X-Shooter spectroscopy of young stellar objects III. Photospheric and chromospheric properties of Class III objects
B.Stelzer (1), A.Frasca (2), J.M.Alcala (3), C.F.Manara (4), K.Biazzo, (3,2), E.Covino (3), E.Rigliaco (5), L.Testi (4), S.Covino (6), and V.D'Elia, (7) ((1) INAF-Palermo, (2) INAF-Catania, (3) INAF-Capodimonte, (4) ESO, Garching, (5) Lunar, Planetary Lab Tucson, (6) INAF-Brera

TL;DR
This study uses X-Shooter spectra to analyze the photospheric and chromospheric properties of Class III young stellar objects, comparing chromospheric and coronal emissions and exploring activity diagnostics across different atmospheric layers.
Contribution
It provides detailed measurements of stellar parameters and activity indicators for Class III objects, and compares chromospheric and coronal emissions, offering new insights into stellar activity in young stars.
Findings
X-ray and Halpha luminosities are independent of effective temperature in early-M stars.
Coronal emission exceeds chromospheric emission by a factor of 2-5 in active pre-main sequence stars.
Flux ratios between emission lines depend smoothly on effective temperature.
Abstract
We analyzed X-Shooter/VLT spectra of 24 ClassIII sources from three nearby star-forming regions (sigmaOrionis, LupusIII, and TWHya). We determined the effective temperature, surface gravity, rotational velocity, and radial velocity by comparing the observed spectra with synthetic BT-Settl model spectra. We investigated in detail the emission lines emerging from the stellar chromospheres and combined these data with archival X-ray data to allow for a comparison between chromospheric and coronal emissions. Both X-ray and Halpha luminosity as measured in terms of the bolometric luminosity are independent of the effective temperature for early-M stars but decline toward the end of the spectral M sequence. For the saturated early-M stars the average emission level is almost one dex higher for X-rays than for Halpha: log(L_x/L_bol) = -2.85 +- 0.36 vs. log(L_Halpha/L_bol) = -3.72 +- 0.21. When…
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