Formation of the Hub–Filament System G33.92+0.11: Local Interplay between Gravity, Velocity, and Magnetic Field

The formation of filaments in molecular clouds is an important process in star formation. Hub–filament systems (HFSs) are a transition stage connecting parsec-scale filaments and protoclusters. Understanding the origin of HFSs is crucial to reveal how star formation proceeds from clouds to cores. Here we report James Clerk Maxwell telescope POL-2 850 μm polarization and IRAM 30 m C18O (2–1) line observations toward the massive HFS G33.92+0.11. The 850 μm continuum map reveals four major filaments converging to the center of G33.92+0.11 with numerous short filaments connecting to the major filaments at local intensity peaks. We estimate the local orientations of filaments, magnetic field, gravity, and velocity gradients from observations, and we examine their correlations based on their local properties. In the high-density areas, our analysis shows that the filaments tend to align with the magnetic field and local gravity. In the low-density areas, we find that the local velocity gradients tend to be perpendicular to both the magnetic field and local gravity, although the filaments still tend to align with local gravity. A global virial analysis suggests that the gravitational energy overall dominates the magnetic and kinematic energy. Combining local and global aspects, we conclude that the formation of G33.92+0.11 is predominantly driven by gravity, dragging and aligning the major filaments and magnetic field on the way to the inner dense center. Traced by local velocity gradients in the outer diffuse areas, ambient gas might be accreted onto the major filaments directly or via the short filaments.

[1]  Lei Zhu,et al.  The JCMT BISTRO Survey: Magnetic Fields Associated with a Network of Filaments in NGC 1333 , 2020, The Astrophysical Journal.

[2]  E. Rosolowsky,et al.  Velocity-coherent Filaments in NGC 1333: Evidence for Accretion Flow? , 2020, The Astrophysical Journal.

[3]  P. Koch,et al.  Multiwavelength Polarimetry of the Filamentary Cloud IC 5146. II. Magnetic Field Structures , 2019, The Astrophysical Journal.

[4]  P. Koch,et al.  Gravity, Magnetic Field, and Turbulence: Relative Importance and Impact on Fragmentation in the Infrared Dark Cloud G34.43+00.24 , 2019, The Astrophysical Journal.

[5]  J. Pineda,et al.  Multicomponent Kinematics in a Massive Filamentary Infrared Dark Cloud , 2018, The Astrophysical Journal.

[6]  E. Pascale,et al.  JCMT BISTRO Survey: Magnetic Fields within the Hub-filament Structure in IC 5146 , 2018, The Astrophysical Journal.

[7]  A. Ginsburg,et al.  Investigating Fragmentation of Gas Structures in OB Cluster-forming Molecular Clump G33.92+0.11 with 1000 au Resolution Observations of ALMA , 2018, The Astrophysical Journal.

[8]  Lei Zhu,et al.  A First Look at BISTRO Observations of the ρ Oph-A core , 2018, 1804.09313.

[9]  Miguel de Val-Borro,et al.  The Astropy Project: Building an Open-science Project and Status of the v2.0 Core Package , 2018, The Astronomical Journal.

[10]  Hua-b. Li,et al.  Probing the Turbulence Dissipation Range and Magnetic Field Strengths in Molecular Clouds. II. Directly Probing the Ion–neutral Decoupling Scale , 2007, The Astrophysical Journal.

[11]  Saeko S. Hayashi,et al.  First Results from BISTRO: A SCUBA-2 Polarimeter Survey of the Gould Belt , 2017, 1704.08552.

[12]  Qizhou Zhang,et al.  MAGNETICALLY DOMINATED PARALLEL INTERSTELLAR FILAMENTS IN THE INFRARED DARK CLOUD G14.225-0.506 , 2016, 1609.08052.

[13]  E. Ostriker,et al.  ANISOTROPIC FORMATION OF MAGNETIZED CORES IN TURBULENT CLOUDS , 2015, 1508.02710.

[14]  H. Liu,et al.  ALMA resolves the spiraling accretion flow in the luminous OB cluster forming region G33.92+0.11 , 2015, 1505.04255.

[15]  Tokyo,et al.  REVEALING THE PHYSICAL PROPERTIES OF MOLECULAR GAS IN ORION WITH A LARGE-SCALE SURVEY IN J = 2–1 LINES OF 12CO, 13CO, AND C18O , 2014, 1412.0790.

[16]  P. Koch,et al.  THE IMPORTANCE OF THE MAGNETIC FIELD FROM AN SMA–CSO-COMBINED SAMPLE OF STAR-FORMING REGIONS , 2014, 1411.3830.

[17]  K. Dobashi,et al.  COLLIDING FILAMENTS AND A MASSIVE DENSE CORE IN THE CYGNUS OB 7 MOLECULAR CLOUD , 2014, 1411.0942.

