 0.21 ± 0.02 0.13 ± 0.02 0.064 ± 0.010 0.049 ± 0.007 0.036 ± 0.006 0.025 ± 0.008 254.9 0.38
−11.72 −11.77 −9.88 −6.91 −4.28 −4.23 −2.57 −2.07
Par−Lup3−1 0.22 ± 0.02 0.024 ± 0.007 0.016 ± 0.007 0.0073 ± 0.0060 <0.0082 <0.0066 <0.0072 <0.0055 140.0 1.43
−15.78 −16.82 −29.99 −9.01 ... ... ... ...
TWA26 0.052 ± 0.008 0.012 ± 0.002 0.0085 ± 0.0016 0.0068 ± 0.0017 0.0038 ± 0.0007 <0.0020 <0.0022 <0.0018 138.4 1.55
−9.91 −27.07 −66.62 −35.39 −97.42 ... ... ...
TWA29 0.019 ± 0.003 <0.0016 <0.0014 <0.0018 <0.0021 <0.0017 <0.0028 <0.0028 114.9 1.56
−14.24 ... ... ... ... ... ... ...

Notes. Fluxes (10-14 erg s-1 cm-2) are reported in the first rows for each object with their errors, with equivalent widhts (Å) in the second rows. The Hα 10% width is in km s-1. The last column refers to the Balmer jump ratio, intened as the ratio between the flux at ~360 nm to the flux at ~400 nm. Upper limits are reported with <.

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