Polarization Properties and Magnetic Field Structures in the High-mass Star-forming Region W51 Observed with ALMA

We present the first ALMA dust polarization observations toward the high-mass star-forming regions W51 e2, e8, and W51 North in Band 6 (230 GHz) with a resolution of about (∼5 mpc). Polarized emission in all three sources is clearly detected and resolved. Measured relative polarization levels are between 0.1% and 10%. While the absolute polarization shows complicated structures, the relative polarization displays the typical anticorrelation with Stokes I, although with a large scatter. Inferred magnetic (B) field morphologies are organized and connected. Detailed substructures are resolved, revealing new features such as comet-shaped B-field morphologies in satellite cores, symmetrically converging B-field zones, and possibly streamlined morphologies. The local B-field dispersion shows some anticorrelation with the relative polarization. Moreover, the lowest polarization percentages together with largest dispersions coincide with B-field convergence zones. We put forward , where ω is the measurable angle between a local B-field orientation and local gravity, as a measure of how effectively the B field can oppose gravity. Maps of for all three sources show organized structures that suggest a locally varying role of the B field, with some regions where gravity can largely act unaffectedly, possibly in a network of narrow magnetic channels, and other regions where the B field can work maximally against gravity.

[1]  A. Ginsburg,et al.  Thermal Feedback in the High-mass Star- and Cluster-forming Region W51 , 2017, 1704.01434.

[2]  A. Ginsburg A review of the W51 Cloud , 2017, 1702.06627.

[3]  A. Lazarian,et al.  A UNIFIED MODEL OF GRAIN ALIGNMENT: RADIATIVE ALIGNMENT OF INTERSTELLAR GRAINS WITH MAGNETIC INCLUSIONS , 2016, 1605.02828.

[4]  R. Paladino,et al.  ALMA SCIENCE VERIFICATION DATA: MILLIMETER CONTINUUM POLARIMETRY OF THE BRIGHT RADIO QUASAR 3C 286 , 2016, 1605.00051.

[5]  A. Ginsburg,et al.  Hot ammonia around young O-type stars. III. High-mass star formation and hot core activity in W51~Main , 2016, 1601.05733.

[6]  Enzo Pascale,et al.  BALLOON-BORNE SUBMILLIMETER POLARIMETRY OF THE VELA C MOLECULAR CLOUD: SYSTEMATIC DEPENDENCE OF POLARIZATION FRACTION ON COLUMN DENSITY AND LOCAL POLARIZATION-ANGLE DISPERSION , 2015, 1509.05298.

[7]  John E. Vaillancourt,et al.  Interstellar Dust Grain Alignment , 2015 .

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

[9]  Qizhou Zhang,et al.  Hot ammonia around young O-type stars - II. JVLA imaging of highly excited metastable NH3 masers in W51-North , 2014, 1411.1075.

[10]  P. Koch,et al.  MAGNETIC FIELDS AND MASSIVE STAR FORMATION , 2014, Proceedings of the International Astronomical Union.

[11]  G. W. Pratt,et al.  Planck intermediate results. XX. Comparison of polarized thermal emission from Galactic dust with simulations of MHD turbulence , 2014, 1405.0872.

[12]  G. W. Pratt,et al.  Planck intermediate results. XIX. An overview of the polarized thermal emission from Galactic dust , 2014, 1405.0871.

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

[14]  Q. Minor BINARY POPULATIONS IN MILKY WAY SATELLITE GALAXIES: CONSTRAINTS FROM MULTI-EPOCH DATA IN THE CARINA, FORNAX, SCULPTOR, AND SEXTANS DWARF SPHEROIDAL GALAXIES , 2013, 1302.0302.

[15]  P. Koch,et al.  DUST CONTINUUM AND POLARIZATION FROM ENVELOPE TO CORES IN STAR FORMATION: A CASE STUDY IN THE W51 NORTH REGION , 2012, 1212.0656.

[16]  C. Henkel,et al.  Ammonia in the hot core W 51-IRS2: 11 new maser lines and a maser component with a velocity drift , 2012, 1211.2484.

[17]  G. Fuller,et al.  Methanol and excited OH masers towards W51: I - Main and South , 2012, 1203.2527.

[18]  P. Koch,et al.  MAGNETIC FIELD STRENGTH MAPS FOR MOLECULAR CLOUDS: A NEW METHOD BASED ON A POLARIZATION–INTENSITY GRADIENT RELATION , 2012, 1201.4263.

[19]  P. Koch,et al.  QUANTIFYING THE SIGNIFICANCE OF THE MAGNETIC FIELD FROM LARGE-SCALE CLOUD TO COLLAPSING CORE: SELF-SIMILARITY, MASS-TO-FLUX RATIO, AND STAR FORMATION EFFICIENCY , 2012, 1201.4313.

[20]  K. Menten,et al.  TRIGONOMETRIC PARALLAX OF W51 MAIN/SOUTH , 2010, 1006.4218.

