2008
DOI: 10.1051/0004-6361:200809658
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Stability of helium accretion discs in ultracompact binaries

Abstract: Context. Stellar companions of accreting neutron stars in ultra compact X-ray binaries (UCXBs) are hydrogen-deficient. Their helium or C/O accretion discs are strongly X-ray irradiated. Both the chemical composition and irradiation determine the disc stability with respect to thermal and viscous perturbations. At shorter periods, UCXBs are persistent, whereas longer-period systems are mostly transient. Aims. To understand this behaviour one has to derive the stability criteria for X-ray irradiated hydrogen-poo… Show more

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Cited by 100 publications
(170 citation statements)
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“…Using the ultracompact X-ray binary evolution track of Deloye & Bildsten (2003), we can thus predict an orbital period of 50 minutes for this system. If the NS experiences enhanced neutrino cooling, then the mass transfer rate would be higher, and the orbital period could be lower, down to 21 minutes (the minimum for transient helium-accreting ultracompact X-ray binaries; Lasota, Dubus & Kruk 2008).…”
Section: Discussionmentioning
confidence: 99%
“…Using the ultracompact X-ray binary evolution track of Deloye & Bildsten (2003), we can thus predict an orbital period of 50 minutes for this system. If the NS experiences enhanced neutrino cooling, then the mass transfer rate would be higher, and the orbital period could be lower, down to 21 minutes (the minimum for transient helium-accreting ultracompact X-ray binaries; Lasota, Dubus & Kruk 2008).…”
Section: Discussionmentioning
confidence: 99%
“…The threshold luminosities in these refined expressions are up to 2 orders of magnitude higher for P orb < 1 h. The luminosity derived from the burst energetics of (3.1±2.3)×10 35 erg s −1 is consistent with a persistently accreting helium disk only if P orb is smaller than 6 min (1σ confidence), or 7 min (2σ confidence). For a carbon-oxygen-rich disk, this limit would be even more extreme because of higher ionization potentials of these atoms (Lasota et al 2008;Menou et al 2002). For a hydrogen disk P orb would be smaller than 35 min, which is impossible because a hydrogen dwarf would not fit within such an orbit (e.g., Nelson et al 1986;Nelemans 2008).…”
Section: Discussionmentioning
confidence: 99%
“…An additional critical rate is associated with the stability of the accretion disk since we assume that the pulsar can turn on during the quiescent state of the system when it exhibits X-ray transient phenomena (see below). The latter critical accretion rate depends upon the composition of the disk and on the degree of irradiation (Lasota, Dubus & Kruk 2008). For a helium (He) star or He WD we use the He disk models, whereas H disk models are used for MS or giant star companions.…”
Section: Distinguishing Between Accretion Ablation and Propellermentioning
confidence: 99%
“…For a helium (He) star or He WD we use the He disk models, whereas H disk models are used for MS or giant star companions. For simplicity we only consider the irradiated disk models (Lasota, Dubus & Kruk 2008) and assume that the outer edge of the disk extends to 0.8 times the NS Roche radius, however, we included the non-irradiated case as an option within BSE. The pure hydrogen equation is (Lasota, Dubus & Kruk 2008; Appendix A), M irr = 1.5 × 10 −11 R 2.39 10 M −0.64…”
Section: Distinguishing Between Accretion Ablation and Propellermentioning
confidence: 99%
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