Please use this identifier to cite or link to this item: http://hdl.handle.net/2289/7929
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dc.contributor.authorDutta, Anirban-
dc.contributor.authorRana, Vikram-
dc.date.accessioned2022-04-28T05:51:33Z-
dc.date.available2022-04-28T05:51:33Z-
dc.date.issued2022-04-
dc.identifier.citationMonthly Notices of the Royal Astronomical Society, 2022, Vol. 511, p4981en_US
dc.identifier.issn0035-8711-
dc.identifier.issn1365-2966 (Online)-
dc.identifier.urihttp://hdl.handle.net/2289/7929-
dc.descriptionRestricted Access. An open-access version is available at arXiv.org (one of the alternative locations)en_US
dc.description.abstractWe present a simultaneous broad-band analysis of X-ray data obtained with the XMM–Newton and the Nuclear Spectroscopic Telescope Array (NuSTAR) for the asynchronous polar source, CD Ind. The spin-folded light curve in the soft 0.3–3.0 keV band shows a single broad hump-like structure superimposed with occasional narrow dips, indicating a single-pole accretion model with a complex intrinsic absorber. Lack of strong modulation in the folded light curve above 3 keV reveals that emission from the corresponding zone of the post-shock region (PSR) remains in view throughout the spin phase. The broad-band spectrum is modelled with a three-component absorbed plasma emission model and absorbed isobaric cooling flow model, both of which fit the data well with similar statistical significance. The presence of a partial covering absorber is evident in the spectra with equivalent column density ∼7×1022cm−2 and a covering fraction of ~25 per cent. Strong ionized oxygen Kα line emission is detected in the spectra. We notice spectral variability during the spin phase 0.75–1.05, when there is a considerable increase in the column density of the overall absorber (from ∼1×1020cm−2 to ∼9×1020cm−2⁠). We required at least three plasma temperatures to describe the multitemperature nature of the PSR. The shock temperature ∼43.3+3.8−3.4 keV, represented by the upper temperature of the cooling flow model, implies a white dwarf mass of ∼0.87+0.04−0.03M⊙⁠. The iron Kα line complex show strong He-like and weak neutral fluorescence lines. We could not unambiguously detect the presence of Compton reflection in the spectra, which is probably very small and signifies a tall shock height.en_US
dc.language.isoenen_US
dc.publisherOxford University Press on behalf of the Royal Astronomical Societyen_US
dc.relation.uriA broad-band X-ray study of the asynchronous polar CD Inden_US
dc.relation.urihttps://arxiv.org/abs/2201.12334en_US
dc.relation.urihttps://doi.org/10.1093/mnras/stac296en_US
dc.rights2022 The Author(s)en_US
dc.subjectaccretionen_US
dc.subjectaccretion discsen_US
dc.subjectstars: individual: EUVE J2115–58.6en_US
dc.subjectstars: individual: RX J2115.7–5840en_US
dc.subjectnovaeen_US
dc.subjectcataclysmic variablesen_US
dc.subjectwhite dwarfsen_US
dc.titleA broad-band X-ray study of the asynchronous polar CD Inden_US
dc.typeArticleen_US
Appears in Collections:Research Papers (A&A)

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