2003
DOI: 10.1046/j.1365-8711.2003.06699.x
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Dynamical bar-mode instability of differentially rotating stars: effects of equations of state and velocity profiles

Abstract: As an extension of our previous work, we investigate the dynamical instability against non‐axisymmetric bar‐mode deformations of differentially rotating stars in Newtonian gravity by varying the equations of state and velocity profiles. We performed the numerical simulation and the follow‐up linear stability analysis by adopting polytropic equations of state with polytropic indices n= 1, 3/2 and 5/2, and with two types of angular velocity profiles (the so‐called j‐constant‐like and Kepler‐like laws). It is con… Show more

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Cited by 113 publications
(104 citation statements)
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“…Recently, a new kind of dynamical rotational nonaxisymmetric instability at a value of β much lower than the classical threshold has been discovered both in numerical and perturbative studies (see, e.g., [17,22,25,[79][80][81][82][83][84][85] and references therein). This low-β instability (making the classical MacLaurin instability a "high"-β instability) appears to amplify nonaxisymmetric modes at points where their pattern speed σ m (the eigenfrequency ω m divided by the azimuthal mode order m) coincides with the local angular velocity of the fluid [22,[81][82][83].…”
Section: Rotation Of the Proto-neutron Starmentioning
confidence: 99%
“…Recently, a new kind of dynamical rotational nonaxisymmetric instability at a value of β much lower than the classical threshold has been discovered both in numerical and perturbative studies (see, e.g., [17,22,25,[79][80][81][82][83][84][85] and references therein). This low-β instability (making the classical MacLaurin instability a "high"-β instability) appears to amplify nonaxisymmetric modes at points where their pattern speed σ m (the eigenfrequency ω m divided by the azimuthal mode order m) coincides with the local angular velocity of the fluid [22,[81][82][83].…”
Section: Rotation Of the Proto-neutron Starmentioning
confidence: 99%
“…The hypermassive NS is expected to be a non-axisymmetric ellipsoid supported against collapse by a combination of thermal pressure and differential rotation [305] and can delay BH formation for 1 ms to 1 s [305,307]. This phase could wit-ness quite a lot of rotational energy emitted as GWs, with a spectrum that is characteristic of the NS EoS [308,309]. A BH without an accretion disk is not a very likely outcome, but it can happen if M > ∼ 3 M [303, 304,310].…”
Section: Stellar-mass Binariesmentioning
confidence: 99%
“…Analytical and semi-analytical models of NS-NS and NS-BH mergers will be crucial for parameter esti-mation and Bayesian hypothesis testing. This will be a huge challenge for the bar-mode instability regime where the signal does not seem to have any phase coherence (see, e.g., simulations in [308,309]). Even so, accurate modeling of the expected spectrum or time-frequency content of the signal can be useful in understanding the physics of dynamical instabilities.…”
Section: Challengesmentioning
confidence: 99%
“…The j5 models may even reach the threshold of 27% for the high-T /|W | dynamical instability within a few hundred ms of bounce. models already at values of T /|W | of order ∼1% [59,[123][124][125][126]. Hence, this instability is commonly referred to as low-T /|W | instability.…”
Section: Evolution Of the Rotation Rate And Prospects For Rotationmentioning
confidence: 99%