2025PASJ...77..277F


Query : 2025PASJ...77..277F

2025PASJ...77..277F - Publ. Astron. Soc. Jap., 77, 277-287 (2025/April-0)

A statistical approach to interpreting polarized dust emission of filamentary molecular clouds toward an estimate of 3D magnetic field structure.

FUKIHARA H., TAKAISHI D., MISUGI Y., SASAKI M. and TSUKAMOTO Y.

Abstract (from CDS):

In this study, we perform 3D magnetohydrodynamics (MHD) simulations of filamentary molecular clouds. We then generate synthetic observations based on the simulation results. Using these, we investigate how the new polarization data analysis method recently introduced by Doi et al. (2021, ApJ, 923, L9) reflects the magnetic field structure in turbulent filamentary molecular clouds. Doi et al. proposed that the $R_{\rm {FWHM}}$, the ratio of the full width at half maximum (FWHM) of the polarized intensity ($PI$) to that of the total intensity ($I$) can be used to probe the three-dimensional structure of the magnetic field. We calculate the $R_{\rm {FWHM}}$ from the density and magnetic field structure obtained in the 3D-MHD simulations. We find that the mean and variance of $R_{\rm {FWHM}}$ within a filament are smaller and larger, respectively, with a larger inclination of the magnetic field to the plane-of-sky. We also find that both small-scale ($\lt $0.1 pc) and large-scale ($\gtrsim$0.1 pc) turbulence affect the polarized intensity of the dust thermal emission. We conclude that future extensive observations of $R_{\rm {FWHM}}$ may be able to quantify the inclination of the magnetic field to the plane-of-sky in the filamentary molecular clouds.

Abstract Copyright: © The Author(s) 2025. Published by Oxford University Press on behalf of the Astronomical Society of Japan.

Journal keyword(s): magnetic fields - polarization - stars: formation

Simbad objects: 4

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Number of rows : 4
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 NGC 1333 OpC 03 29 09.2 +31 20 59           ~ 1575 1
2 Barnard 211 DNe 04 17 35 +27 43.1           ~ 141 0
3 LDN 1495 DNe 04 18.1 +27 37           ~ 408 1
4 M 16 OpC 18 18 45.1 -13 47 31           ~ 1084 1

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