Lavraud, B. and Fargette, N. and Réville, V. and Szabo, A. and Huang, J. and Rouillard, A. P. and Viall, N. and Phan, T. D. and Kasper, J. C. and Bale, S. D. and Berthomier, M. and Bonnell, J. W. and Case, A. W. and Dudok de Wit, T. and Eastwood, J. P. and Génot, V. and Goetz, K. and Griton, L. S. and Halekas, J. S and Harvey, P. and Kieokaew, R. and Klein, K. G. and Korreck, K. E. and Kouloumvakos, A. and Larson, D. E. and Lavarra, M. and Livi, R. and Louarn, P. and MacDowall, R. J. and Maksimovic, M. and Malaspina, D. and Nieves-Chinchilla, T. and Pinto, R. F. and Poirier, N. and Pulupa, M. and Raouafi, N. E. and Stevens, M. L. and Toledo-Redondo, S. and Whittlesey, P. L. (2020) The Heliospheric Current Sheet and Plasma Sheet during Parker Solar Probe’s First Orbit. The Astrophysical Journal, 894 (2). L19. ISSN 2041-8213
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Abstract
We present high-angular-resolution Atacama Large Millimeter/submillimeter Array images of N2H+ (1–0) that have been combined with those from the Nobeyama telescope toward the Orion Molecular Cloud (OMC)-2 and OMC-3 filamentary regions. The filaments (with typical widths of ∼0.1 pc) and dense cores are resolved. The measured 2D velocity gradients of cores are between 1.3 and 16.7 km s−1 pc−1, corresponding to a specific angular momentum (J/M) between 0.0012 and 0.016 pc km s−1. With respect to the core size R, the specific angular momentum follows a power law J/M ∝ R1.52±0.14. The ratio (β) between the rotational energy and gravitational energy ranges from 0.00041 to 0.094, indicating insignificant support from rotation against gravitational collapse. We further focus on the alignment between the cores' rotational axes, which is defined to be perpendicular to the direction of the velocity gradient (θG), and the direction of elongation of filaments (θf) in this massive star-forming region. The distribution of the angle between θf and θG was found to be random, i.e., the cores' rotational axes have no discernible correlation with the elongation of their hosting filament. This implies that, in terms of angular momentum, the cores have evolved to be dynamically independent from their natal filaments.
Item Type: | Article |
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Subjects: | GO for STM > Physics and Astronomy |
Depositing User: | Unnamed user with email support@goforstm.com |
Date Deposited: | 26 May 2023 06:08 |
Last Modified: | 13 Jan 2024 03:57 |
URI: | http://archive.article4submit.com/id/eprint/908 |