2016
DOI: 10.1093/pasj/psw003
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A Suzaku observation of the low-mass X-ray binary GS 1826−238 in the hard state

Abstract: The neutron star Low-Mass X-ray Binary GS 1826−238 was observed with Suzaku on 2009 October 21, for a total exposure of 103 ksec. Except for the type I bursts, the source intensity was constant to within ∼ 10%. Combining the Suzaku XIS, HXD-PIN and HXD-GSO data, burst-removed persistent emission was detected over the 0.8-100 keV range, at an unabsorbed flux of 2.6 × 10 −9 erg s −1 cm −2 . Although the implied 0.8-100 keV luminosity, 1.5 × 10 37 erg s −1 (assuming a distance of 7 kpc), is relatively high, the o… Show more

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Cited by 9 publications
(11 citation statements)
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References 29 publications
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“…Considering the large value of R in , it suggests that the corona is centrally localized, and the disk intrudes into only the outer part of the corona. Similar results were obtained by Ono et al (2016) on GS 1826−238, that only an inner region of a truncated accretion disk is Comptonized.…”
Section: The Spectral Modeling Of Exo 0748−676supporting
confidence: 87%
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“…Considering the large value of R in , it suggests that the corona is centrally localized, and the disk intrudes into only the outer part of the corona. Similar results were obtained by Ono et al (2016) on GS 1826−238, that only an inner region of a truncated accretion disk is Comptonized.…”
Section: The Spectral Modeling Of Exo 0748−676supporting
confidence: 87%
“…Among them, the six observations of Aql X−1 (ObsID from 402053020 to 402053070) were previously analyzed by Sakurai et al (2014) and were updated by Sakurai (2015). Besides, GS 1826−238 was further studied in detail by Ono et al (2016), of which the results are quoted in the present paper.…”
Section: Suzaku Archived Sample Of Non-dipping Lmxbsmentioning
confidence: 93%
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“…A double Comptonization corona was also observed in 4U1915−05 (but see also Gambino et al 2019 for a different interpretation) and MAXIJ0556-332 in the soft state (Sugizaki et al 2013;Zhang et al 2014), in GS1826−238 in the low/ hard state and in AqlX-1 in the low hard state just before it made a transition into the soft state (Ono et al 2016). In the last two cases, the sources were at the highest luminosity end of the hard state (L L 0.1 Edd ), at the same luminosity level as the very hard state of 1RXSJ180408.9−342058.…”
Section: Continuum Emissionmentioning
confidence: 80%