info:eu-repo/semantics/article
The Maser-emitting Structure and Time Variability of the SiS Lines J = 14-13 and 15-14 in IRC+10216
Fecha
2018-06Registro en:
Fonfra, J. P.; Fernandez Lopez, Manuel; Pardo, J. R.; Agúndez, M.; Sánchez Contreras, C.; et al.; The Maser-emitting Structure and Time Variability of the SiS Lines J = 14-13 and 15-14 in IRC+10216; IOP Publishing; Astrophysical Journal; 860; 2; 6-2018; 1-18
0004-637X
CONICET Digital
CONICET
Autor
Fonfra, J. P.
Fernandez Lopez, Manuel
Pardo, J. R.
Agúndez, M.
Sánchez Contreras, C.
Velilla Prieto, L.
Cernicharo, J.
Santander García, M.
Quintana Lacaci, G.
Castro Carrizo, A.
Curiel, S.
Resumen
We present new high angular resolution interferometer observations of the v = 0 J = 14-13 and 15-14 SiS lines toward IRC+10216, carried out with the Combined Array for Research in Millimeter-wave Astronomy and the Atacama Large Millimeter Array. The maps, with angular resolutions of ≃0.″25 and 0.″55, reveal (1) an extended, roughly uniform, and weak emission with a size of ≃0.″5; (2) a component elongated approximately along the east-west direction peaking at ≃0.″13 and 0.″17 at both sides of the central star; and (3) two blue- and redshifted compact components peaking around 0.″07 to the NW of the star. We have modeled the emission with a 3D radiation transfer code, finding that the observations cannot be explained only by thermal emission. Several maser clumps and one arc-shaped maser feature arranged from 5 to 20 from the central star, in addition to a thin shell-like maser structure at ≃13 , are required to explain the observations. This maser-emitting set of structures accounts for 75% of the total emission, while the other 25% is produced by thermally excited molecules. About 60% of the maser emission comes from the extended emission, and the rest comes from the set of clumps and the arc. The analysis of a time monitoring of these and other SiS and 29SiS lines carried out with the IRAM 30 m telescope from 2015 to present suggests that the intensity of some spectral components of the maser emission strongly depends on the stellar pulsation, while other components show a mild variability. This monitoring evidences a significant phase lag of ≃0.2 between the maser and near-IR light curves.