Accretion, winds and jets: High-energy emission from young stellar objects

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Stars: Fomation, X-Rays: Stars, Stars: Pre-Main Sequence, Stars: Wind, Outflows

Scientific paper

Stars form by gravitational collapse from giant molecular clouds. Due to the conservation of angular momentum this collapse does not happen radially, but the matter forms circumstellar disk first and is consequently accreted from the disk onto the star. This thesis deals with the high-energy emission from young stellar objects, which are on the one hand still actively accreting from their disk, and on the other hand are no longer deeply obscured by their natal cloud. Stars of spectral type B and A are called Herbig Ae/Be (HAeBe) stars in this stage, all stars of later spectral type are termed classical T Tauri stars (CTTS); strictly speaking both types are defined by spectroscopic signatures, which are equivalent to the evolutionary stage described above. In this thesis CTTS and HAeBes are studied through high-resolution X-ray and UV spectroscopy and through detailed physical simulations.
Spectroscopic X-ray data is reduced and presented for two targets: The CTTS V4046 Sgr was observed with Chandra for 100 ks, using a high-resolution grating spectrometer. The lightcurve contains one flare and the He-like triplets of SiXIII, NeIX and OVII indicate high densities in the X-ray emitting regions. The second target is the HAeBe HD 163296, which was observed with XMM-Newton for 130 ks. The lightcurve shows only moderate variability, the elemental abundance follows a pattern, that is usual for active stars. The He-like triplet of OVII exhibits line ratios similar to coronal sources, indicating that neither a high density nor a strong UV-field is present in the region of the X-ray emission.
Using these and similar observations, it can be concluded that at least three mechanisms contribute to the observed high-energy emission from CTTS: First, those stars have active coronae similar to main-sequence stars, second, the accreted material passes through a strong accretion shock at the stellar surface, which heats it to a few MK, and, third, some CTTS drive powerful outflows. Shocks within these jets can heat the matter to X-ray emitting temperatures. The first is already well characterised; for the latter two scenarios models are presented in this thesis. The accretion shock is treated in a stationary 1D model, taking non-equilibrium ionisations explicitly into account. The magnetic field is strong enough to suppress motion perpendicular to the field lines, so the use of a 1D geometry is justified. The radiative loss is calculated as optically thin emission with the CHIANTI database. A combination of simulated post-shock cooling zone spectra and coronal gas is fitted to the observations of the CTTS TW Hya and V4046 Sgr. Both stars require only small mass accretion rates to power the X-ray emission (2×10-10 Msun/yr and 3×10-11 Msun/yr, respectively).
The CTTS DG Tau is heavily absorbed and the observed soft X-ray emission originates spatially offset from the star. In this thesis a physical model is presented which explains the emission by a shock front travelling along the ejected jet. Shock velocities between 400 and 500 km/s are required to explain the observed spectrum. For a electron density >105 cm-3 all shock dimensions are so small that they remain undetectable in optical observations as observed.
The spectral resolution in X-rays is not sufficient to analyse the line profiles, so UV data is used for this purpose. Line profiles extend up to 500 km/s in sample of CTTS observed with FUSE. Likely contribution from both, infalling and outflowing gas, contributes to the observed emission. The current models do not explain the observed line profiles in detail, especially the line width causes problems.
HAeBe stars have hot plasma, which can only be explained as an active corona, similar to the CTTS. Accretion does not contribute significantly to the X-ray emission, instead the line ratios in the He-like triplets point to an origin in the outflows, similar to the CTTS jets. A model comparable to DG Tau reproduces the observed emission.

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