4.7 Article

Equation of state effects on gravitational waves from rotating core collapse

Journal

PHYSICAL REVIEW D
Volume 95, Issue 6, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.95.063019

Keywords

-

Funding

  1. Department of Energy Computational Science Graduate Fellowship [DE-FG02-97ER25308]
  2. National Science Foundation (NSF) Blue Waters Graduate Fellowship
  3. National Science Foundation [OCI-0725070, ACI-1238993]
  4. State of Illinois
  5. NSF [CAREER PHY-1151197, AST-1212170, PHY-1404569]
  6. International Research Unit of Advanced Future Studies, Kyoto university
  7. Sherman Fairchild Foundation
  8. NU ORAU
  9. Social Policy grants
  10. Department of Energy National Nuclear Security Administration [DE-NA0000979]
  11. NASA through Hubble Fellowship awarded by the Space Telescope Science Institute [51344.001-A]
  12. National Science Foundation (JINA Center for the Evolution of the Elements) [PHY-1430152, PHY-1102511]
  13. Direct For Computer & Info Scie & Enginr
  14. Office of Advanced Cyberinfrastructure (OAC) [1440050] Funding Source: National Science Foundation
  15. Direct For Computer & Info Scie & Enginr
  16. Office of Advanced Cyberinfrastructure (OAC) [1440083] Funding Source: National Science Foundation
  17. Direct For Mathematical & Physical Scien
  18. Division Of Physics [1404569] Funding Source: National Science Foundation
  19. Direct For Mathematical & Physical Scien
  20. Division Of Physics [1565546, 1151197, 1430152] Funding Source: National Science Foundation

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Gravitational waves (GWs) generated by axisymmetric rotating collapse, bounce, and early postbounce phases of a galactic core-collapse supernova are detectable by current-generation gravitational wave observatories. Since these GWs are emitted from the quadrupole-deformed nuclear-density core, they may encode information on the uncertain nuclear equation of state (EOS). We examine the effects of the nuclear EOS on GWs from rotating core collapse and carry out 1824 axisymmetric general-relativistic hydrodynamic simulations that cover a parameter space of 98 different rotation profiles and 18 different EOS. We show that the bounce GW signal is largely independent of the EOS and sensitive primarily to the ratio of rotational to gravitational energy, T/vertical bar W vertical bar, and at high rotation rates, to the degree of differential rotation. The GW frequency (f(peak) similar to 600-1000 Hz) of postbounce core oscillations shows stronger EOS dependence that can be parametrized by the core's EOS-dependent dynamical frequency root G (rho) over bar (c). We find that the ratio of the peak frequency to the dynamical frequency f(peak)/(root)G (rho) over bar (c) follows a universal trend that is obeyed by all EOS and rotation profiles and that indicates that the nature of the core oscillations changes when the rotation rate exceeds the dynamical frequency. We find that differences in the treatments of lowdensity nonuniform nuclear matter, of the transition from nonuniform to uniform nuclear matter, and in the description of nuclear matter up to around twice saturation density can mildly affect the GW signal. More exotic, higher-density physics is not probed by GWs from rotating core collapse. We furthermore test the sensitivity of the GW signal to variations in the treatment of nuclear electron capture during collapse. We find that approximations and uncertainties in electron capture rates can lead to variations in the GW signal that are of comparable magnitude to those due to different nuclear EOS. This emphasizes the need for reliable experimental and/or theoretical nuclear electron capture rates and for self-consistent multidimensional neutrino radiation-hydrodynamic simulations of rotating core collapse.

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