4.6 Article

General-relativistic Simulations of Four States of Accretion onto Millisecond Pulsars

Journal

ASTROPHYSICAL JOURNAL LETTERS
Volume 851, Issue 2, Pages -

Publisher

IOP PUBLISHING LTD
DOI: 10.3847/2041-8213/aa9c85

Keywords

accretion, accretion disks; magnetohydrodynamics (MHD); pulsars: general; relativistic processes; stars: neutron; X-rays: binaries

Funding

  1. NASA [PF5-160142]
  2. TAC
  3. [NSF PHY-1125915]

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Accreting neutron stars can power a wide range of astrophysical phenomena including short-and long-duration gamma-ray bursts, ultra-luminous X-ray sources, and X-ray binaries. Numerical simulations are a valuable tool for studying the accretion-disk-magnetosphere interaction that is central to these problems, most clearly for the recently discovered transitional millisecond pulsars. However, magnetohydrodynamic (MHD) methods, widely used for simulating accretion, have difficulty in highly magnetized stellar magnetospheres, while force-free methods, suitable for such regions, cannot include the accreting gas. We present an MHD method that can stably evolve essentially force-free, highly magnetized regions, and describe the first time-dependent relativistic simulations of magnetized accretion onto millisecond pulsars. Our axisymmetric general-relativistic MHD simulations for the first time demonstrate how the interaction of a turbulent accretion flow with a pulsar's electromagnetic wind can lead to the transition of an isolated pulsar to the accreting state. This transition naturally leads to the formation of relativistic jets, whose power can greatly exceed the power of the isolated pulsar's wind. If the accretion rate is below a critical value, the pulsar instead expels the accretion stream. More generally, our simulations produce for the first time the four possible accretion regimes, in order of decreasing mass accretion rate: (a) crushed magnetosphere and direct accretion; (b) magnetically channeled accretion onto the stellar poles; (c) the propeller state, where material enters through the light cylinder but is prevented from accreting by the centrifugal barrier; (d) almost perfect exclusion of the accretion flow from the light cylinder by the pulsar wind.

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