1 x-ray enhancement and long- term evolution of swift j1822.3- 1606 arxiv:1310.2758 authors: o....

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1 X-ray enhancement and l ong-term evolution of S wift J1822.3-1606 arXiv:1310.2758 Authors: O. Benli, S. Caliska n, U. Ertan et al. Reporter: Fu, Lei

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Page 1: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

1

X-ray enhancement and long-term evolution of Swift J1822.3-1

606arXiv:1310.2758

Authors: O. Benli, S. Caliskan, U. Ertan et al.

Reporter: Fu, Lei

Page 2: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

2

Outline

• Introduction• Long-term evolution of Swift J1822.3-16

06• X-ray enhancement of Swift J1822.3-16

06• Discussion and Conclusions

Page 3: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Introduction

• Swift J1822.3-1606 was discovered on 2011 July 14

• a SGR-like burst and associate with outburst

Page 4: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Introduction• The observation of ROSAT in 1993• 0.1–2.4 keV• count rate 0.012

Page 5: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Introduction

Page 6: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Introduction

• Swift J1822.3-1606 is the second low-B magnetar

• Quiescent luminosity ~ erg/s

G105-2 ~ 13B

Page 7: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Introduction

• In magnetar model– toroidal and dipole fields of and

Page 8: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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IntroductionRea et al. 2012

Page 9: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Introduction

Page 10: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Introduction

• This work– Fallback disk model– Determine the evolutionary epoch and the field stre

ngth of this source– Explain the X-ray enhancement of this source

Page 11: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Long-term evolution of Swift J1822.3-1606

• Critical parameter

– Initial surface density profile

– Hot-Cold viscosity transition

Page 12: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Long-term evolution of Swift J1822.3-1606

– Initial outer disk radius

– X-ray irradiation flux

C~– Mass transfer is conservative

Page 13: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Long-term evolution of Swift J1822.3-1606

• The spin evolution– AXP/SGR are sources accreting in spin-do

wn phase

– accretion

– accretion stops

Page 14: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Long-term evolution of Swift J1822.3-1606

in units of

,except for dashed line

P0=300ms

Page 15: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Page 16: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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X-ray enhancement of swift J1822.3-1606

• Disk piles up caused by the SGR burst

Page 17: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Page 18: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Discussion and conclusions

• the properties in quiescent state– accretion– no accretion

Page 19: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Discussion and conclusions

Both the X-ray enhancement and long-term evolution can be explained in the frame of fallback disk model

The model sources with the dipole field strength in the

range on the pole of the star and with the initial periods greater than ~55ms can reach the X-ray luminosity and the rotational properties of Swift J1822.3-1606 simultaneously

When accretion stop the variation in could be observed with out a significant change in the observed luminosity of the source

Page 20: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Quantum spindown of highly magnetized neutron stars

arXiv:1310.1938Authors: B. Lamine, C. Berthiere,

A. DupaysReporter: Fu, Lei

Page 21: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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• vacuum magnetized by the rotating dipole m -->

• due to retardation effect a spin-down torque will excerted on the NS

• the energy loss rate is

Page 22: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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• in the classical dipole spin down

• Spin evolution

Page 23: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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• when period derivative has minimum value

• when quantum contribution will be dominant

Page 24: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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the evolution of crab pulsar in 50kyr

Page 25: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Constraints on the mass and radius of NS

Page 26: 1 X-ray enhancement and long- term evolution of Swift J1822.3- 1606 arXiv:1310.2758 Authors: O. Benli, S. Caliskan, U. Ertan et al. Reporter: Fu, Lei

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Thanks