Abstract

Abstract We investigate the internal 3D magnetic structure of dense interstellar filaments within NGC 1333 using polarization data at 850 μm from the B-fields In STar-forming Region Observations survey at the James Clerk Maxwell Telescope. Theoretical models predict that the magnetic field lines in a filament will tend to be dragged radially inward (i.e., pinched) toward the central axis due to the filament’s self-gravity. We study the cross-sectional profiles of the total intensity (I) and polarized intensity (PI) of dust emission in four segments of filaments unaffected by local star formation that are expected to retain a pristine magnetic field structure. We find that the filaments’ FWHMs in PI are not the same as those in I, with two segments being appreciably narrower in PI (FWHM ratio ≃0.7–0.8) and one segment being wider (FWHM ratio ≃1.3). The filament profiles of the polarization fraction (P) do not show a minimum at the spine of the filament, which is not in line with an anticorrelation between P and I normally seen in molecular clouds and protostellar cores. Dust grain alignment variation with density cannot reproduce the observed P distribution. We demonstrate numerically that the I and PI cross-sectional profiles of filaments in magnetohydrostatic equilibrium will have differing relative widths depending on the viewing angle. The observed variations of FWHM ratios in NGC 1333 are therefore consistent with models of pinched magnetic field structures inside filaments, especially if they are magnetically near-critical or supercritical.

Highlights

  • It is widely recognized that filaments in the interstellar medium (ISM) play an essential role in the star formation process (e.g., André et al 2014)

  • Crucial to observe the B-field in quiescent filaments before the onset of star formation to understand their dynamical importance in shaping these ubiquitous structures

  • We estimate the FWHM of the I and polarized intensity (PI) profiles with PI/δPI 3 by fitting 1D Gaussian profiles, which we show as blue dashed lines

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Summary

Introduction

It is widely recognized that filaments in the interstellar medium (ISM) play an essential role in the star formation process (e.g., André et al 2014). Theoretical studies indicate that the magnetic field (B-field hereafter) contributes to the evolution of these filaments (e.g., Hennebelle & Inutsuka 2019). It is, crucial to observe the B-field in quiescent filaments before the onset of star formation to understand their dynamical importance in shaping these ubiquitous structures. Field can be traced with polarimetric observations of the thermal continuum emission from interstellar dust particles (e.g., Hildebrand 1988). The thermal emission from so-aligned dust particles is polarized, and the polarization angle is perpendicular to the POS-projected B-field (Stein 1966; Hildebrand 1988)

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