mass and radius constraints using magnetar giant flare oscillations

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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) QuickTime™ and a decompressor are needed to see thi HEAD Meeting 2013 Apr-8-2013

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Alex T. Deibel. Mass and Radius Constraints Using Magnetar Giant Flare Oscillations. 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 - PowerPoint PPT Presentation

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Page 1: Mass and Radius Constraints Using Magnetar Giant Flare Oscillations

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)

QuickTime™ and a decompressor

are needed to see this picture.

HEAD Meeting 2013 Apr-8-2013

Page 2: Mass and Radius Constraints Using Magnetar Giant Flare Oscillations

QuickTime™ and a decompressor

are needed to see this picture.

• Giant flares triggered by

crust reconfiguration

• Modeled crust oscillations

can be compared to

QPOs

Strohmayer & Watts 2006 Figure: Robert Duncan

Deibel Apr-8-2013

Magnetar Giant Flares - QPOs

Page 3: Mass and Radius Constraints Using Magnetar Giant Flare Oscillations

Deibel, Steiner, and Brown 2013 (submitted) Deibel Apr-8-2013

• Nuclei crystal lattice

• Neutron-rich nuclei

• Degenerate electron and neutron gases

• Magnetic field melts the crust and changes crust thickness

Crust composition

Page 4: Mass and Radius Constraints Using Magnetar Giant Flare Oscillations

Deibel Apr-8-2013

BzBzSurface

Core

Neutron Drip

Outer Crust (Z, N), e

Inner Crust (Z, N), e, n

’ = 0

’ = 0

Perturbing the crust

Page 5: Mass and Radius Constraints Using Magnetar Giant Flare Oscillations

Equilibrium Nuclei

Deibel Apr-8-2013

Solve for

=

Schumaker & Thorne 1983Piro 2005Samuelsson & Andersson 2007Steiner & Watts 2009

Assigning crust modes to QPO frequencies

Page 6: Mass and Radius Constraints Using Magnetar Giant Flare Oscillations

Constraining masses and radii

Deibel Apr-8-2013EOS: Steiner et al. 2010Deibel, Steiner, and Brown 2013 (submitted)

Page 7: Mass and Radius Constraints Using Magnetar Giant Flare Oscillations

Summary

Choose a mass and radius from Steiner et al. EOS

Integrate perturbation through the crust

Compare eigenmodes to QPOs

Magnetar masses and radii agree to within 1with PREs and LMXBs from Steiner et al. 2010

Deibel Apr-8-2013

Find crust composition and shear modulus

Page 8: Mass and Radius Constraints Using Magnetar Giant Flare Oscillations

Extras

Page 9: Mass and Radius Constraints Using Magnetar Giant Flare Oscillations

Discovery of Magnetars

• Class of pulsars with recurringgamma ray emission (SGRs)

Getting the magnetic field:• Observe a pulsar’s period and

spin-down rate

• Assume a moment of inertiato get a dipole magnetic field

Deibel Apr-8-2013

Page 10: Mass and Radius Constraints Using Magnetar Giant Flare Oscillations

10 km 1 km

Core

Crustsuperfluidatm

osphere

Deibel Apr-8-2013

• QPOs are torsional modes

• Oscillations confined to the crust

• Crust modes will depend on crust composition

Crust Modes

Page 11: Mass and Radius Constraints Using Magnetar Giant Flare Oscillations

Shell effects

Deibel Apr-8-2013

Magnetic Field- Landau Quantization

- Magic Numbers

Dieperink 2009

Page 12: Mass and Radius Constraints Using Magnetar Giant Flare Oscillations

With shell effectsNo shell effects

Deibel Apr-8-2013

Model addition (1): Shell Effects

Page 13: Mass and Radius Constraints Using Magnetar Giant Flare Oscillations

B = 0.0 G B = 2.0·1015 G

Deibel Apr-8-2013

Model addition (2): Magnetic Field

Page 14: Mass and Radius Constraints Using Magnetar Giant Flare Oscillations

Core equation of state

Deibel Apr-8-2013Steiner, Lattimer, Brown 2010

1.5 M

1.0 M