4.6 Article

HOT GAS LINES IN T TAURI STARS

Journal

ASTROPHYSICAL JOURNAL SUPPLEMENT SERIES
Volume 207, Issue 1, Pages -

Publisher

IOP PUBLISHING LTD
DOI: 10.1088/0067-0049/207/1/1

Keywords

protoplanetary disks; stars: pre-main sequence; stars: variables: T Tauri, Herbig Ae/Be; surveys; ultraviolet: stars

Funding

  1. NASA through Space Telescope Science Institute (STScI) [HST-GO-11616.10, HST-GO-12161.01]
  2. NASA [NAS 5-26555]
  3. Science & Technology Facilities Council (STFC) [ST/J003255/1]
  4. UK's Science & Technology Facilities Council (STFC) [ST/G00711X/1]
  5. HST GTO [11533, 12036]
  6. STFC [ST/J003255/1, ST/G00711X/1] Funding Source: UKRI
  7. Science and Technology Facilities Council [ST/G00711X/1, ST/J003255/1] Funding Source: researchfish

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For Classical T Tauri Stars (CTTSs), the resonance doublets of NV, Si IV, and C IV, as well as the He II 1640 angstrom line, trace hot gas flows and act as diagnostics of the accretion process. In this paper we assemble a large high-resolution, high-sensitivity data set of these lines in CTTSs and Weak T Tauri Stars (WTTSs). The sample comprises 35 stars: 1 Herbig Ae star, 28 CTTSs, and 6 WTTSs. We find that the C IV, Si IV, and N V lines in CTTSs all have similar shapes. We decompose the C IV and He II lines into broad and narrow Gaussian components (BC and NC). The most common (50%) C IV line morphology in CTTSs is that of a low-velocity NC together with a redshifted BC. For CTTSs, a strong BC is the result of the accretion process. The contribution fraction of the NC to the C IV line flux in CTTSs increases with accretion rate, from similar to 20% to up to similar to 80%. The velocity centroids of the BCs and NCs are such that V-BC greater than or similar to 4 V-NC, consistent with the predictions of the accretion shock model, in at most 12 out of 22 CTTSs. We do not find evidence of the post-shock becoming buried in the stellar photosphere due to the pressure of the accretion flow. The He II CTTSs lines are generally symmetric and narrow, with FWHM and redshifts comparable to those of WTTSs. They are less redshifted than the CTTSs C IV lines, by similar to 10 km s(-1). The amount of flux in the BC of the He II line is small compared to that of the C IV line, and we show that this is consistent with models of the pre-shock column emission. Overall, the observations are consistent with the presence of multiple accretion columns with different densities or with accretion models that predict a slow-moving, low-density region in the periphery of the accretion column. For HN Tau A and RW Aur A, most of the C IV line is blueshifted suggesting that the C IV emission is produced by shocks within outflow jets. In our sample, the Herbig Ae star DX Cha is the only object for which we find a P-Cygni profile in the C IV line, which argues for the presence of a hot (105 K) wind. For the overall sample, the Si IV and N V line luminosities are correlated with the C IV line luminosities, although the relationship between Si IV and C IV shows large scatter about a linear relationship and suggests that TW Hya, V4046 Sgr, AA Tau, DF Tau, GM Aur, and V1190 Sco are silicon-poor, while CV Cha, DX Cha, RU Lup, and RW Aur may be silicon-rich.

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