2014
DOI: 10.1093/mnras/stu1640
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Unveiling the redback nature of the low-mass X-ray binary XSS J1227.0−4859 through optical observations★

Abstract: The peculiar low mass X-ray binary XSS J12270-4859, associated with the Fermi/LAT source 2FGL J1227.7-4853, was in a X-ray, gamma-ray and optical low-luminosity persistent state for about a decade until the end of 2012, when it has entered into the dimmest state ever observed. The nature of the compact object has been controversial until the detection of a 1.69ms radio pulsar early 2014. We present optical spectroscopy and optical/near-IR photometry during the previous brighter and in the recent faint states. … Show more

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Cited by 55 publications
(66 citation statements)
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“…. Similar transitions were also observed in IGR J1825-2452, in the M28 globular cluster (Papitto et al 2013) and in the galactic field X-ray source XSS J12270-4859 (henceforth J1227) Bogdanov et al 2014;de Martino et al 2014). The transitions occured on timescales much shorter than secular evolution, likely controlled by variations in the mass transfer rate from the late-type companion.…”
Section: ;supporting
confidence: 64%
“…. Similar transitions were also observed in IGR J1825-2452, in the M28 globular cluster (Papitto et al 2013) and in the galactic field X-ray source XSS J12270-4859 (henceforth J1227) Bogdanov et al 2014;de Martino et al 2014). The transitions occured on timescales much shorter than secular evolution, likely controlled by variations in the mass transfer rate from the late-type companion.…”
Section: ;supporting
confidence: 64%
“…This is because the average density of the star is set entirely by the orbital period (Frank et al 2002). In the case of XSS J12270-4859, for example, the orbital period of ≈ 0.7 hours implies a density similar to a K3V/K4V star, but the spectral type is much earlier, at F5V-G5V, depending upon phase (de Martino et al 2014). XSS J12270-4859 therefore does not fall on the Main Sequence relation and so must be undermassive.…”
Section: Soar Spectroscopy and Properties Of The Secondarymentioning
confidence: 99%
“…According to analytical calculations made by Poutanen & Beloborodov (2006), the ratio of the amplitude of the second harmonic to the fundamental observed from a fast pulsar whose antipodal spots are always visibile, is c 2 /c 1 = 1/2(tan i tan θ), where i is the binary inclination and θ is the spot colatitude. de Martino et al (2014) constrained the inclination of XSS J12270-4859 between 45 and 65…”
Section: Accretion-powered Pulsationsmentioning
confidence: 99%
“…These include, (i) IGR J18245-2452, a binary of the globular cluster M28 that turned on as a bright (L X ≈ 10 36 erg s −1 ) AMSP in 2013, and was observed as a rotationally-powered MSP a few years before, and a few weeks after the accretion event (Papitto et al 2013); (ii) PSR J1023+0038, an MSP that had a sub-luminous ( 10 34 erg s −1 ) accretion disk in 2000/2001 (Archibald et al 2009), and that have entered back again in such a state in 2013 Stappers et al 2014); (iii) XSS J12270-4859, an LMXB that remained for a decade in a subluminous disk accretion phase (Saitou et al 2009;de Martino et al 2010de Martino et al , 2013, characterized by correlated X-ray and UV flux variability (de Martino et al 2013) and by bright radio and GeV emission (de Martino et al 2010;Hill et al 2011); during December 2012 it then transited to an MSP state characterized by the detection of 1.69 ms radio pulsations (Roy et al 2014), a fainter Xray and gamma-ray emission (Tam et al 2013;Bassa et al 2014;Bogdanov et al 2014;Xing & Wang 2014), and the absence of an accretion disk (de Martino et al 2014). …”
Section: Introductionmentioning
confidence: 99%