2015
DOI: 10.1103/physrevd.91.064057
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Stiffness effects on the dynamics of the bar-mode instability of neutron stars in full general relativity

Abstract: We present results on the effect of the stiffness of the equation of state on the dynamical barmode instability in rapidly rotating polytropic models of neutron stars in full General Relativity. We determine the change in the threshold for the emergence of the instability for a range of the adiabatic Γ index from 2.0 to 3.0, including two values chosen to mimic more realistic equations of state at high densities.PACS numbers: 04.25. 04.40.Dg, 95.30.Lz, 97.60.Jd

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Cited by 19 publications
(26 citation statements)
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“…The latter condition is indeed approximately reached at the end of the presented simulations. These quantities are defined in terms of the two vectors ξ µ (t) = (1, 0, 0, 0) and ξ µ (φ) = (0, cos(φ), sin(φ), 0) (see 8), and are the same that were also used in [22,23] to characterize the properties of isolated rotating stars. Namely:…”
Section: Models Resulting In Collapse To a Black Holementioning
confidence: 99%
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“…The latter condition is indeed approximately reached at the end of the presented simulations. These quantities are defined in terms of the two vectors ξ µ (t) = (1, 0, 0, 0) and ξ µ (φ) = (0, cos(φ), sin(φ), 0) (see 8), and are the same that were also used in [22,23] to characterize the properties of isolated rotating stars. Namely:…”
Section: Models Resulting In Collapse To a Black Holementioning
confidence: 99%
“…Also shown are two often-used isentropic EOS with P = Kρ Γ , Γ ∈ {2.75, 3.00}. These can be seen as a singlepiece approximant of the same SLy EOS (see [22,23]), and have been used for test cases here. The exact parameters of the seven-segment isentropic polytropic approximant are shown in Table I and, as can be seen in the panels of Fig.…”
Section: Initial Models and Numerical Methodsmentioning
confidence: 99%
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“…As noted in the introduction, the state of the system in the post-merger phase is a single (excited) differentially rotating neutron star with a non trivial rotational profile. The remnant may be subject to various instabilities, namely the dynamical bar-mode instability (see [103][104][105] and references therein), the secular Chandrasekhar-Friedman-Schutz (CFS) instability [39,40] and shear instabilities that can develop in differentially rotating stars (see e.g. [106] and references therein).…”
Section: F Corotation and Mode Revivalmentioning
confidence: 99%