4.7 Article

TW Hya: SPECTRAL VARIABILITY, X-RAYS, AND ACCRETION DIAGNOSTICS

Journal

ASTROPHYSICAL JOURNAL
Volume 750, Issue 1, Pages -

Publisher

IOP PUBLISHING LTD
DOI: 10.1088/0004-637X/750/1/73

Keywords

accretion, accretion disks; stars: individual (TW Hydrae); stars: pre-main sequence; stars: variables: T Tauri, Herbig Ae/Be; stars: winds, outflows

Funding

  1. Science and Technology Facilities Council of the UK
  2. Division Of Astronomical Sciences
  3. Direct For Mathematical & Physical Scien [0754568] Funding Source: National Science Foundation

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The nearest accreting T Tauri star, TW Hya was intensively and continuously observed over similar to 17 days with spectroscopic and photometric measurements from four continents simultaneous with a long segmented exposure using the Chandra satellite. Contemporaneous optical photometry from WASP-S indicates a 4.74 day period was present during this time. The absence of a similar periodicity in the H alpha flux and the total X-ray flux which are dominated by accretion processes and the stellar corona, respectively, points to a different source of photometric variations. The H alpha emission line appears intrinsically broad and symmetric, and both the profile and its variability suggest an origin in the post-shock cooling region. An accretion event, signaled by soft X-rays, is traced spectroscopically for the first time through the optical emission line profiles. After the accretion event, downflowing turbulent material observed in the H alpha and H beta lines is followed by He I (lambda 5876) broadening near the photosphere. Optical veiling resulting from the heated photosphere increases with a delay of similar to 2 hr after the X-ray accretion event. The response of the stellar coronal emission to an increase in the veiling follows similar to 2.4 hr later, giving direct evidence that the stellar corona is heated in part by accretion. Subsequently, the stellar wind becomes re-established. We suggest a model that incorporates the dynamics of this sequential series of events: an accretion shock, a cooling downflow in a supersonically turbulent region, followed by photospheric and later, coronal heating. This model naturally explains the presence of broad optical and ultraviolet lines, and affects the mass accretion rates determined from emission line profiles.

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