Gravitational waves from binary neutron star mergers with a spectral equation of state
Creators
Abstract
In numerical simulations of binary neutron star systems, the equation of state of the dense neutron star matter is an important factor in determining both the physical realism and the numerical accuracy of the simulations. Some equations of state used in simulations are C2 or smoother in the pressure/density relationship function, such as a polytropic equation of state, but may not have the flexibility to model stars or remnants of different masses while keeping their radii within known astrophysical constraints. Other equations of state, such as tabular or piecewise polytropic, may be flexible enough to model additional physics and multiple stars' masses and radii within known constraints, but are not as smooth, resulting in additional numerical error. We will study in this paper a recently developed family of equation of state, using a spectral expansion with sufficient free parameters to allow for a larger flexibility than current polytropic equations of state, and with sufficient smoothness to reduce numerical errors compared to tabulated or piecewise polytropic equations of state. We perform simulations at three mass ratios with a common chirp mass, using two distinct spectral equations of state, and at multiple numerical resolutions. We evaluate the gravitational waves produced from these simulations, comparing the phase error between resolutions and equations of state, as well as with respect to analytical models. From our simulations, we estimate that the phase difference at the merger for binaries with a dimensionless weighted tidal deformability difference greater than ΔΛ˜≈55 can be captured by the spectral Einstein code for these equations of state.
Copyright and License
© 2024 American Physical Society.
Acknowledgement
A. K and F. F. gratefully acknowledge support from the Department of Energy, Office of Science, Office of Nuclear Physics, under Contract No. DE-AC02-05CH11231 and from the NSF through Grant No. AST-2107932. M. D. gratefully acknowledges support from the NSF through Grant No. PHY-2110287. M. D. and F. F. gratefully acknowledge support from NASA through Grant No. 80NSSC22K0719. M. S. acknowledges funding from the Sherman Fairchild Foundation and by NSF Grants No. PHY-1708212, No. PHY-1708213, and No. OAC-1931266 at Caltech. L. K. acknowledges funding from the Sherman Fairchild Foundation and by NSF Grants No. PHY-1912081, No. PHY-2207342, and No. OAC-1931280 at Cornell. Computations for this manuscript were performed on the Plasma cluster, a Cray CS500 supercomputer at UNH supported by the NSF MRI program under grant AGS-1919310, and on the Wheeler cluster at Caltech, supported by the Sherman Fairchild Foundation. The authors acknowledge the Texas Advanced Computing Center (TACC) at The University of Texas at Austin and the NSF for providing resources on the Frontera cluster [40] that have contributed to the research results reported within this paper. Computations were also performed on ACCESS resources through Grant No. PHY990002.
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PhysRevD.110.023034.pdf
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Additional details
Related works
- Is new version of
- Discussion Paper: arXiv:2307.03250 (arXiv)
Funding
- United States Department of Energy
- DE-AC02-05CH11231
- National Science Foundation
- AST-2107932
- National Science Foundation
- PHY-2110287
- National Aeronautics and Space Administration
- 80NSSC22K0719
- Sherman Fairchild Foundation
- National Science Foundation
- PHY-1708212
- National Science Foundation
- PHY-1708213
- National Science Foundation
- OAC-1931266
- National Science Foundation
- PHY-1912081
- National Science Foundation
- PHY-2207342
- National Science Foundation
- OAC-1931280
- National Science Foundation
- AGS-1919310
- The University of Texas at Austin
- National Science Foundation
- PHY990002
Dates
- Submitted
-
2023-07-11
- Accepted
-
2024-01-30