The JCMT BISTRO Survey: A Spiral Magnetic Field in a Hub-filament Structure, Monoceros R2

Author:

Hwang JihyeORCID,Kim JongsooORCID,Pattle KateORCID,Lee Chang WonORCID,Koch Patrick M.ORCID,Johnstone DougORCID,Tomisaka KohjiORCID,Whitworth AnthonyORCID,Furuya Ray S.ORCID,Kang Ji-hyunORCID,Lyo A-RanORCID,Chung Eun JungORCID,Arzoumanian DorisORCID,Park GeumsookORCID,Kwon WoojinORCID,Kim ShinyoungORCID,Tamura MotohideORCID,Kwon JungmiORCID,Soam ArchanaORCID,Han IlseungORCID,Hoang ThiemORCID,Kim Kyoung HeeORCID,Onaka TakashiORCID,Eswaraiah ChakaliORCID,Ward-Thompson DerekORCID,Liu Hong-LiORCID,Tang XindiORCID,Chen Wen PingORCID,Matsumura MasafumiORCID,Hoang Thuong DucORCID,Chen ZhiweiORCID,Le Gouellec Valentin J. M.ORCID,Kirchschlager FlorianORCID,Poidevin FrédérickORCID,Bastien PierreORCID,Qiu KepingORCID,Hasegawa TetsuoORCID,Lai Shih-PingORCID,Byun Do-YoungORCID,Cho JungyeonORCID,Choi Minho,Choi Youngwoo,Choi Yunhee,Jeong Il-GyoORCID,Kang MijuORCID,Kim Hyosung,Kim Kee-TaeORCID,Lee Jeong-EunORCID,Lee Sang-SungORCID,Lee Yong-HeeORCID,Lee HyeseungORCID,Kim Mi-RyangORCID,Yoo HyunjuORCID,Yun Hyeong-SikORCID,Chen Mike,Francesco James DiORCID,Fiege Jason,Fissel Laura M.ORCID,Franzmann EricaORCID,Houde MartinORCID,Lacaille KevinORCID,Matthews BrendaORCID,Sadavoy Sarah,Moriarty-Schieven GeraldORCID,Tahani MehrnooshORCID,Ching Tao-ChungORCID,Dai Y. SophiaORCID,Duan Yan,Gu QilaoORCID,Law Chi-Yan,Li Dalei,Li Di,Li Guangxing,Li Hua-baiORCID,Liu TieORCID,Lu XingORCID,Qian LeiORCID,Wang Hongchi,Wu JintaiORCID,Xie JinjinORCID,Yuan Jinghua,Zhang Chuan-PengORCID,Zhang Guoyin,Zhang YapengORCID,Zhou JianjunORCID,Zhu Lei,Berry DavidORCID,Friberg PerORCID,Graves SarahORCID,Liu JunhaoORCID,Mairs SteveORCID,Parsons HarrietORCID,Rawlings MarkORCID,Doi YasuoORCID,Hayashi SaekoORCID,Hull Charles L. H.ORCID,Inoue TsuyoshiORCID,Inutsuka Shu-ichiroORCID,Iwasaki Kazunari,Kataoka AkimasaORCID,Kawabata KojiORCID,Kim GwanjeongORCID,Kobayashi Masato I. N.ORCID,Nagata TetsuyaORCID,Nakamura FumitakaORCID,Nakanishi Hiroyuki,Pyo Tae-SooORCID,Saito Hiro,Seta Masumichi,Shimajiri YoshitoORCID,Shinnaga Hiroko,Tsukamoto Yusuke,Zenko Tetsuya,Chen Huei-Ru VivienORCID,Duan Hao-YuanORCID,Fanciullo LapoORCID,Kemper FranciscaORCID,Lee Chin-FeiORCID,Lin Sheng-JunORCID,Liu Sheng-YuanORCID,Ohashi NagayoshiORCID,Rao RamprasadORCID,Tang Ya-WenORCID,Wang Jia-WeiORCID,Yang Meng-Zhe,Yen Hsi-WeiORCID,Bourke Tyler L.ORCID,Chrysostomou AntonioORCID,Debattista VictorORCID,Eden DavidORCID,Eyres Stewart,Falle SamORCID,Fuller Gary,Gledhill TimORCID,Greaves JaneORCID,Griffin Matt,Hatchell JenniferORCID,Karoly JanikORCID,Kirk JasonORCID,Könyves VeraORCID,Longmore StevenORCID,van Loo SvenORCID,Looze Ilse de,Peretto Nicolas,Priestley Felix,Rawlings JonathanORCID,Retter Brendan,Richer JohnORCID,Rigby AndrewORCID,Savini GiorgioORCID,Scaife AnnaORCID,Viti SerenaORCID,Diep Pham NgocORCID,Ngoc Nguyen BichORCID,Tram Le NgocORCID,André PhilippeORCID,Coudé SimonORCID,Dowell C. Darren,Friesen RachelORCID,Robitaille Jean-FranćoisORCID

Abstract

Abstract We present and analyze observations of polarized dust emission at 850 μm toward the central 1 × 1 pc hub-filament structure of Monoceros R2 (Mon R2). The data are obtained with SCUBA-2/POL-2 on the James Clerk Maxwell Telescope (JCMT) as part of the B-fields in Star-forming Region Observations survey. The orientations of the magnetic field follow the spiral structure of Mon R2, which are well described by an axisymmetric magnetic field model. We estimate the turbulent component of the magnetic field using the angle difference between our observations and the best-fit model of the underlying large-scale mean magnetic field. This estimate is used to calculate the magnetic field strength using the Davis–Chandrasekhar–Fermi method, for which we also obtain the distribution of volume density and velocity dispersion using a column density map derived from Herschel data and the C18O (J = 3 − 2) data taken with HARP on the JCMT, respectively. We make maps of magnetic field strengths and mass-to-flux ratios, finding that magnetic field strengths vary from 0.02 to 3.64 mG with a mean value of 1.0 ± 0.06 mG, and the mean critical mass-to-flux ratio is 0.47 ± 0.02. Additionally, the mean Alfvén Mach number is 0.35 ± 0.01. This suggests that, in Mon R2, the magnetic fields provide resistance against large-scale gravitational collapse, and the magnetic pressure exceeds the turbulent pressure. We also investigate the properties of each filament in Mon R2. Most of the filaments are aligned along the magnetic field direction and are magnetically subcritical.

Publisher

American Astronomical Society

Subject

Space and Planetary Science,Astronomy and Astrophysics

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