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Published November 10, 2008 | Published
Journal Article Open

Redshifted absorption at He I λ10830 as a probe of the accretion geometry of T Tauri stars

Abstract

We probe the geometry of magnetospheric accretion in classical T Tauri stars (CTTSs) by modeling red absorption at He I λ10830 via scattering of the stellar and veiling continua. Under the assumptions that the accretion flow is an azimuthally symmetric dipole and helium is sufficiently optically thick that all incident 1 μm radiation is scattered, we illustrate the sensitivity of He I λ10830 red absorption to both the size of the magnetosphere and the filling factor of the hot accretion shock. We compare model profiles to those observed in 21 CTTSs with subcontinuum redshifted absorption at He I λ10830 and find that about half of the stars have red absorption and 1 μm veilings that are consistent with dipole flows of moderate width with accretion shock filling factors matching the size of the magnetospheric footpoints. However, the remaining 50% of the profiles, with a combination of broad, deep absorption and low 1 μm veiling, require very wide flows where magnetic footpoints are distributed over 10%-20% of the stellar surface but accretion shock filling factors are <1%. We model these profiles by invoking large magnetospheres dilutely filled with accreting gas, leaving the disk over a range of radii in many narrow "streamlets" that fill only a small fraction of the entire infall region. In some cases accreting streamlets need to originate in the disk between several R_* and at least the corotation radius. A few stars have such deep absorption at velocities >0.5V_(esc) that flows near the star with less curvature than a dipole trajectory seem to be required.

Additional Information

© The American Astronomical Society. Received 2008 April 24, accepted for publication 2008 July 14. NASA grant NNG506GE47G issued through the Office of Space Science provides support for this project. Thanks to A. Rostopchina for personally providing the lastmeasurement needed to derive stellar parameters for every star in the sample and to M. Romanova for stimulating conversations on accretion flows. We acknowledge helpful conversations with J. Bjorkman, S. Cabrit, N. Calvet, L. Hartmann, S. Matt, and an anonymous referee. The authors wish to recognize and acknowledge the very significant cultural role and reverence that the summit of Mauna Kea has always had within the indigenous Hawaiian community. We are most fortunate to have had the opportunity to conduct observations with the Keck II telescope from this mountain.

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