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Search for radio pulsations in LS I +61 303

dc.contributor.authorCañellas, A.
dc.contributor.authorJoshi, B.C.
dc.contributor.authorParedes i Poy, Josep Maria
dc.contributor.authorIshwara-Chandra, C. H.
dc.contributor.authorMoldón Vara, Francisco Javier
dc.contributor.authorZabalza de Torres, Víctor
dc.contributor.authorMartí Ribas, Josep
dc.contributor.authorRibó Gomis, Marc
dc.date.accessioned2020-02-25T10:23:53Z
dc.date.available2020-02-25T10:23:53Z
dc.date.issued2012-07-09
dc.date.updated2020-02-25T10:23:53Z
dc.description.abstractContext. LS I +61 303 is a member of the select group of gamma-ray binaries: galactic binary systems that contain a massive star and a compact object, show a changing milliarcsecond morphology and a similar broad spectral energy distribution (SED) that peaks at MeV-TeV energies and is modulated by the orbital motion. The nature of the compact object is unclear in LS I +61 303, LS 5039 and HESS J0632+057, whereas PSR B1259-63 harbours a 47.74 ms radio pulsar. Aims. A scenario in which a young pulsar wind interacts with the stellar wind has been proposed to explain the very high energy (VHE, E > 100 GeV) gamma-ray emission detected from LS I +61 303, although no pulses have been reported from this system at any wavelength. We aim to find evidence of the pulsar nature of the compact object. Methods. We performed phased array observations with the Giant Metrewave Radio Telescope (GMRT) at 1280 MHz centred at phase 0.54. Simultaneous data from the multi-bit phased array (PA) back-end with a sampling time of tsamp = 128 microsec and from the polarimeter (PMT) back-end with tsamp = 256 microsec where taken. Results. No pulses have been found in the data set, with a minimum detectable mean flux density of \sim 0.38 mJy at 8-sigma level for the pulsed emission from a putative pulsar with period P >2 ms and duty cycle D = 10% in the direction of LS I +61 303. Conclusions. The detection of posible radio pulsations will require deep and sensitive observations at frequencies \sim0.5-5 GHz and orbital phases 0.6-0.7. However, it may be unfeasible to detect pulses if the putative pulsar is not beamed at the Earth or if there is a strong absorption within the binary system.
dc.format.mimetypeapplication/pdf
dc.identifier.idgrec617032
dc.identifier.issn0004-6361
dc.identifier.urihttps://hdl.handle.net/2445/151124
dc.language.isoeng
dc.publisherEDP Sciences
dc.relation.isformatofReproducció del document publicat a: https://doi.org/10.1051/0004-6361/201117619
dc.relation.ispartofAstronomy & Astrophysics, 2012, vol. 543A, p. 122C
dc.relation.urihttps://doi.org/10.1051/0004-6361/201117619
dc.rights(c) The European Southern Observatory (ESO), 2012
dc.rights.accessRightsinfo:eu-repo/semantics/openAccess
dc.sourceArticles publicats en revistes (Física Quàntica i Astrofísica)
dc.subject.classificationRaigs gamma
dc.subject.classificationRaigs X
dc.subject.classificationPúlsars
dc.subject.classificationGalàxies
dc.subject.otherGamma rays
dc.subject.otherX-rays
dc.subject.otherPulsars
dc.subject.otherGalaxies
dc.titleSearch for radio pulsations in LS I +61 303
dc.typeinfo:eu-repo/semantics/article
dc.typeinfo:eu-repo/semantics/publishedVersion

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