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Constraining the Equation Of State (EOS) of neutron stars with eXTP/GDP Long Ji.

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Presentation on theme: "Constraining the Equation Of State (EOS) of neutron stars with eXTP/GDP Long Ji."— Presentation transcript:

1 Constraining the Equation Of State (EOS) of neutron stars with eXTP/GDP Long Ji

2 Lattimer, J. M.& Prakash, M. 2001

3 Nicer’s result

4 Target: 1, burst oscillations 2, accreting millisecond pulsars 3, rotation-powered pulsars Light bending : R/M Doppler effect(rotate rapidly) : R Key point : the local radiative model

5 1. the mass M of the neutron star; 2. the equatorial radius Req of the neutron star; 3. its specific spin angular momentum a ≡ 2πIf c/GM2, where I is its moment of inertia; 4. the inclination i; 5. the observer colatitude of the spot θs; Dimitrios Psaltis 2014 (if ρ <=10°)

6 Ka Ho Lo et al. 2013

7 Low background: ignore Minimum detectable polarization (MDP), 99% confidence level

8 For type-I bursts Plane-parallel symmetry semi-infinite optical depth Chandra 1947

9 flame spreading Spitkovsky, A. et al. 2002

10 flame spreading Spitkovsky, A. et al. 2002

11 K. Viironen and J. Poutanen 2004

12 Results:

13

14

15 Summary: GDP do not have enough ability to detect the polarization level during bursts.

16 Accreting millisecond pulsars:

17 Marek Gierlinski et al. 2005 Comp/total flux model A: 0.5-5 keV : 77% 0.5-20 keV : 93% model B: 0.5-5 keV : 40% 0.5-20 keV : 79%

18 Can we distinguish them if we have a larger effective area? Produce a faked spectrum by using model A, and then fit it with model B.

19

20 thaw kT_bb

21 trapped by a local minimum

22 Gridding the parameter space

23 n: scattering orders tau: optical density K. Viironen and J. Poutanen 2004

24 Summary: GDP is very helpful to decouple the radiative models

25 X-ray pulsars (slow spin) Distinguish different radiation mechanisms

26 Further improvement?

27 Thanks !!

28 1. the mass M of the neutron star; 2. the equatorial radius Req of the neutron star; 3. the ellipticity of its surface s; 4. its specific spin angular momentum a ≡ 2πIf c/GM2, where I is its moment of inertia; 5 the quadrupole moment of its spacetime as measured by the parameter η; 6. the inclination i; 7. the observer colatitude of the spot θs; and 8. the angular radius of the spot ρ. Dimitrios Psaltis 2014

29 Observables : 1 , flux rms 2 , the ratio of the fundamental to second harmonic 3 , color rms 4 , phase difference Dimitrios Psaltis 2014

30 R 307.28 139.51 norm 21.59 41.85 0.045 0.0091 (0.5-20 1.7429e-09 1.6187e-09) 93% (0.5-20 1.7222e-09 1.3356e-09) 77% (0.5-5 4.4853e-10 5.6668e-10 79%) (0.5-5 2.06e-10 5.139e-10 40%)

31 Dimitrios Psaltis 2014

32 Alessandro Patruno 2009


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