[18]  D. Iono,et al.  CLUSTER FORMATION TRIGGERED BY FILAMENT COLLISIONS IN SERPENS SOUTH , 2014, 1407.1235.

[19]  L. Mundy,et al.  CARMA LARGE AREA STAR FORMATION SURVEY: OBSERVATIONAL ANALYSIS OF FILAMENTS IN THE SERPENS SOUTH MOLECULAR CLOUD , 2014, 1407.0755.

[20]  Qizhou Zhang,et al.  CORE AND FILAMENT FORMATION IN MAGNETIZED, SELF-GRAVITATING ISOTHERMAL LAYERS , 2014, 1405.1013.

[21]  E. Ostriker,et al.  FORMATION OF MAGNETIZED PRESTELLAR CORES WITH AMBIPOLAR DIFFUSION AND TURBULENCE , 2014, 1403.0582.

[22]  J. Pineda,et al.  MUSCLE W49: A MULTI-SCALE CONTINUUM AND LINE EXPLORATION OF THE MOST LUMINOUS STAR FORMATION REGION IN THE MILKY WAY. I. DATA AND THE MASS STRUCTURE OF THE GIANT MOLECULAR CLOUD , 2013, 1309.4129.

[23]  E. Vázquez-Semadeni,et al.  FILAMENTS IN SIMULATIONS OF MOLECULAR CLOUD FORMATION , 2013, 1308.6298.

[24]  P. Koch,et al.  INTERPRETING THE ROLE OF THE MAGNETIC FIELD FROM DUST POLARIZATION MAPS , 2013, 1308.6185.

[25]  P. Goldsmith,et al.  LOW VIRIAL PARAMETERS IN MOLECULAR CLOUDS: IMPLICATIONS FOR HIGH-MASS STAR FORMATION AND MAGNETIC FIELDS , 2013, 1308.5679.

[26]  Gildas Team,et al.  GILDAS: Grenoble Image and Line Data Analysis Software , 2013 .

[27]  G. Wilson,et al.  FILAMENTARY ACCRETION FLOWS IN THE EMBEDDED SERPENS SOUTH PROTOCLUSTER , 2013, 1301.6792.

[28]  G. Bruce Berriman,et al.  Astrophysics Source Code Library , 2012, ArXiv.

[29]  T. Robitaille,et al.  APLpy: Astronomical Plotting Library in Python , 2012 .

[30]  M. Tamura,et al.  NEAR-INFRARED-IMAGING POLARIMETRY TOWARD SERPENS SOUTH: REVEALING THE IMPORTANCE OF THE MAGNETIC FIELD , 2011, 1104.2977.

[31]  E. Ostriker,et al.  DENSE CORE FORMATION IN SUPERSONIC TURBULENT CONVERGING FLOWS , 2011, 1101.2650.

[32]  P. Myers FILAMENTARY STRUCTURE OF STAR-FORMING COMPLEXES , 2009, 0906.2005.

[33]  G. Fazio,et al.  A SPITZER SURVEY OF YOUNG STELLAR CLUSTERS WITHIN ONE KILOPARSEC OF THE SUN: CLUSTER CORE EXTRACTION AND BASIC STRUCTURAL ANALYSIS , 2009, 0906.0201.

[34]  Jessie L. Dotson,et al.  DISPERSION OF MAGNETIC FIELDS IN MOLECULAR CLOUDS. II. , 2008, 0909.5227.

[35]  Coleman Krawczyk,et al.  RE-EXAMINING LARSON'S SCALING RELATIONSHIPS IN GALACTIC MOLECULAR CLOUDS , 2008, 0809.1397.

[36]  Zhi-Yun Li,et al.  Magnetically Regulated Star Formation in Three Dimensions: The Case of the Taurus Molecular Cloud Complex , 2008, 0804.4201.

[37]  Gopal Narayanan,et al.  Large-Scale Structure of the Molecular Gas in Taurus Revealed by High Linear Dynamic Range Spectral Line Mapping , 2008, 0802.2206.

[38]  D. Ward-Thompson,et al.  SCUBA Polarization Measurements of the Magnetic Field Strengths in the L183, L1544, and L43 Prestellar Cores , 2003, astro-ph/0305604.

[39]  M. Reid,et al.  H I Absorption toward Ultracompact H II Regions: Distances and Galactic Structure , 2003 .

[40]  C. McKee,et al.  The Formation of Massive Stars from Turbulent Cores , 2002, astro-ph/0206037.

[41]  James M. Stone,et al.  Density, Velocity, and Magnetic Field Structure in Turbulent Molecular Cloud Models , 2000, astro-ph/0008454.

[42]  L. Mundy,et al.  Molecular Environments of Young Massive Stars: G34.26+0.15, G11.94–0.62, G33.92+0.11, and IRAS 18511+0146 , 1999 .

[43]  E. Ostriker,et al.  Dissipation in Compressible Magnetohydrodynamic Turbulence , 1998, astro-ph/9809357.