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Gravitational waves and neutrino emission from the merger of binary neutron stars. Ref.) 1105.5035. Kenta Kiuchi Collaboration with Y. Sekiguchi , K. Kyutoku , M. Shibata. Introduction. Our research target = high energy astrophysical phenomena
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Gravitational waves and neutrino emission from the merger of binary neutron stars Ref.) 1105.5035 Kenta Kiuchi Collaboration with Y. Sekiguchi, K. Kyutoku, M. Shibata
Introduction Our research target =high energy astrophysical phenomena e.g., Supernova energy ≈ 1.5*1046J = energy the Sun consumes for 1.2 trillion years !! SN1054 (Crab Nebula) Energy source = gravitational potential energy ∝ r-1 ~10km ~1000km r ~Solar mass
Products of high energy astrophysical phenomena ~10km ~3km(1 Solar mass) ✓Density~1015g/cm3(1.41 g/cm3) ⇒ General Relativity, Strong interaction ✓Temperature~1011K(15.7×106K)⇒Weak interaction ✓Magnetic fields~1015 Gauss (Sunspot:several thousand Gauss)⇒Electromagnetic force All of fundamental interaction play an essential role.
Physical aspects of high energy astrophysical phenomena ✓Highly dynamical ✓No special symmetry, e.g., spherical symmetry ⇒Numerical modeling including four kinds of forces Numerical Relativity Figuring out high energy astrophysical phenomena by numerically solving the Einstein equations
Importance of Numerical Relativity ○ Gravitational waves ✓imprinting “raw” information of sources ✓extremely weak signal, hc∼10-22 = the change of (Size of H atoms)/(Distance to Sun) GW detectors Need to prepare theoretical templates of GWs
Today’s topic = Coalescence of binary neutron stars ✓Promising source of GWs ✓Theoretical candidate of Short-Gamma-Ray Burst ✓High-end laboratory for Nuclear theory A nuclear theory ⇒ Mass-Radius relation for Neutron Star Mass-Radius Image of GRB Black hole + disk?
Overview of binary neutron star merger Rapidly rotating massive NS G.Ws. imprintonly information of mass G.Ws. imprintinformation of radius Mtotal< Mcrit NS Mtotal>Mcrit BH and torus ✓Mcritdepends on the Equation of State, i.e. Mcrit= 1.2-1.7 Mmax ✓Final massive NS or torus around BH are extremely hot, T ∼O(10) MeV⇒Neutrino cooling plays an importance role
Set up of binary neutron star ○Shen or Shen-Hyperon EOS based on RMF theory (Shen+,98, Sumiyoshi+,11) ⇒ Mcrit = 2.8-2.9 Solar mass for Shen, 2.3-2.4 Solar mass for Shen-Hyperon EOS ○ Neutrino cooling based on GR leakage scheme (Sekiguchi,10) ○ Equal mass model with 1.35 Solar mass, i.e., Mtot=2.7 Solar mass Mass-Radius Observed BNSs (Lattimer & Paraksh 06) Observation constraint by PSR J1614-2230
Result Density color contour on equatorial (x-y) plane = orbital plane In units of millisecond Log10(ρ [g/cc]) In units of Kilometer
Gravitational Waveforms NSs orbit around each other Massive NS oscillates Shen BH formation Shen-Hyperon
Gravitational Wave Spectrum Sensitivity curves for GW detectors Shen Shen-Hyperon Amplitude frequency GWs could be detected if the merger happens within 30 Mpc.
Neutrino Luminosity Anti electron neutrino Electron neutrino μ, τ neutrino Shen ○ ○ Neutrino cooling timescale ∼ 2-3 second ○ Huge luminosity ∼ 1053 erg/s ○ Could be detected if it happened within 10 Mpc for HK BH formation Shen+ Hyperon
Summary ○ Binary neutron star merger Numerical Relativity simulations with microphysical process for the first time ○ GWs could be detected if it happened within 30 Mpc ○ Neutrino could be detected if it happened within 10 Mpc ⇒ Multi messenger astronomy is coming soon !! Thanks to SR16000 in YITP Thank you for your attention