Table 1
Sources analyzed in this work and their properties: class, [O i] flux, LX and LFUV, and presence of an optical jet/outflow.
Name | Class | [O i] 63 μm | [O i] 63 μm | L FUV | L X | Outflow |
[1e–17 W/m2] | disk only | [1e30 erg/s] | [1e30 erg/s] | [YES/NO] | ||
|
||||||
AATau | II | 2.2 ± 0.2 | 0.60 | 28.821 | 1.24![]() |
Y |
BPTau | II | 0.10 ± 0.03 | 58.641 | 1.36![]() |
N | |
CITau | II | 3.3 ± 0.5 | 13.321 | 0.19![]() |
N | |
CWTau | II | 7.2 ± 0.4 | 0.82 | 111.132 | 2.84![]() |
Y |
CXTau | T | 0.7 ± 0.3 | 0.681 | – | N | |
CYTau | II | 1.2 ± 0.4 | 13.321 | 0.13![]() |
N | |
DETau | II | 0.7 ± 0.6 | 30.411 | – | N | |
DFTau | II | 6.1 ± 0.6 | 9.951 | – | Y | |
DGTau | II | 134.00 ± 17.0 | 4.70 | 318.042 | 0.55![]() |
Y |
DHTau | II | <1.35 | – | 8.46![]() |
N | |
DKTau | II | 1.6 ± 0.3 | 18.582 | 0.92![]() |
N | |
DLTau | II | 2.2 ± 0.2 | 13.971 | – | Y | |
DMTau | T | 0.7 ± 0.2 | 58.281 | 2.00![]() |
N | |
DNTau | T | 0.6 ± 0.2 | 6.521 | 1.15![]() |
N | |
DOTau | II | 7.1 ± 1.0 | 1.45 | 470.601 | 0.24![]() |
Y |
DPTau | II | 14.8 ± 1.3 | 0.57 | 96.291 | 0.10![]() |
Y |
DQTau | II | 2.1 ± 0.4 | 0.822 | – | N | |
DSTau | II | 0.9 ± 0.2 | 49.961 | – | N | |
FFTau | III | <1.01 | – | 0.80![]() |
N | |
FMTau | II | 1.0 ± 0.2 | 4.891 | 0.53![]() |
N | |
FOTau | T | 1.20 ± 0.5 | – | 0.06![]() |
N | |
FQTau | II | <0.92 | – | 0.12![]() |
N | |
FSTau-A | II-FS | 35.8 ± 0.5 | – | 3.22![]() |
Y | |
FXTau | II | <1.38 | – | 0.50![]() |
N | |
GGTau | II | 5.1 ± 0.4 | 10.512 | – | N | |
GHTau | II | <0.85 | – | 0.11![]() |
N | |
GI-KTau | II | 3.1 ± 1.4 | 10.861 | 0.83![]() |
N | |
GMAur | T | 2.4 ± 0.5 | 28.241 | 1.60![]() |
N | |
GOTau | II | <5.38 | – | 0.25![]() |
N | |
HBC358 | III | <1.4 | – | 0.38![]() |
N | |
HKTau | II | 3.4 ± 0.2 | – | 0.08![]() |
N | |
HLTau | I | 51.3 ± 0.5 | – | 3.84![]() |
Y | |
HNTau | II | 4.1 ± 0.2 | 0.56 | 21.291 | 0.32![]() |
Y |
HOTau | II | <1.03 | – | 0.05![]() |
N | |
Haro6-13 | II | 7.0 ± 0.5 | – | 0.80![]() |
Y | |
IPTau | T | 0.6 ± 0.2 | 4.051 | – | N | |
IQTau | II | 1.5 ± 0.3 | – | 0.42![]() |
N | |
IRAS043 | II | 4.9 ± 0.2 | – | 0.40![]() |
Y | |
LkCa15 | T | 1.0 ± 0.2 | 4.453 | – | N | |
RWAur | II | 15.4 ± 0.5 | – | 1.60![]() |
Y | |
RYTau | T? | 10.5 ± 0.5 | 3.80 | 1042.561 | 5.52![]() |
Y |
SUAur | II | 8.6 ± 0.3 | 2.51 | 127.421 | 9.46![]() |
Y |
UYAur | II | 31.4 ± 0.4 | 2.16 | 27.732 | 0.40![]() |
Y |
UZTau | II | 4.5 ± 1.4 | – | 0.89![]() |
Y | |
V710Tau | II | 1.0 ± 0.6 | – | 1.38![]() |
N | |
V773Tau | II | 6.5 ± 0.3 | – | 9.49![]() |
Y | |
V819Tau | II | <0.898 | – | 2.44![]() |
N | |
XZTau | II | 36.1 ± 0.09 | – | 0.96![]() |
Y |
Notes. LX is measured between 0.3 and 10 keV, LFUV is measured between 7 and 10 eV. The oxygen fluxes listed in the fourth column are the estimated disk contribution to the total [O i] flux as explained in Sect. 5.2. The class of the objects is taken from Andrews & Williams (2005), X-ray luminosities between 0.3 and 10 kev are taken from Güdel et al. (2007, 2010), FUV luminosities with superscript 1 are retrieved from Yang et al. (2012) (errors are estimated to be ±30%), while the ones with superscript 2 and 3 are calculated using the accretion luminosity retrieved from Gullbring et al. (1998), and Ingleby et al. (2009) respectively (in this case the error is the one associated with the correlation: 0.38 dex). These values are then scaled by a factor 4.25 to estimate the luminosity in the 6–13.6 eV range. Outflow sources are objects for which extended emission in the optical, associated to a jet, has been observed. The [O i] emission from these objects has not been included in the primary analysis performed in this work.
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