2013
DOI: 10.1002/asna.201211770
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Accretion, winds and outflows in young stars

Abstract: Young stars and planetary systems form in molecular clouds. After the initial radial infall an accretion disk develops. For classical T Tauri stars (CTTS, F-K type precursors) the accretion disk does not reach down to the central star, but it is truncated near the co-rotation radius by the stellar magnetic field. The inner edge of the disk is ionized by the stellar radiation, so that the accretion stream is funneled along the magnetic field lines. On the stellar surface an accretion shock develops, which is ob… Show more

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Cited by 15 publications
(12 citation statements)
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“…The physical motivation for an inner edge is a magnetospheric cavity (Bouvier et al 2007), where ionized material of the disk is lifted by the magnetic field lines from the midplane and accreted onto the star. This typically happens at the corotation radius (e.g., Günther 2013), where the magnetic field rotates at the same speed as the gas. It is therefore reasonable to not extend the modeled disk closer to the star than its corotation radius.…”
Section: Inner Edgementioning
confidence: 99%
“…The physical motivation for an inner edge is a magnetospheric cavity (Bouvier et al 2007), where ionized material of the disk is lifted by the magnetic field lines from the midplane and accreted onto the star. This typically happens at the corotation radius (e.g., Günther 2013), where the magnetic field rotates at the same speed as the gas. It is therefore reasonable to not extend the modeled disk closer to the star than its corotation radius.…”
Section: Inner Edgementioning
confidence: 99%
“…Inner disk edge R in The physical motivation for an inner edge of the gas disk is the development of a magnetospheric cavity (Bouvier et al 2007), which is thought to extend to the corotation radius, i.e. the location where the angular velocity of the stellar magnetic field and of the orbiting gas are equal (e.g., Günther 2013). For the numerical disk, we adopted the orbit radius corresponding to the rotation period of its host star for R in .…”
Section: Dust-to-gas Ratio ζ Dgmentioning
confidence: 99%
“…The dominant timescale in the optical is the stellar rotation period, typically a few days to a week or more (Rydgren & Vrba 1983;Bouvier et al 1986;Nguyen et al 2009). YSOs can have cool spots caused by magnetic activity similar to our Sun and also hot spots which mark the impact points of the accretion funnels onto the stellar surface (see, e.g., review by Günther 2013). This impact happens at freefall velocities up to 500 km s −1 ; thus, the accretion shock heats the accreted mass to X-ray emitting temperatures (see, e.g., reviews by Güdel 2004;Günther 2011).…”
Section: Ormentioning
confidence: 99%
“…YSOs can have cool spots caused by magnetic activity similar to our Sun and also hot spots which mark the impact points of the accretion funnels onto the stellar surface (see, e.g., review by Günther 2013). This impact happens at freefall velocities up to 500 km s −1 ; thus, the accretion shock heats the accreted mass to X-ray emitting temperatures (see, e.g., reviews by Güdel 2004;Günther 2011). In the optical, the accretion region appears as emission that often is approximated as a blackbody with temperature T < 10 000 K (Calvet & Gullbring 1998;Ingleby et al 2012, but see also Dodin & Lamzin 2012 who argue that line emission contributes to the veiling in addition to a continuum).…”
Section: Ormentioning
confidence: 99%