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Collapsar Accretion and the Gamma-Ray Burst X-Ray Light Curve Chris Lindner Milos Milosavljevic, Sean M. Couch, Pawan Kumar
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Gamma Ray Bursts High Energy (foe) Highly Variable Two Types – Short Duration – Associated with compact object mergers – Long Duration – Associated with Core- Collapse supernova Observable in multiple wavelengths
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X-ray Light Curve Typically, long duration GRB exhibit 3 distinct phases in the first 10 3 s Phase 0 – 10 1 s – Prompt Phase Phase I – 10 2 s – Fast Decay Phase II – 10 3 s – Plateau Phase X-ray flares often occur in fast decay and plateau phase The x-ray light curve for GRB 050315 from Vaughan et al. 2006
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The Collapsar model Outer H layers stripped away off of a massive Wolf-Rayet progenitor Center of star collapses into a neutron star or black hole Rotation causes a disk (torus) to form Magnetic (?) Jets form and are able to push through the star Luminosity is modulated by central object accretion rate http://www.tls-tautenburg.de/research/klose/GRB.review.html Simulation from MacFadyen
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The Collapsar model: Questions Does the accretion history in the collapsar model actually mimic the variability in the X-ray light curve? If so, what causes the joined, distinct phases? Is there enough material to account for late time (> 10 3 - 10 4 s) activity? What is the source of viscosity in the accretion disk? MRI? Will jets actually form? Why? What causes X-ray flares? What is the mechanism of explosion? Jets? Neutrinos? Both?
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Kumar, Narayan, & Johnson 2008 Constructed an analytical model of collapsar accretion Use 14 solar mass progenitor star from Woosley & Heger 2006 Use a basic power law model for rotation profile Used α-model viscosity (α=.1) Compute onset of accretion shock (~10 2 s), a steep decline phase, and plateau phase
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Lindner, Milosavljevic, Couch, Kumar 2009 (Submitted to ApJ) 2D Hydrodynamic (HD) simulation of collapsar model using FLASH AMR HD code Start with same 14 Solar Mass Heger & Woosley model (16TI) WR – high rotation – low metalicity Use an explicit shear viscosity (modified α model) Set up a modified outflow inner boundary at (Rmin=5.0E7 to 2E8 cm) Ran simulations for up to 1000 s
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Lindner, Milosavljevic, Couch, Kumar 2009 (Submitted to ApJ) 2D Hydrodynamic (HD) simulation of collapsar model using FLASH AMR HD code Start with same 14 Solar Mass Heger & Woosley model (16TI) WR – high rotation – low metalicity Use an explicit shear viscosity (modified α model) Set up a modified outflow inner boundary at (Rmin=5.0E7 to 2E8 cm) Ran simulations for up to 1000 s
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Results: (play movies)
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Results: Mass Accretion
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Phase 0: Quasiradial accretion
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Phase I: Funnel and Thick Disk Accretion
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Phase II: Funnel Outflow, Thick Disk Accretion
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Future Work 2D MHD Simulations 3D Simulations – X-ray Flares? Jets and Neutrinos Early Universe Progenitors
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Conclusions The three initial phases of the GRB X-ray light curve fit well with the three phases of accretion history in the collapsar model – Phase 0: Quasiradial Accretion – Phase I: Funnel and Thick Disk Accretion – Phase II: Funnel Outflow, Thick Disk Accretion Future Work 2D MHD Simulations 3D Simulations – X-ray Flares? Jets and Neutrinos Early Universe Progenitors
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Pressure
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Gravity
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Pressure Gravity Magnetic Fields
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Pressure Gravity Magnetic Fields Radiation
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Basic Equations of Hydrodynamics Momentum Continuity: Conservation of Energy: Continuity of Mass: Poisson Equation:
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-Each grid point contains a full set of fluid variables -Hydrodynamic equations allow grid coordinates to ‘talk’ to each other
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