Abstract

A physical mechanism that drives FU Orionis-type outbursts is reconsidered. We study the effect of the inner part of a circumstellar disk covering a region from near the central star to a radius of approximately 5 au (hereafter, the inner disk). Using the fluctuating mass accretion rate onto the inner disk |$\dot{M}\,_{\rm out}$|⁠, we consider the viscous evolution of the inner disk and the time variability of the mass accretion rate onto the central star |$\dot{M}\,_{\rm in}$| by means of numerical calculation of an unsteady viscous accretion disk in a one-dimensional axisymmetric model. First, we calculate the evolution of the inner disk assuming an oscillating |$\dot{M}\,_{\rm out}$|⁠. It is shown that the time variability of |$\dot{M}\,_{\rm in}$| does not coincide with |$\dot{M}\,_{\rm out}$| due to viscous diffusion. Second, we investigate the properties of spontaneous outbursts with temporally constant |$\dot{M}\,_{\rm out}$|⁠. Outbursts occur only in a limited range of mass accretion rates onto the inner disk of |$10^{-10}<\dot{M}\,_{\rm out}< 3\times 10^{-6}{\,M}_{\odot }\:$|yr−1 due to the gravo-magneto limit cycle (GML). Finally, we discuss the case with a combination of episodic |$\dot{M}\,_{\rm out}$| and accretion outbursts caused by the GML in the inner disk. The GML can drive accretion outbursts onto the star even for the case of fluctuating |$\dot{M}\,_{\rm out}$|⁠, although fluctuations of |$\dot{M}\,$| decay while transmitting the inner disk inwards. We have newly identified two modes of outburst, one spontaneous and one stimulated. In the stimulated mode of outburst, |$\dot{M}\,_{\rm out}$| does appear directly in |$\dot{M}\,_{\rm in}$| (the latter defining the stellar accretion luminosity). In the spontaneous mode of outburst, |$\dot{M}\,_{\rm out}$| appears as the interval between outbursts.

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