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2016
DOI: 10.1093/mnras/stw3222
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Discovery and modelling of a flattening of the positive cyclotron line/luminosity relation in GX 304−1 withRXTE

Abstract: The RXTE observed four outbursts of the accreting X-ray binary transient source, GX 304−1 in 2010 and 2011. We present results of detailed 3−100 keV spectral analysis of 69 separate observations, and report a positive correlation between cyclotron line parameters, as well as other spectral parameters, with power law flux. The cyclotron line energy, width and depth versus flux, and thus luminosity, correlations show a flattening of the relationships with increasing luminosity, which are well described by quasi-… Show more

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Cited by 41 publications
(50 citation statements)
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“…In the case of Swift J0243.6+6124 , the continuum from NuSTAR data was found to be described with NPEX or HECut model along with a hot blackbody at ∼3 keV. A blackbody component associated with a continuum model was also detected in other pulsars such as EXO 2030+375 (Reig & Coe 1999), RX J0440.9+4431 (Ferrigno et al 2013), GX 304-1 (Rothschild et al 2017) and GX 1+4 (Yoshida et al 2017). Assuming a distance of 2.5 kpc, the size of blackbody emitting region was calculated to be ≈325 m. This value is relatively small and consistent with the typical size of accretion column.…”
Section: Discussionmentioning
confidence: 90%
“…In the case of Swift J0243.6+6124 , the continuum from NuSTAR data was found to be described with NPEX or HECut model along with a hot blackbody at ∼3 keV. A blackbody component associated with a continuum model was also detected in other pulsars such as EXO 2030+375 (Reig & Coe 1999), RX J0440.9+4431 (Ferrigno et al 2013), GX 304-1 (Rothschild et al 2017) and GX 1+4 (Yoshida et al 2017). Assuming a distance of 2.5 kpc, the size of blackbody emitting region was calculated to be ≈325 m. This value is relatively small and consistent with the typical size of accretion column.…”
Section: Discussionmentioning
confidence: 90%
“…The second model associates shifts of the CRSF energy with changes of the height of a collisionless shock above the NS polar cap (Rothschild et al 2017). For the dipole field, the decrease of line energy from ∼60 to 15 keV implies an increase of the height of the line forming region by half a NS radius.…”
Section: Cyclotron Linementioning
confidence: 99%
“…This is likely to be the main stopping agent of the accretion flow when the photon luminosities are low enough for radiation pressure to be unimportant for the accretion flow breaking (but in the CRSF, where the optical depth is very high even at low luminosities, see Bykov & Krasilshchikov (2004)). This model has recently been used to describe the observed non-linear dependencies of the CRSF parameters on luminosity in another subcritical X-ray pulsar GX 304−1 (Rothschild et al 2017). We develop this model in more detail so that it can also be used to describe the evolution of the spectral hardness ratio (HR) with luminosity.…”
Section: Colissionless Shock Modelmentioning
confidence: 99%