Abstract

We show that thin accretion disks made of carbon or oxygen are subject to the same thermal ionization instability as hydrogen and helium disks. We argue that the instability applies to disks of any metal content. The relevance of the instability to supernova fallback disks probably means that their power-law evolution breaks down when they first become neutral. We construct simple analytical models for the viscous evolution of fallback disks to show that it is possible for these disks to become neutral when they are still young (ages of a few 103 to 104 yr), compact in size (a few 109 to 1011 cm) and generally accreting at sub-Eddington rates ( ~ a few 1014-1018 g s-1). Based on recent results on the nature of viscosity in the disks of close binaries, we argue that this time may also correspond to the end of the disk activity period. Indeed, in the absence of a significant source of viscosity in the neutral phase, the entire disk will likely turn to dust and become passive. We discuss various applications of the evolutionary model, including anomalous X-ray pulsars and young radio pulsars. Our analysis indicates that metal-rich fallback disks around newly born neutron stars and black holes become neutral generally inside the tidal truncation radius (Roche limit) for planets at ≈1011 cm. Consequently, the efficiency of the planetary formation process in this context will mostly depend on the ability of the resulting disk of rocks to spread via collisions beyond the Roche limit. It appears easier for the merger product of a doubly degenerate binary, whether it is a massive white dwarf or a neutron star, to harbor planets because its remnant disk has a rather large initial angular momentum, which allows it to spread beyond the Roche limit before becoming neutral. The early super-Eddington phase of accretion is a source of uncertainty for the disk evolution models presented here.

Highlights

  • Fallback is a standard ingredient of contemporary core-collapse supernova scenarios

  • Chatterjee et al find that, depending on the initial values of the neutron star spin period, magnetic field strength and disk mass, a system can evolve into an X-ray luminous Anomalous X-ray Pulsars (AXPs), where the neutron star has been substantially slowed down by the torque exerted by the disk during a long propeller phase, or into a radio pulsar which did not interact as strongly with its surrounding disk

  • One of the shortcomings of the Chatterjee et al model for AXPs is the necessity to postulate that the end of the activity period for the fallback disk corresponds to a transition to a radiatively inefficient Advection-Dominated Accretion Flow (ADAF; see Narayan, Mahadevan & Quataert 1998 for a review)

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Summary

Introduction

Fallback is a standard ingredient of contemporary core-collapse supernova scenarios. It occurs when the reverse shock, triggered by the impact of the ejected core material against the stellar envelope, reaches the central compact object (Colgate 1988; Chevalier 1989; see, e.g., Fryer & Heger 2000 for recent core-collapse numerical simulations). Woosley & Bodenheimer (1991) considered the evolution of a fallback disk in more detail, with a particular emphasis on the planetary formation process around young neutron stars. Chatterjee, Hernquist & Narayan (2000) developed a model for Anomalous X-ray Pulsars (AXPs) based on the viscous evolution of a fallback disk and its magnetospheric interaction with the newly-formed neutron star. Chatterjee, Hernquist & Narayan (2000) developed a model for Anomalous X-ray Pulsars (AXPs) based on the viscous evolution of a fallback disk and its magnetospheric interaction with the newly-formed neutron star. Alpar (1999, 2000) presents an accretion scenario for AXPs. Marsden, Lingenfelter & Rothschild (2001a; see Marsden, Lingenfelter & Rothschild 2001b) have recently considered the effect of fallback disks on the spin evolution of radio pulsars

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