1986
DOI: 10.1086/164330
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Model atmospheres for X-ray bursting neutron stars

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Cited by 124 publications
(141 citation statements)
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“…These model spectra describe the observed X-ray spectra of X-ray bursting NSs in Low-Mass X-ray Binaries (LMXBs), and they are close to diluted blackbody spectra with a hardness factor f c ∼ 1.5 -1.9 (London et al 1986;Lapidus et al 1986, Madej 1991Pavlov et al 1991). But these model atmospheres with Compton scattering taken into account are not calculated for relatively cool atmospheres with T eff < 10 MK.…”
Section: Introductionsupporting
confidence: 59%
See 1 more Smart Citation
“…These model spectra describe the observed X-ray spectra of X-ray bursting NSs in Low-Mass X-ray Binaries (LMXBs), and they are close to diluted blackbody spectra with a hardness factor f c ∼ 1.5 -1.9 (London et al 1986;Lapidus et al 1986, Madej 1991Pavlov et al 1991). But these model atmospheres with Compton scattering taken into account are not calculated for relatively cool atmospheres with T eff < 10 MK.…”
Section: Introductionsupporting
confidence: 59%
“…It is well known that the Compton down-scattering determines the shape of emergent model spectra of hotter NS atmospheres with T eff ∼ 20 MK and close to Eddington limit (London et al 1986;Lapidus et al 1986;Ebisuzaki 1987). These model spectra describe the observed X-ray spectra of X-ray bursting NSs in Low-Mass X-ray Binaries (LMXBs), and they are close to diluted blackbody spectra with a hardness factor f c ∼ 1.5 -1.9 (London et al 1986;Lapidus et al 1986, Madej 1991Pavlov et al 1991).…”
Section: Introductionmentioning
confidence: 97%
“…Electron scattering dominates the opacity in the neutron star atmosphere, leading to deviations from the original Planckian spectrum (van Paradijs 1982;London et al 1984London et al , 1986see also Titarchuk 1994;Madej 1997, and references therein). Similarly, electron scattering in a disk corona (e.g.…”
Section: Type I X-ray Burstsmentioning
confidence: 99%
“…After 70 s the flux starts to decrease, signifying the end of the Eddington-limited phase. At that time the spectrum shows a hardening lasting approximately 40 s, which may be caused by Comptonization of the thermal photons against a hot receding atmosphere (London et al 1986;Madej et al 2004). The simultaneous radius measurements are most probably biased by this systematic effect and do not represent true variations of the photospheric size.…”
Section: Spectramentioning
confidence: 99%