Abstract
We determine the magnetic field strength in the OMC1 region of the Orion A filament via a new implementation of the Chandrasekhar Fermi method using observations performed as part of the James Clerk Maxwell Telescope (JCMT) B-Fields In Star-forming Region Observations (BISTRO) survey with the POL-2 instrument. We combine BISTRO data with archival SCUBA-2 and HARP observations to find a plane-of-sky magnetic field strength in OMC1 of B 6.6 4.7 pos = mG, where dBpos = 4.7 mG represents a predominantly systematic uncertainty. We develop a new method for measuring angular dispersion, analogous to unsharp masking. We find a magnetic energy density of ∼ 1.7 10-7 J m-3 in OMC1, comparable both to the gravitational potential energy density of OMC1 (∼10-7 J m-3) and to the energy density in the Orion BN/KL outflow (∼10-7 J m-3). We find that neither the Alfvén velocity in OMC1 nor the velocity of the super-Alfvénic outflow ejecta is sufficiently large for the BN/ KL outflow to have caused large-scale distortion of the local magnetic field in the ∼500 yr lifetime of the outflow. Hence, we propose that the hourglass field morphology in OMC1 is caused by the distortion of a primordial cylindrically symmetric magnetic field by the gravitational fragmentation of the filament and/or the gravitational interaction of the BN/KL and S clumps. We find that OMC1 is currently in or near magnetically supported equilibrium, and that the current large-scale morphology of the BN/KL outflow is regulated by the geometry of the magnetic field in OMC1, and not vice versa.
Original language | English |
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Article number | 122 |
Journal | Astrophysical Journal |
Volume | 846 |
Issue number | 2 |
DOIs | |
Publication status | Published - 5 Sept 2017 |
Keywords
- ISM: individual objects (OMC 1)
- magnetic fields
- stars: formation
- techniques: polarimetric