Constraining the nature of DG Tau A's thermal and non-thermal radio emission

被引:0
|
作者
Purser S.J.D. [1 ]
Ainsworth R.E. [1 ,2 ]
Ray T.P. [1 ]
Green D.A. [3 ]
Taylor A.M. [1 ,4 ]
Scaife A.M.M. [2 ]
机构
[1] School of Cosmic Physics, Dublin Institute for Advanced Studies, 31 Fitzwilliam Place
[2] Jodrell Bank Centre for Astrophysics, School of Physics and Astronomy, University of Manchester, Alan Turing Building, Oxford Road, Manchester
[3] Astrophysics Group, Cavendish Laboratory, 19 J. J. Thomson Avenue, Cambridge
[4] DESY, Platanenallee 6, Zeuthen
基金
欧盟地平线“2020”; 英国科学技术设施理事会; 欧洲研究理事会;
关键词
ISM: jets and outflows; Radiationmechanisms: non-thermal; Radio continuum: general; Stars: formation; Stars: individual (DG Tau A); Stars: low-mass;
D O I
10.1093/MNRAS/STY2649
中图分类号
学科分类号
摘要
DG Tau A, a class-II young stellar object (YSO), displays both thermal and non-thermal radio emission associated with its bipolar jet. To investigate the nature of this emission, we present sensitive (σ ~ 2 μJy beam-1), Karl G. Jansky Very Large Array (VLA) 6 and 10 GHz observations. Over 3.81 yr, no proper motion is observed towards the non-thermal radio knot C, previously thought to be a bowshock. Its quasi-static nature, spatially resolved variability, and offset from the central jet axis support a scenario whereby it is instead a stationary shock driven into the surrounding medium by the jet. Towards the internal working surface, knot A, we derive an inclination-corrected absolute velocity of 258 ± 23 km s-1. DG Tau A's receding counterjet displays a spatially resolved increase in flux density, indicating a variable massloss event, the first time such an event has been observed in the counterjet. For this ejection, we measure an ionized mass-loss rate of (3.7 ± 1.0) × 10-8M⊙ yr-1 during the event. A contemporaneous ejection in the approaching jet is not seen, showing it to be an asymmetric process. Finally, using radiative transfermodelling, we find that the extent of the radio emission can only be explained with the presence of shocks, and therefore reionization, in the flow. Our modelling highlights the need to consider the relative angular size of optically thick, and thin, radio emission from a jet, to the synthesized beam, when deriving its physical conditions from its spectral index. © 2018 The Author(s).
引用
收藏
页码:5532 / 5542
页数:10
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