Journal
ASTRONOMY & ASTROPHYSICS
Volume 644, Issue -, Pages -Publisher
EDP SCIENCES S A
DOI: 10.1051/0004-6361/202039081
Keywords
stars: protostars; protoplanetary disks; accretion, accretion disks; instabilities
Categories
Funding
- Austrian Science Fund (FWF) [I2549-N27]
- Swiss National Science Foundation (SNSF) [200021L_163172]
- Large Scientific Project of the Russian Ministry of Science and Higher Education Theoretical and experimental studies of the formation and evolution of extrasolar planetary systems and characteristics of exoplanets [075-15-2020-780, 780-10]
- Natural Sciences and Engineering Research Council (NSERC) of Canada
- Swiss National Science Foundation (SNF) [200021L_163172] Funding Source: Swiss National Science Foundation (SNF)
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Aims. Accretion bursts triggered by the magnetorotational instability (MRI) in the innermost disk regions were studied for protoplanetary gas-dust disks that formed from prestellar cores of a various mass M-core and mass-to-magnetic flux ratio lambda. Methods. Numerical magnetohydrodynamics simulations in the thin-disk limit were employed to study the long-term (similar to 1.0 Myr) evolution of protoplanetary disks with an adaptive turbulent alpha-parameter, which explicitly depends on the strength of the magnetic field and ionization fraction in the disk. The numerical models also feature the co-evolution of gas and dust, including the back-reaction of dust on gas and dust growth. Results. A dead zone with a low ionization fraction of x less than or similar to 10(-13) and temperature on the order of several hundred Kelvin forms in the inner disk soon after its formation, extending from several to several tens of astronomical units depending on the model. The dead zone features pronounced dust rings that are formed due to the concentration of grown dust particles in the local pressure maxima. Thermal ionization of alkaline metals in the dead zone trigger the MRI and associated accretion burst, which is characterized by a sharp rise, small-scale variability in the active phase, and fast decline once the inner MRI-active region is depleted of matter. The burst occurrence frequency is highest in the initial stages of disk formation and is driven by gravitational instability (GI), but it declines with diminishing disk mass-loading from the infalling envelope. There is a causal link between the initial burst activity and the strength of GI in the disk fueled by mass infall from the envelope. We find that the MRI-driven burst phenomenon occurs for lambda = 2-10, but diminishes in models with M-core less than or similar to M-circle dot, suggesting a lower limit on the stellar mass for which the MRI-triggered burst can occur. Conclusions. The MRI-triggered bursts occur for a wide range of mass-to-magnetic flux ratios and initial cloud core masses. The burst occurrence frequency is highest in the initial disk formation stage and reduces as the disk evolves from a gravitationally unstable to a viscous-dominated state. The MRI-triggered bursts are intrinsically connected with the dust rings in the inner disk regions, and both can be a manifestation of the same phenomenon, that is to say the formation of a dead zone.
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