2023ApJ...945..160L


Query : 2023ApJ...945..160L

2023ApJ...945..160L - Astrophys. J., 945, 160 (2023/March-2)

Multi-scale Physical Properties of NGC 6334 as Revealed by Local Relative Orientations between Magnetic Fields, Density Gradients, Velocity Gradients, and Gravity.

LIU J., ZHANG Q., KOCH P.M., LIU H.B., LI Z.-Y., LI S., GIRART J.M., CHEN H.-R.V., CHING T.-C., HO P.T.P., LAI S.-P., QIU K., RAO R. and TANG Y.-W.

Abstract (from CDS):

We present ALMA dust polarization and molecular line observations toward four clumps (I(N), I, IV, and V) in the massive star-forming region NGC 6334. In conjunction with large-scale dust polarization and molecular line data from JCMT, Planck, and NANTEN2, we make a synergistic analysis of relative orientations between magnetic fields (θB), column density gradients (θNG), local gravity (θLG), and velocity gradients (θVG) to investigate the multi-scale (from ∼30 to 0.003 pc) physical properties in NGC 6334. We find that the relative orientation between θB and θNG changes from statistically more perpendicular to parallel as column density (${N}_{{{\rm{H}}}_{2}}$) increases, which is a signature of trans-to-sub-Alfvénic turbulence at complex/cloud scales as revealed by previous numerical studies. Because θNG and θLG are preferentially aligned within the NGC 6334 cloud, we suggest that the more parallel alignment between θB and θNG at higher ${N}_{{{\rm{H}}}_{2}}$ is because the magnetic field line is dragged by gravity. At even higher ${N}_{{{\rm{H}}}_{2}}$, the angle between θB and θNG or θLG transits back to having no preferred orientation, or statistically slightly more perpendicular, suggesting that the magnetic field structure is impacted by star formation activities. A statistically more perpendicular alignment is found between θB and θVG throughout our studied ${N}_{{{\rm{H}}}_{2}}$ range, which indicates a trans-to-sub-Alfvénic state at small scales as well, and this signifies that magnetic field has an important role in the star formation process in NGC 6334. The normalized mass-to-flux ratio derived from the polarization-intensity gradient (KTH) method increases with ${N}_{{{\rm{H}}}_{2}}$, but the KTH method may fail at high ${N}_{{{\rm{H}}}_{2}}$ due to the impact of star formation feedback.

Abstract Copyright: © 2023. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Polarimetry - Magnetic fields - Star formation - Molecular clouds - Interstellar medium

Simbad objects: 10

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Number of rows : 10
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NAME NGC 6334 FIR V Cl* 17 19 57 -35 57.5           ~ 99 0
2 NAME NGC 6334-IV Cl* 17 20 17 -35 54.9           ~ 48 1
3 NGC 6334 HII 17 20 53 -36 07.9           ~ 740 0
4 NAME NGC 6334-I Cl* 17 20 53.35 -35 47 01.5           ~ 373 0
5 NAME NGC 6334 I(N) smm 17 20 54 -35 45.0           ~ 165 1
6 PMN J1733-3722 Rad 17 33 15.1930935 -37 22 32.398009           ~ 56 1
7 4C 09.57 BLL 17 51 32.81857326 +09 39 00.7284066   17.46 16.78 15.57   ~ 1007 1
8 QSO J1851+005 QSO 18 51 46.72295 +00 35 32.3649           ~ 138 1
9 QSO B1921-293 BLL 19 24 51.05595254 -29 14 30.1210248   18.71 18.21 15.07   ~ 918 1
10 NAME Gould Belt PoG ~ ~           ~ 956 1

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