2014
DOI: 10.1051/0004-6361/201424136
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X-shooter spectroscopy of young stellar objects

Abstract: Disks around T Tauri stars are known to lose mass, as best shown by the profiles of the forbidden emission lines of low-ionization species. At least two separate kinematic components have been identified, one characterized by velocity shifts of tens to hundreds of km s −1 (HVC) and one with a much lower velocity of a few km s −1 (LVC). The HVC are convincingly associated to the emission of jets, but the origin of the LVC is still unknown. In this paper we analyze the forbidden line spectrum of a sample of 44 m… Show more

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Cited by 94 publications
(139 citation statements)
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“…From the diagnostic analysis it results that the LVC shares the same electron density and extinction as the base of the HVC, but has a lower temperature, on the order of ∼7000 K. Forbidden line emission components centered close to systemic velocity are features commonly observed in CTT stars (e.g., Hartigan et al 1995;Natta et al 2014). The typical peak velocities of CTT LVCs are in the range ∼5−20 km s −1 (thus closer to systemic velocity than the HH34 LVC) and they are usually brighter than the corresponding HVC emission, even in sources known to drive prominent jets (e.g., Hartigan et al 1995).…”
Section: Origin Of the Lvcmentioning
confidence: 95%
“…From the diagnostic analysis it results that the LVC shares the same electron density and extinction as the base of the HVC, but has a lower temperature, on the order of ∼7000 K. Forbidden line emission components centered close to systemic velocity are features commonly observed in CTT stars (e.g., Hartigan et al 1995;Natta et al 2014). The typical peak velocities of CTT LVCs are in the range ∼5−20 km s −1 (thus closer to systemic velocity than the HH34 LVC) and they are usually brighter than the corresponding HVC emission, even in sources known to drive prominent jets (e.g., Hartigan et al 1995).…”
Section: Origin Of the Lvcmentioning
confidence: 95%
“…This is a particularly interesting relation as it is obtained independently from models of PMS evolution, thus it can be considered a "purely observational" plot. The plot also indicates the best-fit relation for the GTO sample by Natta et al (2014), in which the slope is 1.53 ± 0.18.…”
Section: Accretion Luminosity and Stellar Luminosity Relationmentioning
confidence: 99%
“…Star-disk interaction processes can be studied observationally through the strong signatures they introduce in the spectra of YSOs. Accretion shocks give rise to continuum excess emission in the UV (e.g., Valenti et al 1993;Gullbring et al 1998Gullbring et al , 2000Calvet et al 2000) and the prominent emission of permitted lines across the whole spectrum (e.g., Muzerolle et al 1998aMuzerolle et al ,b,c, 2003Natta et al 2004), while winds are traced by various forbidden emission lines (e.g., Hartigan et al 1995;Rigliaco et al 2013;Natta et al 2014). In recent years, new instruments have provided the possibility of studying these processes simultaneously in large samples of objects.…”
Section: Introductionmentioning
confidence: 99%
“…The Taurus targets analyzed here follow the L acc -L distribution of the Lupus targets, while the Chamaeleon II targets are located in the lower part of the distribution. With respect to the best fit of the sample of Alcalá et al (2014) (shown in the figure as a black dotted line, from Natta et al 2014), the Chamaeleon I targets follow a steeper slope of L acc vs. L . However, the two values are compatible.…”
Section: Accretion Luminosity and Stellar Luminosity Dependencementioning
confidence: 99%