2014
DOI: 10.1093/mnras/stu1034
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Variations in the pulsation and spectral characteristics of OAO 1657−415

Abstract: We present broad-band pulsation and spectral characteristics of the accreting X-ray pulsar OAO 1657-415 with a 2.2 d long Suzaku observation carried out covering its orbital phase range ∼ 0.12-0.34, with respect to the mid-eclipse. During the last third of the observation, the X-ray count rate in both the X-ray Imaging Spectrometer (XIS) and the HXD-PIN instruments increased by a factor of more than 10. During this observation, the hardness ratio also changed by a factor of more than 5, uncorrelated with the i… Show more

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Cited by 27 publications
(65 citation statements)
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References 33 publications
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“…This implies a characteristic volume of the clump of V c ≃ R c 3 ≈ 10 35 cm 3 , which would then give the clump responsible for the bright flare a mass of M c ∼ 10 21 g. The estimated values of the mass and radius of the clump are compatible with estimates of the clump mass and radius obtained for other supergiant HMXBs (Bozzo et al 2011;Martínez-Núñez et al 2014;Pradhan et al 2014). The derived value is also in qualitative agreement with the predictions of the clumpy wind model of HMXBs (Ducci et al 2009).…”
Section: Physical Properties Of the Clump Ingested During Flaresupporting
confidence: 79%
“…This implies a characteristic volume of the clump of V c ≃ R c 3 ≈ 10 35 cm 3 , which would then give the clump responsible for the bright flare a mass of M c ∼ 10 21 g. The estimated values of the mass and radius of the clump are compatible with estimates of the clump mass and radius obtained for other supergiant HMXBs (Bozzo et al 2011;Martínez-Núñez et al 2014;Pradhan et al 2014). The derived value is also in qualitative agreement with the predictions of the clumpy wind model of HMXBs (Ducci et al 2009).…”
Section: Physical Properties Of the Clump Ingested During Flaresupporting
confidence: 79%
“…In the last few years, a number of papers have presented analyses for some of these objects using broadband X-ray data from missions such as NuSTAR or Suzaku. Thus Jaisawal & Naik (2015) analyze Suzaku data for 4U1700−37; Sasano et al (2014) analyze Suzaku data for 4U1822−371; Naik et al (2011) analyze Suzaku, andFarinelli et al (2016) Suzaku and NuSTAR data for Cen X−3; Tomsick et al (2014) and Parker et al (2015) analyze Suzaku and NuSTAR data for Cyg X−1, while Walton et al (2016) NuSTAR-only data for the same object; Suchy et al (2012) analyze Suzaku data for GX 301−2; Yoshida et al (2017) analyze Suzaku data for GX 1+4; Fürst et al (2013) and Wolff et al (2016) analyze NuSTAR, andFarinelli et al (2016) Suzaku and NuS-TAR data for Her X−1; Shtykovsky et al (2017) analyze NuSTAR, and Hung et al (2010) Suzaku data for LMCX−4; Jaisawal & Naik (2014) and Pradhan et al (2014) analyze Suzaku data for OAO 1657−415;and Maitra & Paul (2013) analyze Suzaku data for Vela X−1.…”
Section: Appendix a Details On Individual Sources And Observationsmentioning
confidence: 99%
“…Note that an additional Gaussian component had to be included for both the BN11 and MYTORUS models due to excess line-like emission at ∼ 6.68 keV, likely due to Fe XXV(r). Pradhan et al (2014) interpret the strong spectral and Xray intensity variations of their phase-resolved Suzaku observations as evidence of a highly inhomogeneous, clumpy stellar wind from the supergiant Ofpe/WN9-type companion, which belongs to a class characterized by exceptionally intense stellar winds with low terminal velocities and high mass loss rates (Martins et al 2007;Mason et al 2012). They estimate clump masses of the order of ∼ 3 × 10 24 g, and further suggest that this object could belong to a distinct class between Supergiant Fast X-ray Transients (SFXTs), which are known to show irregular outbursts lasting from minutes to hours, and "normal" HMXBs.…”
Section: A13 Oao 1657−415mentioning
confidence: 99%
“…Being located at a low galactic latitude, OAO 1657-415 is highly absorbed with a column density of 10 23 cm À2 (Polidan et al 1978;Kamata et al 1990). The energy spectrum of the pulsar can be described by a power law continuum with an exponential high energy cutoff along with a soft excess and prominent emission lines at 6.4, 6.7 and 7.1 keV (Kamata et al 1990;Audley et al 2006;Barnstedt et al 2008;Pradhan et al 2014Pradhan et al , 2019Jaisawal & Naik 2014).…”
Section: Introductionmentioning
confidence: 99%