Knotty protostellar jets as a signature of episodic protostellar accretion?

TL;DR

This study links knotty jet structures in a young protostar to episodic accretion events, using simulations and observations to suggest that jet knots reflect underlying accretion burst patterns.

Contribution

It demonstrates that the observed knot spacings in CARMA 7's jet can be explained by episodic accretion bursts in gravitationally unstable disks, with model-observation alignment suggesting specific inclination angles.

Findings

Model bursts show bi-modal time spacing distribution.

Jet knot spacings can be matched to accretion bursts with inclination correction.

Best-fit inclination angles are between 55-80 degrees.

Abstract

We aim at studying the causal link between the knotty jet structure in CARMA 7, a young Class 0 protostar in the Serpens South cluster, and episodic accretion in young protostellar disks. We used numerical hydrodynamics simulations to derive the protostellar accretion history in gravitationally unstable disks around solar-mass protostars. We compared the time spacing between luminosity bursts \Delta\tau_mod, caused by dense clumps spiralling on the protostar, with the differences of dynamical timescales between the knots \Delta\tau_obs in CARMA 7. We found that the time spacing between the bursts have a bi-modal distribution caused by isolated and clustered luminosity bursts. The former are characterized by long quiescent periods between the bursts with \Delta\tau_mod = a few * (10^3-10^4) yr, whereas the latter occur in small groups with time spacing between the bursts \Delta\tau_mod= a few * (10-10^2) yr. For the clustered bursts, the distribution of \Delta\tau_mod in our models can be fit reasonably well to the distribution of \Delta\tau_obs in the protostellar jet of CARMA 7, if a certain correction for the (yet unknown) inclination angle with respect to the line of sight is applied. The K-S test on the model and observational data sets suggests the best-fit values for the inclination angles of 55-80 deg., which become narrower (75-80 deg.) if only strong luminosity bursts are considered. The dynamical timescales of the knots in the jet of CARMA 7 are too short for a meaningful comparison with the long time spacings between isolated bursts in our models. The exact sequences of time spacings between the luminosity bursts in our models and knots in the jet of CARMA 7 were found difficult to match. (abridged)