Abstract

Planck observations at 353GHz provide the first fully-sampled maps of the polarized dust emission towards interstellar filaments and their backgrounds. The polarization data provide insight on the structure of their magnetic field (B). We present the polarization maps of three nearby star forming filament of moderate column density (NH~10^22cm^-2): Musca, B211, and L1506. We use the spatial information to separate Stokes I, Q, and U of the filaments from those of their backgrounds, an essential step to measure the intrinsic polarization fraction (p) and angle (psi) of each emission component. We find that the polarization angles in the three filaments (psi_fil) are coherent along their lengths and not the same as in their backgrounds (psi_bg). The differences between psi_fil and psi_bg are 12deg, 6deg, and 54deg for Musca, B211, and L1506, respectively. These differences for Musca and L1506 are larger than the dispersions of psi, both along the filaments and in their backgrounds. The observed changes of psi are direct evidence for variations of the orientation of the plane of the sky (POS) projection of the B-field. As in previous studies, we find a decrease of several percent of p with NH. We show that the drop in p cannot be explained by random fluctuations of the orientation of B within the filaments because they are too small (sigma_psi<10deg). We recognize the degeneracy between dust alignment efficiency and the structure of B in causing variations in p, but we argue that the decrease of p from the backgrounds to the filaments results in part from depolarization associated with the 3D structure of B: both its orientation in the POS and with respect to the POS. We do not resolve the inner structure of the filaments, but at the smallest scales accessible with Planck (~0.2pc), the observed changes of psi and p hold information on the B-field structure within filaments.

Highlights

  • The interstellar medium (ISM) has been observed to be filamentary for more than three decades

  • The regions that we study in this paper are within the regions of high signal-to-noise ratio (S/N), which are not masked in Planck Collaboration Int

  • We find that BPOS in the backgrounds of Musca and B211 are close, within 20◦, to being orthogonal to the filament crest, while for L1506, the background BPOS is at 37◦

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Summary

Introduction

The interstellar medium (ISM) has been observed to be filamentary for more than three decades. Filaments are striking features of Galactic images from the far-infrared/submm Herschel space observatory (André et al 2010; Motte et al 2010; Molinari et al 2010) They are ubiquitous both in the diffuse ISM and in star-forming molecular clouds, and the densest ones are observed to be associated with prestellar cores (e.g., Arzoumanian et al 2011; Palmeirim et al 2013; Konyves et al 2015). Planck Collaboration Int. XXXII (2016) identify interstellar filaments over the intermediate latitude sky, and present a statistical analysis of their orientation with respect to the component of the magnetic field on the POS (BPOS). We make use of the Planck polarization data to study the structure of the magnetic field within three fields comprising the archetypical examples of star-forming filaments of moderate column density: B211, L1506, and Musca. In Appendix A, we present a two-component model that applies as a first approximation to the polarized emission from interstellar filaments and their backgrounds

Planck observations
The filaments as seen by Planck
The Musca filament
The Taurus B211 filament
The Taurus L1506 filament
Polarized intensity and polarization fraction
Polarization properties
A two-component model: filament and background
Derivation of the polarization properties
Comparing the filament properties with that of their backgrounds
Interpretation of the polarization fraction
Mean magnetic field orientation
Fluctuation of the magnetic field orientation
Grain alignment efficiency and dust growth
Conclusions
Mean polarization angle along the LOS
Depolarization from rotation of the POS component of the magnetic field
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