The Neutron Star—Black Hole Connection 2001
DOI: 10.1007/978-94-010-0548-7_25
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Spin-Orbit Couplings in X-Ray Binaries

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Cited by 199 publications
(471 citation statements)
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“…In the prerecycling phase, the neutron star has a mass of 1:4 M and the companion a mass m co of 0:8 M , consistent with evolutionary scenarios of low-mass binary pulsars (Tauris & Savonije 1999). The initial semimajor axis of the binary [NS, CO] is 0.03 AU, corresponding to an orbital period P orb;B ¼ 1:3 days, below the bifurcation point (CPG).…”
Section: The Binary Pulsarsupporting
confidence: 59%
“…In the prerecycling phase, the neutron star has a mass of 1:4 M and the companion a mass m co of 0:8 M , consistent with evolutionary scenarios of low-mass binary pulsars (Tauris & Savonije 1999). The initial semimajor axis of the binary [NS, CO] is 0.03 AU, corresponding to an orbital period P orb;B ¼ 1:3 days, below the bifurcation point (CPG).…”
Section: The Binary Pulsarsupporting
confidence: 59%
“…The low eccentricity and few-day orbital period of PSR J0740+6620 are consistent with expectations for an He WD companion. A well-defined relationship is observed between P b and M c in such systems (Tauris & Savonije 1999;Istrate et al 2016) and, in the case of PSR J0740+6620, predicts a companion mass M 0.2  . We can also calculate the minimum companion mass by assuming i=90°and M M 1.4 p =  and find M M 0.2 c,min =  .…”
Section: Psr J0740+6620: Constraints On Pulsar and Companion Massmentioning
confidence: 82%
“…The well-known double neutron star (DNS) system PSR B1913+16 provided the first observational evidence for the existence of gravitational waves (GWs; Taylor & Weisberg 1989;Weisberg et al 2010), and the double pulsar system J0737−3039 continues to place ever more stringent constraints on deviations from general relativity (GR) in the strong-field regime (Kramer et al 2006). Neutron star mass measurements can be used to study nuclear physics and the equation of state of ultradense matter (Demorest et al 2010) while also providing insight into the mass distribution of the neutron star population (Özel et al 2012;Kiziltan et al 2013;Antoniadis et al 2016) and, in turn, formation mechanisms and evolution (e.g., Lattimer & Prakash 2004;Tauris & Savonije 1999). Proper-motion measurements can be used to estimate transverse velocity, which also informs theories of neutron star formation and supernova energetics (Ferdman et al 2013).…”
Section: Introductionmentioning
confidence: 99%
“…This may be due to the assumptions made on the mass loss rate during the evolution of the secondaries, which was not derived from a detailed physical model. As a matter of fact, the evolutionary calculations by Tauris & Savonije (1999), who included a more sophisticated treatment of mass loss, yield larger maximum radii for the secondaries. It is interesting to note that our assumption of constant envelope mass is not critical because the dependencies on M env cancels each other in the expression for e 2 .…”
Section: Discussionmentioning
confidence: 99%
“…Since the maximum radius is equal to the Roche lobe radius at the end of mass transfer, we can express the semi-major axis and the orbital period as a function of M . More accurate expressions of the massperiod relation are given by King & Ritter (1999) and Tauris & Savonije (1999).…”
Section: The Residual Eccentricitymentioning
confidence: 99%