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Thin accretion discs around millisecond X- ray pulsars —arXiv:1011.2621v1 Reporter: Shaoyong

Thin accretion discs around millisecond X-ray pulsars —arXiv:1011.2621v1 Reporter : Shaoyong

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Page 1: Thin accretion discs around millisecond X-ray pulsars —arXiv:1011.2621v1 Reporter : Shaoyong

Thin accretion discs around millisecond X-ray pulsars

—arXiv:1011.2621v1

Reporter: Shaoyong

Page 2: Thin accretion discs around millisecond X-ray pulsars —arXiv:1011.2621v1 Reporter : Shaoyong

• Millisecond x-ray pulsars have weak magnetic dipole moments of compared to ordinary X-ra∼y pulsars with dipole moments of .

• The accretion disc then extends much closer to the neutron star, where it reaches such a high temperature that the opacity is dominated by electron scattering and radiation pressure can grow stronger than the gas pressure.

• The magnetohydrodynamical turbulence in the accretion disc is also generating a magnetic field through a dynamo action

20 310 Tm

16 310 Tm

Page 3: Thin accretion discs around millisecond X-ray pulsars —arXiv:1011.2621v1 Reporter : Shaoyong

• the magnetic field due to a internal dynamo can strengthen the coupling between the accretion disc and the neutron star.

• the magnetic field due to a dynamo can strengthen the coupling between the accretion disc and the neutron star, and it is shown that the angular momentum exchange between the accretion disc and the neutron star can increase by more than an order of magnitude compared to the standard model by Ghosh & Lamb (1979).

Page 4: Thin accretion discs around millisecond X-ray pulsars —arXiv:1011.2621v1 Reporter : Shaoyong

Divide the disc into three regions:

1. outer region with gas pressure and free-free opacity.

2. middle region with gas pressure and electron scattering opacity.

3. inner region with radiation pressure and electron scattering opacity.

Page 5: Thin accretion discs around millisecond X-ray pulsars —arXiv:1011.2621v1 Reporter : Shaoyong

12 2 13

6 3 312

1.5 104

spinc spin

GMPR P M m

3/2

As

c

R

R

1

72/72 4

4 1/7 4/714 1 16

2 20

21.4 10AR M M m

GM M

20/211/3 10/21 4/7

1 14 1647OMr M M

22/218/21 10/21 4/7

1 14 1612IMr M M

:es ff

:g rp p

Page 6: Thin accretion discs around millisecond X-ray pulsars —arXiv:1011.2621v1 Reporter : Shaoyong

Case :ⅠCase :ⅡCase :ⅢFor a neutron star of M=1.4 ,

A OMR R

IM A OMR R R

A IMR R

sunM 4.8spinP ms

Page 7: Thin accretion discs around millisecond X-ray pulsars —arXiv:1011.2621v1 Reporter : Shaoyong

the magnetic torques due to the dynamo is:

1

0

, 2

0

, , ,

4R z dyn

dyn R

dyn outer dyn mid dyn inner

B BN R dR

N N N

Page 8: Thin accretion discs around millisecond X-ray pulsars —arXiv:1011.2621v1 Reporter : Shaoyong
Page 9: Thin accretion discs around millisecond X-ray pulsars —arXiv:1011.2621v1 Reporter : Shaoyong

• The accretion rates that have been observed in millisecond X-ray pulsars cover several orders of magnitude, and the highest accretion rates are sufficient that the innermost part of the accretion disc is dominated by radiation pressure and electron scattering.

• The large spin changes that have been observed in some of the accreting millisecond X-ray pulsars are difficult to explain in the model by Ghosh & Lamb (1979), but the inclusion of a disc dynamo produces a significant enhancement of the torque between the accretion disc and the neutron star.

Page 10: Thin accretion discs around millisecond X-ray pulsars —arXiv:1011.2621v1 Reporter : Shaoyong

Thank you!