Multiscale Synthetic observations of Polarized dust emission: On the origin of Depolarization effect from Molecular clouds to Starless cores and Constraints on Dust Physics
astro-ph.GA
Submitted: 2026-08-30
Updated: 2026-08-30
Comments: Accepted to be published in ApJ. 24 pages, 11 figures in Main text, 8 pages in Appendix
License: http://creativecommons.org/licenses/by/4.0/
The gist: Submillimeter observations of polarized dust emission from molecular clouds to starless cores frequently report a decrease in polarization fraction (p) with increasing dust emission intensity (I).
Terminology
Abstract
Submillimeter observations of polarized dust emission from molecular clouds to starless cores frequently report a decrease in polarization fraction (p) with increasing dust emission intensity (I). This feature is commonly attributed to the alignment loss of dust grains or the geometrical effects of magnetic fields, yet, the detailed contributions remain unclear. To investigate the mechanism responsible for the depolarization, we use POLARIS to perform the multiscale synthetic dust polarization observations at 850μm from magnetically aligned dust grains by RAdiative Torques (RATs) mechanism. We adopt three collapsing cloud models with different magnetic energy levels and explore the effects of grain magnetic properties and grain growth on dust polarization. The field geometrical effect is the dominant depolarization mechanism at N H<10 21-10 22 cm-2. We find that if grains grow beyond >0.5μm and are superparamagnetic (SPM) with large iron clusters, RATs remain effective at high column densities, and grain alignment loss contributes to depolarization only at N H > 10 23 cm-2. If neither of these conditions is satisfied, the alignment loss (in cases of insufficient grain growth); or the reduced grain alignment efficiency by gaseous damping (for paramagnetic grains or SPM grains with small iron cluster sizes) can become the dominant depolarization mechanism at N H > 10 22 cm-2, regardless of how tangled the magnetic field lines in our simulation. Finally, we show that the depolarization mechanism and the underlying dust physical properties inside starless cores may be identified through the p-I slope and the mean p at the core center.
Sources
- Pristine composition or size evolution: Can current dust models reproduce emissivities observed in nearby protostars?
- The JCMT BISTRO Survey: The Magnetic Fields of the IC 348 Star-forming Region
- Effects of Grain Magnetic Properties and Grain Growth on Synthetic Dust Polarization of MHD Simulations in Protostellar Environments
- The radiative torque spin-up efficiency of ballistic dust grain aggregates
- Magnetic fields in star formation: from clouds to cores
- The role of magnetic fields in the formation of protostars, disks, and outflows
- Synthetic observations using POLARIS: an application to simulations of massive prestellar cores
Related papers
- Apparent Stability in Self-Gravitating Turbulence and the Evolution of Molecular Clouds
- Two sets of potential-density basis pairs for the study of radial perturbations in collisionless spherical stellar systems
- Constraining reionization-era Ly alpha escape with JELS-MUSE: a highly complete H alpha-selected sample at z about6.1
- Deriving volume density profiles of filaments from observed surface densities
- Little Red Dots and Supermassive Black Hole Seed Formation in Ultralight Dark Matter Halos
- MEGATRON: how the first stars can create an iron metallicity plateau in the smallest dwarf galaxies