[21]  J. Han,et al.  A BIPOLAR OUTFLOW FROM THE MASSIVE PROTOSTELLAR CORE W51e2-E , 2010, 1006.4058.

[22]  Jessie L. Dotson,et al.  350 μm POLARIMETRY FROM THE CALTECH SUBMILLIMETER OBSERVATORY , 2010, 1001.2790.

[23]  J. Han,et al.  NATURE OF W51e2: MASSIVE CORES AT DIFFERENT PHASES OF STAR FORMATION , 2010, 1001.1101.

[24]  P. Koch,et al.  EVOLUTION OF MAGNETIC FIELDS IN HIGH-MASS STAR FORMATION: LINKING FIELD GEOMETRY AND COLLAPSE FOR THE W51 e2/e8 CORES , 2009, 0905.1996.

[25]  Brenda C. Matthews,et al.  THE LEGACY OF SCUPOL: 850 μm IMAGING POLARIMETRY FROM 1997 TO 2005 , 2009 .

[26]  K. Menten,et al.  A RING/DISK/OUTFLOW SYSTEM ASSOCIATED WITH W51 NORTH: A VERY MASSIVE STAR IN THE MAKING , 2009, 0904.0325.

[27]  K. Menten,et al.  TRIGONOMETRIC PARALLAXES OF MASSIVE STAR-FORMING REGIONS: III. G59.7+0.1 AND W 51 IRS2 , 2008, 0811.0701.

[28]  E. Keto,et al.  The Ionization of Accretion Flows in High-Mass Star Formation: W51e2 , 2008, 0804.0514.

[29]  K. Menten,et al.  Forming an early O-type star through gas accretion? , 2007, 0711.4941.

[30]  M. Reid,et al.  THE ASTROPHYSICAL JOURNAL Preprint typeset using LATEX style emulateapj v. 10/09/06 PROPER MOTIONS OF OH MASERS AND MAGNETIC FIELDS IN MASSIVE STAR-FORMING REGIONS , 2007 .

[31]  A. Lazarian,et al.  Radiative torques: analytical model and basic properties , 2007, 0707.0886.

[32]  A. Lazarian,et al.  Grain Alignment by Radiation in Dark Clouds and Cores , 2005, astro-ph/0505571.

[33]  Qizhou Zhang,et al.  The Case for Local Collapse in the W51 Star-forming Region , 2004 .

[34]  J. Nakajima,et al.  3-D Kinematics of Water Masers in the W 51A Region , 2002, astro-ph/0207648.

[35]  J. Hough,et al.  The magnetic field structure in W51A , 2002, astro-ph/0201499.

[36]  K. Menten,et al.  Outflow 20-2000 AU from a High-Mass Protostar in W51-IRS 2 , 2001, astro-ph/0112093.

[37]  J. Girart,et al.  Interferometric Mapping of Magnetic Fields in Star-forming Regions. I. W51 e1/e2 Molecular Cores , 2000, astro-ph/0107322.

[38]  A. Lazarian Physics of Grain Alignment , 2000, astro-ph/0003314.

[39]  P. Ho,et al.  Radiative Transfer Modeling of the Accretion Flow onto a Star-forming Core in W51 , 1998, astro-ph/9806058.

[40]  Qizhou Zhang,et al.  Dynamical Collapse in W51 Massive Cores: CS (3-2) and CH3CN Observations , 1998 .

[41]  Qizhou Zhang,et al.  Dynamical Collapse in W51 Massive Cores: NH3 Observations , 1997 .

[42]  P. Ho,et al.  The Contracting Molecular Cores e1 and e2 in W51 , 1996 .

[43]  J. Weingartner,et al.  Radiative Torques on Interstellar Grains. II. Grain Alignment , 1996, astro-ph/9611149.

[44]  J. Weingartner,et al.  Radiative Torques on Interstellar Grains: I. Superthermal Spinup , 1996, astro-ph/9605046.

[45]  D. Mehringer Radio Continuum and Radio Recombination Line Observations of W51 , 1994 .

[46]  Ronald D. Brown,et al.  Pumping the Interstellar (6,3) Ammonia Maser , 1991 .

[47]  Giles A Novak,et al.  Detection of submillimeter polarization in the Orion nebula , 1984 .

[48]  W. Cudlip,et al.  Far infrared polarimetry of W51A and M42 , 1982 .

[49]  M. Reid,et al.  Proper motions and distances of H2O maser sources. III - W51NORTH , 1981 .

[50]  J. Wardle,et al.  The linear polarization of quasi-stellar radio sources at 3.71 and 11.1 centimeters. , 1974 .

[51]  A. Martin High Resolution Observations of W51 , 1972 .

[52]  Enrico Fermi,et al.  Magnetic fields in spiral arms , 1953 .

[53]  R. B. Barreiro,et al.  Planck intermediate results IV , 2022 .