TY - JOUR
T1 - A Three-dimensional Simulation of a Magnetized Accretion Disk
T2 - Fast Funnel Accretion onto a Weakly Magnetized Star
AU - Takasao, Shinsuke
AU - Tomida, Kengo
AU - Iwasaki, Kazunari
AU - Suzuki, Takeru K.
N1 - Funding Information:
We thank Drs. K. Shibata, S. Inutsuka, H. Kobayashi, T. Hosokawa, S. Okuzumi, T. Muto, M. Kunitomo, Z. Zhu, and J. Stone for fruitful discussion. We also thank the referee for useful comments. S.T. acknowledges support by the Research Fellowship of the Japan Society for the Promotion of Science (JSPS). This work was supported in part by the Ministry of Education, Culture, Sports, Science and Technology (MEXT), Grants-in-Aid for Scientific Research, 17H01105 (T.K.S.), 16H05998 (K.T. and K.I.), 16K13786 (K.T.), and JSPS KAKENHI grant No. 16J02063 (S.T.). Numerical computations were carried out on the Cray XC30 at the Center for Computational Astrophysics, National Astronomical Observatory of Japan. Test calculations were carried out on the XC40 at the Yukawa Institute for Theoretical Physics in Kyoto University. This research was also supported by MEXT as “Exploratory Challenge on Post-K computer” (Elucidation of the Birth of Exoplanets [Second Earth] and the Environmental Variations of Planets in the Solar System).
Publisher Copyright:
© 2018. The American Astronomical Society. All rights reserved..
PY - 2018/4/10
Y1 - 2018/4/10
N2 - We present the results of a global, three-dimensional magnetohydrodynamics simulation of an accretion disk with a rotating, weakly magnetized central star. The disk is threaded by a weak, large-scale poloidal magnetic field, and the central star has no strong stellar magnetosphere initially. Our simulation investigates the structure of the accretion flows from a turbulent accretion disk onto the star. The simulation reveals that fast accretion onto the star at high latitudes occurs even without a stellar magnetosphere. We find that the failed disk wind becomes the fast, high-latitude accretion as a result of angular momentum exchange mediated by magnetic fields well above the disk, where the Lorentz force that decelerates the rotational motion of gas can be comparable to the centrifugal force. Unlike the classical magnetospheric accretion scenario, fast accretion streams are not guided by magnetic fields of the stellar magnetosphere. Nevertheless, the accretion velocity reaches the free-fall velocity at the stellar surface due to the efficient angular momentum loss at a distant place from the star. This study provides a possible explanation why Herbig Ae/Be stars whose magnetic fields are generally not strong enough to form magnetospheres also show indications of fast accretion. A magnetically driven jet is not formed from the disk in our model. The differential rotation cannot generate sufficiently strong magnetic fields for the jet acceleration because the Parker instability interrupts the field amplification.
AB - We present the results of a global, three-dimensional magnetohydrodynamics simulation of an accretion disk with a rotating, weakly magnetized central star. The disk is threaded by a weak, large-scale poloidal magnetic field, and the central star has no strong stellar magnetosphere initially. Our simulation investigates the structure of the accretion flows from a turbulent accretion disk onto the star. The simulation reveals that fast accretion onto the star at high latitudes occurs even without a stellar magnetosphere. We find that the failed disk wind becomes the fast, high-latitude accretion as a result of angular momentum exchange mediated by magnetic fields well above the disk, where the Lorentz force that decelerates the rotational motion of gas can be comparable to the centrifugal force. Unlike the classical magnetospheric accretion scenario, fast accretion streams are not guided by magnetic fields of the stellar magnetosphere. Nevertheless, the accretion velocity reaches the free-fall velocity at the stellar surface due to the efficient angular momentum loss at a distant place from the star. This study provides a possible explanation why Herbig Ae/Be stars whose magnetic fields are generally not strong enough to form magnetospheres also show indications of fast accretion. A magnetically driven jet is not formed from the disk in our model. The differential rotation cannot generate sufficiently strong magnetic fields for the jet acceleration because the Parker instability interrupts the field amplification.
KW - accretion, accretion disks
KW - magnetohydrodynamics (MHD)
KW - stars: pre-main sequence
KW - stars: protostars
KW - stars: variables: T Tauri, Herbig Ae/Be
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U2 - 10.3847/1538-4357/aab5b3
DO - 10.3847/1538-4357/aab5b3
M3 - Article
AN - SCOPUS:85045581397
SN - 0004-637X
VL - 857
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 1
M1 - 4
ER -