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Merger of Binary Neutron Stars in General Relativity: Insights from Numerical Simulations

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35 diapositives · 498 Views · Aug 25, 2014

This study explores the merger of binary neutron stars (BNS) within the framework of general relativity. It summarizes properties of confirmed BNS systems and emphasizes the importance of gravitational waves (GW) as potential markers of frequent mergers in the universe. Highlighting the simulation of neutron star mergers, it investigates the implications for equation of state (EOS) determination and the potential connection to short gamma-ray bursts (GRBs). The findings underscore that BNS mergers are not rare events and offer valuable insights into the dynamics of strong gravity.

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  1. Merger of binary neutron stars in general relativity M. Shibata(U. Tokyo) Jan 19, 2007 at U. Tokyo

  2. IIntroduction: Binary neutron stars • Formed after 2 supernovae • 4 BNS confirmed: • Orbital Period < 0.5days, • Orbital radius ~ Million km • Total Mass ~ 2.6—2.8 solar mass • PSRB1913+16, P=0.323 d, e=0.617, M=1.387, 1.441 • PSRB1534+12, P=0.421 d, e=0.274, M=1.333, 1.345 • PSRB2127+11, P=0.335 d, e=0.681, M=1.35, 1.36 • PSRJ0737-3039, P=0.102 d, e=0.088, M=1.25,1.34 I. H. Stairs, Science, 304, 547, 2004

  3. Evolve by gravitational radiation Gravitational waves TGW >> Period

  4. Merger time • PSRB1913+16, P=0.323 d, T=0.245 Billion yrs • PSRB1534+12, P=0.421 d, T=2.25 • PSRB2127+11, P=0.335 d, T=0.22 • PSRJ0737-3039, P=0.102 d, T=0.085 Merge within Hubble time ~ 13.7 B yrs  Merger could happen frequently.

  5. Merger rate • per ~10^4 yrs • in our Galaxy • ⇒1 per yrs in • ~ 50 Mpc • (<<4000Mpc) • Not rare event V. Kalogera et al. 04

  6. Frequency of GW in the last 15min r f = 10 Hz (r = 700 km) f = 1—1.2 kHz at onset of merger (r ~ 25 km) f ~ 3 kHz ? during merger f ~ 7 kHz ? black hole QNM ~ 8000 revolution from r=700 km Massive NS Black hole

  7. NS-NS merger = GW source 1st LIGO LIGO Advanced LIGO Frequency (Hz) TAMA VIRGO

  8. Status of first LIGO = Completed ! h(1/Hz^1/2/m) h~10^-21 f (Hz)

  9. Last 15 min of NS-NS 1st LIGO Current level ~100 events per yrs for A-LIGO Advanced LIGO Frequency (Hz)

  10. Before mergerAfter merger ? Need numerical relativity Inspiral signal = well-known Information on Neutron star & Strong gravity Information on mass and spin

  11. g-ray bursts (GRBs) • High-energy transient phenomena of very short duration 10 ms—1000 s • Emit mostly g-rays • Huge total energy E ~ 10^48-10^52 ergs  Central engine = BH + hot torus

  12. One of the Central issues in astrophysics

  13. ?

  14. To summarize Introduction NS-NS merger is • not rare, • promising source of GW, • candidate for short GRBs.  Deserves detailed study

  15. 2Simulation of binary neutron star merger Best approach • Solve Einstein equations & GR hydro equations with no approximation • With realistic initial condition • With realistic EOS GR Simulation is feasible now. Introduce our latest work.

  16. R-M relation of NSs Mass Quark star Lattimer & Prakash Science 304, 2004 Radius

  17. M-r relation for stiff EOS PSR J0751-1807 APR Sly FPS 2s level Choose stiff EOSs Clarify dependence of GW on EOS

  18. Qualitatively universal results Mass (a) 1.50 – 1.50 M_sun (b) 1.35 – 1.65 M_sun (c) 1.30 – 1.30 M_sun with APR EOS Grid #: 633 * 633 * 317 @ NAOJ Memory: 240 GBytes

  19. 1.5-1.5M_sun : Density in the z=0

  20. 1.35-1.65M_sun : Density in the z=0 1.65 1.35

  21. 1.5 – 1.5 M_sun case : final snapshot Apparent horizon X-Y X-Z Y Z ~ no disk mass X X

  22. 1.35 – 1.65 M_sun case : final snapshot Apparent horizon X-Y X-Z Y Z Small disk mass X X

  23. Gravitational waves; BH QNM ringing h ~ 5*10^{-23} at r = 100 Mpc f = 6.5 kHz for a=0.75 & M=2.9M_sun

  24. GW signal 1st LIGO 100kpc Too small Advanced LIGO Frequency (Hz)

  25. 1.3-1.3M_sun : Density in the z=0 Lapse

  26. Case 1.3 – 1.3 M_sun :                       Massive elliptical NS formation X-Y X-Z Y Z X X Dotted curve=2e14 g/cc center=1.3e15 g/cc

  27. Gravitational waves from HMNS + mode Quasi-Periodic oscillation x mode Inspiral wave form

  28. For r <50Mpc Detectable ! GW signal 1st LIGO Detection = HMNS exists ⇒ Constrain EOS Advanced LIGO Frequency (Hz)

  29. Summary for merger: General feature • Large mass case (Mtot > Mcrit)Collapse to a BH in ~ 1ms. For unequal-mass merger ⇒ disk formation  May be Short GRB. • Small mass case (Mtot < Mcrit)Hypermassive NS (HMNS) is formed.Elliptical shape ⇒ Strong GW source Note: Mcrit depends on EOS. Mcrit ~ 2.8M_sun in APR EOS (M_max~2.20) ~ 2.7M_sun in SLY EOS ( ~2.04) ~ 2.4M_sun in FPS EOS ( ~1.80)

  30. Implication of the detection of quasiperiodic signal • Detection = Massive neutron star is formed. • Formation = EOS is sufficiently stiff: Because in soft EOSs, threshold mass is small. • Total mass of system will be determined by chirp signal emitted in the inspiral phase  the threshold mass is constrained constrain EOS • If GW from MHS of M=2.8Msun is detected, SLy & FPS EOSs are rejected: One detection is significant.

  31. 4 Summary • NS-NS merger: one per yrs in ~ 50 Mpc • GW from HMNS will be detected by advanced LIGO if it is formed  Constrain EOS • NS-NS merger may form a central engine of short GRBs. Candidates are • Unequal-mass NS-NS merger to BH. • NS-NS merger to HMNS.

  32. Fate: Summary Merger Elliptical HMNS with diff. rot. Black hole GW emission ~ Equal mass Unequal No disk Small Disk Spheroid T ~ 50 ms B-fields effects BH with Small disk Weak short GRB? BH with Heavy disk Short GRB?

  33. Massive NS • Discovery of PSR J0751-1807:                    Binary of heavy NS + WD • Mass of NS = 2.1 +- 0.2 M_sun (1 sigma)(Nice et al. astro-ph/0508050) Implying very stiff EOS is preferable • But, still large error bar.

  34. PSR J0751-1807 (astroph/0508050) Constrain by GW emission and Shapiro’s time delay Near edge-on