1982
DOI: 10.1086/160028
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Low-luminosity accretion onto magnetized neutron stars

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Cited by 74 publications
(99 citation statements)
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“…The hard emission from X-ray pulsars is believed to originate in the accretion column, as a result of Comptonization of soft photons coming from the neutron star thermal mound by high-energy electrons in the accretion flow (Becker & Wolff 2007). We speculate that as the accretion rate increases, the photons spend more time on average being upscattered in the flow before escaping from the accretion column, which results in harder X-ray spectra (Langer & Rappaport 1982;Becker & Wolff 2007).…”
Section: Spectral Analysismentioning
confidence: 91%
“…The hard emission from X-ray pulsars is believed to originate in the accretion column, as a result of Comptonization of soft photons coming from the neutron star thermal mound by high-energy electrons in the accretion flow (Becker & Wolff 2007). We speculate that as the accretion rate increases, the photons spend more time on average being upscattered in the flow before escaping from the accretion column, which results in harder X-ray spectra (Langer & Rappaport 1982;Becker & Wolff 2007).…”
Section: Spectral Analysismentioning
confidence: 91%
“…2. For sources to the left of this line, we expect that the effect of Coulomb interactions is reduced, and the final stopping occurs via passage through a discontinuous, gas-mediated shock (Langer & Rappaport 1982). Hence we anticipate that the emission region approaches the stellar surface as L X is reduced below L coul .…”
Section: Comparison Of L X With L Coulmentioning
confidence: 96%
“…The associated drop in the density causes the Thomson depth τ to fall below the value τ * ∼ 20 required for the gas to be effectively stopped via Coulomb interactions. It is not completely clear what happens in this case, but we expect that the final phase of deceleration will occur via passage through a gas-mediated shock near the stellar surface (Langer & Rappaport 1982). By combining Eqs.…”
Section: Transition From Coulomb Stopping To Gas Shockmentioning
confidence: 99%
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“…Our knowledge of plasma physics in a strong magnetic field is insufficient to decide if a collisionless shock forms or not (Langer & Rappaport 1982;Arons et al 1987). However, if a collisionless shock forms (which is an assumption) then its height above the NS surface depends on the mass accretion rate: the lower the mass accretion rate, the higher the location of the collisionless shock.…”
Section: Sub-critical X-ray Pulsarsmentioning
confidence: 99%