B-fields and Dust in Interstellar Filaments Using Dust Polarization (BALLAD-POL). II. Testing the Radiative Torque Paradigm in Musca and OMC-1

Abstract Polarization of starlight and thermal dust emission caused by aligned dust grains is a valuable tool to characterize magnetic fields ( B -fields) and constrain dust properties. However, the grain alignment physics is not fully understood. To test the radiative torque (RAT) paradigm, including RAT alignment (RAT-A) and disruption (RAT-D), we use dust polarization observed by Planck and Stratosphere Observatory for Infrared Astronomy/High-resolution Airborne Wideband Camera Plus toward two filaments, Musca and OMC-1, with contrasting physical conditions. Musca, a quiescent filament, is ideal for testing RAT-A, while OMC-1, an active star-forming region OMC-1, is most suitable for testing RAT-D. We found that polarization fraction, P , decreases with increasing polarization angle dispersion function, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi class="MJX-tex-calligraphic" mathvariant="script">S</mml:mi> </mml:math> , and increasing column density, N (H 2 ), consistent with RAT-A. However, P increases with increasing dust temperature, T d , but decreases when T d reaches a certain high value. We compute the polarization fraction for the ideal models with B -fields in the plane of sky based on the RAT paradigm, accounting for the depolarization effect by B -field tangling. We then compare the realistic polarization model with observations. For Musca with well-ordered B -fields, our numerical model successfully reproduces the decline of P toward the filament spine (aka polarization hole), having higher N (H 2 ) and lower T d , indicating the loss of grain alignment efficiency due to RAT-A. For OMC-1, with stronger B -field variations and higher temperatures, our model can reproduce the observed P – T d and P − N (H 2 ) relations only if the B -field tangling and RAT-D effect are incorporated. Our results provide more robust observational evidence for the RAT paradigm, particularly the recently discovered RAT-D.

Authors

Publication Details

Journal
The Astrophysical Journal
Published
2024-10-01
DOI
https://doi.org/10.3847/1538-4357/ad6a5e
Citations
6
Primary Topic
Astrophysics and Star Formation Studies
Type
article
Field-Weighted Citation Impact
1.99

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article

B-fields and Dust in Interstellar Filaments Using Dust Polarization (BALLAD-POL). II. Testing the Radiative Torque Paradigm in Musca and OMC-1

Thiem Hoang, Nguyen Bich Ngoc, Pham Ngoc Diep, Le Ngoc Tram
6 citations
The Astrophysical Journal
Astrophysics and Star Formation Studies
1.99
article

B-fields and Dust in Interstellar Filaments Using Dust Polarization (BALLAD-POL). II. Testing the Radiative Torque Paradigm in Musca and OMC-1

Thiem Hoang, Nguyen Bich Ngoc, Pham Ngoc Diep, Le Ngoc Tram
article en
6 citations

Abstract

Abstract Polarization of starlight and thermal dust emission caused by aligned dust grains is a valuable tool to characterize magnetic fields ( B -fields) and constrain dust properties. However, the grain alignment physics is not fully understood. To test the radiative torque (RAT) paradigm, including RAT alignment (RAT-A) and disruption (RAT-D), we use dust polarization observed by Planck and Stratosphere Observatory for Infrared Astronomy/High-resolution Airborne Wideband Camera Plus toward two filaments, Musca and OMC-1, with contrasting physical conditions. Musca, a quiescent filament, is ideal for testing RAT-A, while OMC-1, an active star-forming region OMC-1, is most suitable for testing RAT-D. We found that polarization fraction, P , decreases with increasing polarization angle dispersion function, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi class="MJX-tex-calligraphic" mathvariant="script">S</mml:mi> </mml:math> , and increasing column density, N (H 2 ), consistent with RAT-A. However, P increases with increasing dust temperature, T d , but decreases when T d reaches a certain high value. We compute the polarization fraction for the ideal models with B -fields in the plane of sky based on the RAT paradigm, accounting for the depolarization effect by B -field tangling. We then compare the realistic polarization model with observations. For Musca with well-ordered B -fields, our numerical model successfully reproduces the decline of P toward the filament spine (aka polarization hole), having higher N (H 2 ) and lower T d , indicating the loss of grain alignment efficiency due to RAT-A. For OMC-1, with stronger B -field variations and higher temperatures, our model can reproduce the observed P – T d and P − N (H 2 ) relations only if the B -field tangling and RAT-D effect are incorporated. Our results provide more robust observational evidence for the RAT paradigm, particularly the recently discovered RAT-D.

The Astrophysical JournalVol. 974(1)
Simons Foundation, Quỹ Đổi mới sáng tạo Vingroup
Openalex Percentile: Top 14%
Astrophysics and Star Formation Studies
1.99
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