4.7 Article

The role of magnetic field geometry in the evolution of neutron star merger accretion discs

期刊

出版社

OXFORD UNIV PRESS
DOI: 10.1093/mnras/stz2552

关键词

accretion, accretion discs; stars: black holes; (stars:) gamma-ray burst: general; stars: jets

资金

  1. Natural Sciences and Engineering Research Council of Canada (NSERC) [RGPIN-2017-04286]
  2. Faculty of Science at the University of Alberta
  3. Simons Foundation
  4. Gordon and Betty Moore Foundation [GBMF5076]
  5. NASA [80NSSC18K0565]
  6. Office of Science of the U.S. Department of Energy [DE-AC02-05CH11231]

向作者/读者索取更多资源

Neutron star mergers are unique laboratories of accretion, ejection, and r-process nucleosynthesis. We used 3D general relativistic magnetohydrodynamic simulations to study the role of the post-merger magnetic geometry in the evolution of merger remnant discs around stationary Kerr black holes. Our simulations fully capture mass accretion, ejection, and jet production, owing to their exceptionally long duration exceeding 4 s. Poloidal post-merger magnetic field configurations produce jets with energies E-jet similar to (4-30) x 10(50) erg, isotropic equivalent energies E-iso similar to (4-20) x 10(52) erg, opening angles theta(jet) similar to 6-13 degrees, and durations t(j) less than or similar to 1 s. Accompanying the production of jets is the ejection of f(ej) similar to 30-40 per cent of the post-merger disc mass, continuing out to times >1 s. We discover that a more natural, purely toroidal post-merger magnetic field geometry generates large-scale poloidal magnetic flux of alternating polarity and striped jets. The first stripe, of E-jet similar to 2 x 10(48) erg, E-iso similar to 10(51) erg, theta(jet) similar to 3.5-5 degrees, and t(j) similar to 0.1 s, is followed by greater than or similar to 4 s of striped jet activity with f(ej) similar or equal to 27 per cent. The dissipation of such stripes could power the short-duration gamma-ray burst (sGRB) prompt emission. Our simulated jet energies and durations span the range of sGRBs. We find that although the blue kilonova component is initially hidden from view by the red component, it expands faster, outruns the red component, and becomes visible to off-axis observers. In comparison to GW 170817/GRB 170817A, our simulations underpredict the mass of the blue relative to red component by a factor of few. Including the dynamical ejecta and neutrino absorption may reduce this tension.

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