1994
DOI: 10.1086/173934
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Rapidly rotating neutron stars in general relativity: Realistic equations of state

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Cited by 630 publications
(759 citation statements)
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“…and a unit time-like description for the four velocity vector we can decompose the Einstein field equations projected onto the frame of reference of a Zero Angular Momentum Observer (ZAMO) to yield three elliptic equations for γ, ρ and ω and a linear ordinary differential equation for α (Cook et al 1994). The elliptic equations are then converted to integral equations using the Green's function approach.…”
Section: Computation Of Rapidly Spinning Stellar Structuresmentioning
confidence: 99%
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“…and a unit time-like description for the four velocity vector we can decompose the Einstein field equations projected onto the frame of reference of a Zero Angular Momentum Observer (ZAMO) to yield three elliptic equations for γ, ρ and ω and a linear ordinary differential equation for α (Cook et al 1994). The elliptic equations are then converted to integral equations using the Green's function approach.…”
Section: Computation Of Rapidly Spinning Stellar Structuresmentioning
confidence: 99%
“…In addition to this instability limit, there are three other limits: (1) the static or nonspinning limit, where ν → 0 and J → 0; (2) the mass-shed limit, at which the compact star spins too fast to keep matter bound to the surface; and (3) the low-mass limit, below which a compact star cannot form. These four limits together define the stable stellar parameter space for an EoS model (Cook et al 1994). Here, apart from the instability limit, we calculate the static and massshed limit sequences, but we do not attempt to determine the low-mass limit, where the numerical solutions are less accurate (Cook et al 1994).…”
Section: Computation Of Rapidly Spinning Stellar Structuresmentioning
confidence: 99%
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“…This allows us to obtain an approximate set of trajectories by using null geodesics of the Kerr metric. For our chosen pulsar period, mass and radius, we estimate appropriate values for a(\J/M) using the numerical models calculated by Cook, Shapiro, & Teukolsky (1994). We adopt a \ 0.47/P (ms) measured in units of M as appropriate to their moderately soft "" FPS ÏÏ model at M \ 1.4 M _ and low…”
Section: Kerr Propagationmentioning
confidence: 99%
“…The dashed line shows the gravitational mass corresponding to a rest mass of 1.4 M⊙ if the binding energy per mass is uniform throughout a star and equal to its surface value. In practice, this provides a strong lower limit to the gravitational mass (see, e.g., the numerical calculations of Cook, Shapiro, & Teukolsky 1994).…”
Section: Results: Vela X-1mentioning
confidence: 99%