Mass and Radius Constraints Using Magnetar Giant Flare
- Slides: 14
Mass and Radius Constraints Using Magnetar Giant Flare Oscillations Alex T. Deibel With: Edward F. Brown (Michigan State University) Andrew W. Steiner (INT, University of Washington) HEAD Meeting 2013 Apr-8 -2013
Magnetar Giant Flares - QPOs • Giant flares triggered by crust reconfiguration • Modeled crust oscillations can be compared to QPOs Strohmayer & Watts 2006 Figure: Robert Duncan Deibel Apr-8 -2013
Crust composition • Nuclei crystal lattice • Neutron-rich nuclei • Degenerate electron and neutron gases • Magnetic field melts the crust and changes crust thickness Deibel, Steiner, and Brown 2013 (submitted) Deibel Apr-8 -2013
Perturbing the crust Bz ’ = 0 Surface Bz Outer Crust (Z, N), e Neutron Drip Inner Crust (Z, N), e, n Core ’ = 0 Deibel Apr-8 -2013
Assigning crust modes to QPO frequencies Equilibrium Nuclei Solve for Schumaker & Thorne 1983 Piro 2005 Samuelsson & Andersson 2007 Steiner & Watts 2009 = Deibel Apr-8 -2013
Constraining masses and radii EOS: Steiner et al. 2010 Deibel, Steiner, and Brown 2013 (submitted) Deibel Apr-8 -2013
Summary Choose a mass and radius from Steiner et al. EOS Find crust composition and shear modulus Integrate perturbation through the crust Compare eigenmodes to QPOs Magnetar masses and radii agree to within 1 with PREs and LMXBs from Steiner et al. 2010 Deibel Apr-8 -2013
Extras
Discovery of Magnetars • Class of pulsars with recurring gamma ray emission (SGRs) Getting the magnetic field: • Observe a pulsar’s period and spin-down rate • Assume a moment of inertia to get a dipole magnetic field Deibel Apr-8 -2013
Crust Modes • QPOs are torsional modes • Oscillations confined to the crust e t d ui rfl pe su us Cr er ph os m at • Crust modes will depend on crust composition Core 10 km 1 km Deibel Apr-8 -2013
Shell effects - Magic Numbers Dieperink 2009 Magnetic Field - Landau Quantization Deibel Apr-8 -2013
Model addition (1): Shell Effects No shell effects With shell effects Deibel Apr-8 -2013
Model addition (2): Magnetic Field B = 0. 0 G B = 2. 0· 1015 G Deibel Apr-8 -2013
Core equation of state 1. 5 M 1. 0 M Steiner, Lattimer, Brown 2010 Deibel Apr-8 -2013
- Flare in cavity preparation
- Magnetar
- Flare radius
- Trend of size in periodic table
- Outline form definition sturdevant
- Bloom and lens flare
- Civica app flare
- Tony camilli
- Modified double flare technique
- Supposing a snowmobile is equipped with a flare
- Avaya flare
- Temporal flare
- Anterior rib counterstrain
- Microdose flare protocol
- Convex contour symbol