Beta Equilibrium under Neutron Star Merger Conditions
We calculate the nonzero-temperature correction to the beta equilibrium condition in nuclear matter under neutron star merger conditions, in the temperature range 1mEv < <i>T</i> ≲ 5 mEv. We improve on previous work using a consistent description of nuclear matter based on the IUF and...
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MDPI AG
2021
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oai:doaj.org-article:e5dd0214faf3433b83333f2bb21933a02021-11-25T19:09:27ZBeta Equilibrium under Neutron Star Merger Conditions10.3390/universe71103992218-1997https://doaj.org/article/e5dd0214faf3433b83333f2bb21933a02021-10-01T00:00:00Zhttps://www.mdpi.com/2218-1997/7/11/399https://doaj.org/toc/2218-1997We calculate the nonzero-temperature correction to the beta equilibrium condition in nuclear matter under neutron star merger conditions, in the temperature range 1mEv < <i>T</i> ≲ 5 mEv. We improve on previous work using a consistent description of nuclear matter based on the IUF and SFHo relativistic mean field models. This includes using relativistic dispersion relations for the nucleons, which we show is essential in these models. We find that the nonzero-temperature correction can be of order 10 to 20 MeV, and plays an important role in the correct calculation of Urca rates, which can be wrong by factors of 10 or more if it is neglected.Mark G. AlfordAlexander HaberSteven P. HarrisZiyuan ZhangMDPI AGarticlenuclear matterneutron star mergerbeta equilibrationweak interactionElementary particle physicsQC793-793.5ENUniverse, Vol 7, Iss 399, p 399 (2021) |
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DOAJ |
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DOAJ |
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nuclear matter neutron star merger beta equilibration weak interaction Elementary particle physics QC793-793.5 |
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nuclear matter neutron star merger beta equilibration weak interaction Elementary particle physics QC793-793.5 Mark G. Alford Alexander Haber Steven P. Harris Ziyuan Zhang Beta Equilibrium under Neutron Star Merger Conditions |
description |
We calculate the nonzero-temperature correction to the beta equilibrium condition in nuclear matter under neutron star merger conditions, in the temperature range 1mEv < <i>T</i> ≲ 5 mEv. We improve on previous work using a consistent description of nuclear matter based on the IUF and SFHo relativistic mean field models. This includes using relativistic dispersion relations for the nucleons, which we show is essential in these models. We find that the nonzero-temperature correction can be of order 10 to 20 MeV, and plays an important role in the correct calculation of Urca rates, which can be wrong by factors of 10 or more if it is neglected. |
format |
article |
author |
Mark G. Alford Alexander Haber Steven P. Harris Ziyuan Zhang |
author_facet |
Mark G. Alford Alexander Haber Steven P. Harris Ziyuan Zhang |
author_sort |
Mark G. Alford |
title |
Beta Equilibrium under Neutron Star Merger Conditions |
title_short |
Beta Equilibrium under Neutron Star Merger Conditions |
title_full |
Beta Equilibrium under Neutron Star Merger Conditions |
title_fullStr |
Beta Equilibrium under Neutron Star Merger Conditions |
title_full_unstemmed |
Beta Equilibrium under Neutron Star Merger Conditions |
title_sort |
beta equilibrium under neutron star merger conditions |
publisher |
MDPI AG |
publishDate |
2021 |
url |
https://doaj.org/article/e5dd0214faf3433b83333f2bb21933a0 |
work_keys_str_mv |
AT markgalford betaequilibriumunderneutronstarmergerconditions AT alexanderhaber betaequilibriumunderneutronstarmergerconditions AT stevenpharris betaequilibriumunderneutronstarmergerconditions AT ziyuanzhang betaequilibriumunderneutronstarmergerconditions |
_version_ |
1718410251206656000 |