2010
DOI: 10.1051/0004-6361/201014025
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Search for pulsations at high radio frequencies from accreting millisecond X-ray pulsars in quiescence

Abstract: Context. It is commonly believed that millisecond radio pulsars have been spun up by transfer of matter and angular momentum from a low-mass companion during an X-ray active mass transfer phase. A subclass of low-mass X-ray binaries is that of the accreting millisecond X-ray pulsars, transient systems that show periods of X-ray quiescence during which radio emission could switch on. Aims. The aim of this work is to search for millisecond pulsations from three accreting millisecond X-ray pulsars, XTE J1751−305,… Show more

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Cited by 23 publications
(13 citation statements)
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“…However, we cannot rule out that a large eclipse duration or temporal broadening from scattering in the interstellar medium are responsible for the non-detection. Most AMXPs fail to show detectable radio pulsations during quiescence (e.g., Iacolina et al 2010;Patruno et al 2017), but this does not rule out that they become rotation-powered pulsars (e.g., Burderi et al 2003). Their rotation-powered activity during quiescence will be better probed by the future Square Kilometre Array (Keane et al 2015), which provides a major boost in sensitivity.…”
Section: Discussionmentioning
confidence: 99%
“…However, we cannot rule out that a large eclipse duration or temporal broadening from scattering in the interstellar medium are responsible for the non-detection. Most AMXPs fail to show detectable radio pulsations during quiescence (e.g., Iacolina et al 2010;Patruno et al 2017), but this does not rule out that they become rotation-powered pulsars (e.g., Burderi et al 2003). Their rotation-powered activity during quiescence will be better probed by the future Square Kilometre Array (Keane et al 2015), which provides a major boost in sensitivity.…”
Section: Discussionmentioning
confidence: 99%
“…No radio pulsations have been detected, setting the strongest possible upper limit (30 μJy at 2 GHz) on the presence of radio pulsations that exist (to date) for any AMXP. Iacolina et al (2010) performed radio pulsation searches toward SAX J1808.4-3658 at the higher observing frequency of 5 GHz and obtained an upper limit of 59 μJy on the presence of radio pulsations (this is equivalent to a 2 GHz upper limit of 280 μJy, if one assumes a power-law spectrum with index −1.7). Their approach assumed that detectability would be limited by freefree absorption, which could be avoided by observing at higher frequencies.…”
Section: Discussionmentioning
confidence: 99%
“…Hence, our observations were conducted at a relatively high central observing frequency of 2 GHz in orderto mitigate these effectswhile still maintaining sensitivity to the typically steep spectra of radio pulsars (ν −1.4 , where ν is the frequency of the electromagnetic radiation; see Bates et al 2013, although note that this result is specifictoisolated nonrecycled pulsars). A previousand complementarysearch of SAX J1808.4−3658 used an even higher observing frequency of 5 GHz in order to avoid free-free absorption from eclipsing material, but itwas correspondingly much less sensitive to steep-spectrum radio emission (Iacolina et al 2010).…”
Section: Radio Observationsmentioning
confidence: 99%
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“…For SAX J1808.4-3658, in particular, the amount of optical light reprocessed by the companion star during X-ray quiescence (Homer et al 2001) is compatible with irradiation by a radio pulsar (Burderi et al 2009), the decrease of the NS spin period between consecutive outbursts is similar to the rate observed from MSPs (Hartman et al 2009;Patruno et al 2012), and the rapid increase of the orbital period suggests ejection of the mass transferred from the companion star and/or changes in the mass quadrupole moment of the companion (di Salvo et al 2008;Burderi et al 2009;Patruno et al 2012). However, radio pulsations have not been detected from either SAX J1808.4-3658 or other AM-SPs (Burgay et al 2003;Iacolina et al 2009Iacolina et al , 2010, except for the case of IGR J18245-2453 (Papitto et al 2013). This could be due to an intrinsic low luminosity of the radio pulsar, geometrical effects, and/or free-free absorption from material ejected from the system by the pulsar radiation pressure (di Salvo et al 2008).…”
Section: Introductionmentioning
confidence: 96%