2013
DOI: 10.1051/0004-6361/201219675
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Testing reflection features in 4U 1705−44 withXMM-Newton,BeppoSAX, and RXTE in the hard and soft states

Abstract: We use data from the bright atoll source 4U 1705−44 taken with XMM-Newton, BeppoSAX, and RXTE both in the hard and in the soft state to perform a self-consistent study of the reflection component in this source. Although the data from these X-ray observatories are not simultaneous, the spectral decomposition is shown to be consistent among the different observations, when the source flux is similar. We have therefore selected observations performed at similar flux levels in the hard and soft states to study th… Show more

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Cited by 56 publications
(89 citation statements)
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“…Unfortunately, Model1 cannot be applied to the B1, B2, or B3 spectra because in the banana state the electron cloud temperature is ∼3 keV (Piraino et al 2007;Di Salvo et al 2009;Egron et al 2013), while the compPS component was considered for electron cloud temperatures T e > 10 keV. We also tried to fit the island state spectrum I using the alternative model wabs*(diskline+compTT+compPS) (Model2), containing a soft Comptonization component (compTT) with spherical geometry, plus a second hard Comptonization component (compPS) with disk geometry.…”
Section: Spectral Analysismentioning
confidence: 99%
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“…Unfortunately, Model1 cannot be applied to the B1, B2, or B3 spectra because in the banana state the electron cloud temperature is ∼3 keV (Piraino et al 2007;Di Salvo et al 2009;Egron et al 2013), while the compPS component was considered for electron cloud temperatures T e > 10 keV. We also tried to fit the island state spectrum I using the alternative model wabs*(diskline+compTT+compPS) (Model2), containing a soft Comptonization component (compTT) with spherical geometry, plus a second hard Comptonization component (compPS) with disk geometry.…”
Section: Spectral Analysismentioning
confidence: 99%
“…The addition of a blackbody component to this model was not statistically significant, suggesting that we did not observe the seed photon component. Recently, Egron et al (2013), combining data from XMM-Newton, RXTE, and BeppoSAX (with the exclusion of the PDS instrument), obtained a similar spectral deconvolution using the model phabs*(nthComp+highecut*rdblur*reflionx), which contains a thermally Comptonized continuum (nthComp; Zdziarski et al 1996;Zycki et al 1999) plus a self-consistent reflection model including both the reflection continuum and the corresponding discrete features (Ross & Fabian 2005). The relativistically smeared rdblur kernel (Fabian et al 1989) was also used.…”
Section: The Island Statementioning
confidence: 99%
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“…Broad iron line profiles have been seen in these accreting systems that harbor a black hole (e.g., Fabian et al 1989;Miller 2007;Reis et al 2008Reis et al , 2009a or a neutron star (NS; e.g., Bhattacharyya & Strohmayer 2007;Cackett et al 2008Cackett et al , 2009Cackett et al , 2010Papitto et al 2008;di Salvo et al 2009;Egron et al 2013;Miller et al 2013) as the primary accreting compact object. The asymmetrically, broadened profile of the Fe a K line gives a direct measure of the position of the inner disk since the effects of gravitational redshift and Doppler redshift/boosting on the emission line become stronger closer to the compact object (Fabian et al 1989).…”
Section: Introductionmentioning
confidence: 99%