Synthetic Modeling of Polarized Dust Emission in Intermediate-mass Young Stellar Objects. II. Effects of Radiative Torque Disruption on Dust Grains in Protostellar Jets/ Outflows

One possible explanation for the presence of very large grains (VLGs) larger than 10 μm in the inner envelope of intermediate-mass Class 0/I young stellar objects is their migration from the protostellar disk via outflows. To assess whether RATD hinders this grain transport, we conducted numerical m...

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Detalles Bibliográficos
Autores: Giang, Nguyen Chau, Le Gouellec, Valentin J. M., Hoang, Thiem, Maury, Anaëlle, Hennebelle, Patrick
Tipo de recurso: artículo
Estado:Versión publicada
Fecha de publicación:2025
País:España
Institución:Consejo Superior de Investigaciones Científicas (CSIC)
Repositorio:DIGITAL.CSIC. Repositorio Institucional del CSIC
OAI Identifier:oai:digital.csic.es:10261/418865
Acceso en línea:http://hdl.handle.net/10261/418865
https://api.elsevier.com/content/abstract/scopus_id/105028424031
Access Level:acceso abierto
Palabra clave:Dust destruction
Dust physics
Circumstellar dust
http://astrothesaurus.org/uat/2268
http://astrothesaurus.org/uat/2229
http://astrothesaurus.org/uat/236
Descripción
Sumario:One possible explanation for the presence of very large grains (VLGs) larger than 10 μm in the inner envelope of intermediate-mass Class 0/I young stellar objects is their migration from the protostellar disk via outflows. To assess whether RATD hinders this grain transport, we conducted numerical modeling of RATD alongside grain dynamics, using gas velocity and density profiles from an MHD simulation of an intermediate Class 0 protostar. Our results show that, when the central luminosity Lcenter is ∼5L⊙, porous grains larger than 1 μm with tensile strengths Smax 10 10 erg cm 3 4 3 are efficiently destroyed by RATD at the outflow within ∼1 yr. This limits the outward migration of VLGs/submillimeter grains and leads submicron grains to dominate a few hundred astronomical unit inside the outflow cavity until Lcenter drops below <5L⊙. In contrast, Lcenter > 20L⊙ is required for RATD significantly affecting aggregate/composite grains with higher Smax 10 erg cm 5 3. We further incorporated RATD into POLARIS under the assumption that grains remain stationary. POLARIS accurately models the disruption for porous grains, but overestimates results for aggregate/composite grains at Lcenter = 100L⊙. At such high luminosities, the destruction of VLGs with Smax 10 10 erg cm 3 4 3 within the outflow cavity wall and inner envelope (after ∼20 yr) can reduce the observed polarization degree along the cavity wall by a factor of 2. However, RATD is not the dominant factor shaping dust polarization; magnetic inclusions, such as iron, play a more significant role.