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Neutron Star Magnetic Mountains: An Improved Model

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2) B distorted Equilibrium NS asphericity. 4) Spin/Dipole axes misaligned Q 0 GW ... MHS Equilibrium: |B|max and ?max versus Maccreted. Attained ?max realistic (cf. ... – PowerPoint PPT presentation

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Title: Neutron Star Magnetic Mountains: An Improved Model


1
Neutron Star Magnetic Mountains An Improved
Model
Orange 2009 Pulsar Meeting
Maxim Priymak Supervisor Dr. A. Melatos
2
Overview
  • Accreting Neutron Stars (NS) as Gravitational
    Wave (GW) sources
  • Magnetic mountain mechanism
  • Improved magnetic mountain model
  • Implemented more realistic EoS
  • GW detectability decreases
  • Motivation
  • Quantify GW detectability of accreting NS by
    LIGO/ALIGO
  • Construct GW search templates
  • Infer NS properties (Maccreted, conductivity etc)

3
Accreting Neutron Stars
  • Accreting Neutron Stars (NS)
  • X-ray sources (LMXB/HMXB)
  • NS spin up
  • NS spin measurements
  • X-ray pulsations/Burst oscillations/QPO
  • Spin distribution cut off gt 700 Hz
  • None at Obreak up (1500-3000 Hz)
  • NOT a selection effect
  • 2 mechanisms explain this
  • Gravitational Wave (GW) emission
  • Propeller effect
  • Dominant mechanism Inconclusive
  • both contribute

4
Magnetic Mountain
  • Current model deficiencies
  • Rigid crust no sinking
  • Irrotational no FCORIOLIS
  • Constant BCs no crustal freezing
  • Isothermal no variable resistivity
  • No inclination unrealistic
  • Ideal isothermal EoS (P cs2?)
    unrealistic
  • Accretion driven (LMXB/HMXB)
  • B confines matter
  • 1) PHYDROSTATIC gt PMAGNETIC Matter
    Spreads
  • 2) B distorted Equilibrium NS
    asphericity
  • 4) Spin/Dipole axes misaligned Q ? 0
    GW
  • Advantages (as GW emitter)
  • Known position and/or signal f (X-ray / Optical /
    Radio) Persistent
  • Current Models
  • 2D (Payne Melatos 2004)
  • Axisymmetric MHS equilibrium
  • Stable
  • 3D (Vigelius Melatos 2008)
  • Non-ideal MHD
  • Stable

5
Solving the MHS equilibrium
Lorentz force (pressure tension)
  • Supplemented with
  • EoS
  • Mass-flux Constraint dM/d?final dM/d?initial
    dM/d?accreted

Pressure gradient
Gravitational force
Net Force
6
MHS Equilibrium Dipole Moment (µ) and
Ellipticity (e) versus Maccreted
  • 2 Feasible EoS (P K?G)
  • Degenerate Neutron EoS K 5.4e4 (SI), G 5/3
  • Relativistic Degenerate Electron EoS K 4.9e9
    (SI), G 4/3
  • (cf. Ideal Isothermal EoS P cs2? )

7
MHS Equilibrium Bmax and ?max versus Maccreted
  • Attained ?max realistic (cf. Ideal Isothermal
    EoS)
  • Above Bcracking plastic flow ?

8
Magnetic Mountain Ideal Isothermal EoS
Maccreted 3.3x10-5 M?
9
Magnetic Mountain Adiabatic EoS
Degenerate n EoS
Maccreted 3.3x10-7 M?
Degenerate Relativistic e- EoS
Maccreted 3.3x10-8 M?
10
LIGO/ALIGO Estimates
  • GW strain h is

Ma 10-4 M?
Ohmic diffusion arrests mountain growth
Ma 10-5 M?
Ma 10-6 M?
Ma 10-7 M?
Ma 10-8 M?
Ma 10-9 M?
No observed NS that spin fast enough
11
Current Work
  • Extend to realistic Maccreted
  • Implement Realistic Nuclear EoS

Future Work
  • Crustal freezing / sinking
  • Compute feedback b/w mountain and magnetosphere
    Cornell Collaboration
  • Application to X-ray bursts
  • Light curves cyclones / Episodic decay of the
    mountain
  • WHY?
  • Quantify the effects on GW detectability by
    LIGO/ALIGO
  • Construct GW search templates
  • Infer NS properties (Maccreted, conductivity etc)

12
The End
Thank you for your attention.
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