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hal.structure.identifierMax-Planck-Institut für Radioastronomie [MPIFR]
dc.contributor.authorGUILLEMOT, Lucas
hal.structure.identifierMax-Planck-Institut für Radioastronomie [MPIFR]
dc.contributor.authorC. C. FREIRE, P.
hal.structure.identifierUnité Scientifique de la Station de Nançay [USN]
hal.structure.identifierLaboratoire de Physique et Chimie de l'Environnement et de l'Espace [LPC2E]
dc.contributor.authorCOGNARD, Ismaël
hal.structure.identifierNational Research Council Associate
dc.contributor.authorJ. JOHNSON, T.
hal.structure.identifierResearch Institute for Science and Engineering
dc.contributor.authorTAKAHASHI, Y.
hal.structure.identifierResearch Institute for Science and Engineering
dc.contributor.authorKATAOKA, J.
hal.structure.identifierMax-Planck-Institut für Radioastronomie [MPIFR]
dc.contributor.authorDESVIGNES, G.
hal.structure.identifierColumbia Astrophysics Laboratory [CAL]
dc.contributor.authorCAMILO, F.
hal.structure.identifierNASA Goddard Space Flight Center [GSFC]
dc.contributor.authorC. FERRARA, E.
hal.structure.identifierNASA Goddard Space Flight Center [GSFC]
dc.contributor.authorK. HARDING, A.
hal.structure.identifierJodrell Bank Centre for Astrophysics
dc.contributor.authorH. JANSSEN, G.
hal.structure.identifierCSIRO Astronomy and Space Science
dc.contributor.authorKEITH, M.
hal.structure.identifierW. W. Hansen Experimental Physics Laboratory [HEPL]
dc.contributor.authorKERR, M.
hal.structure.identifierMax-Planck-Institut für Radioastronomie [MPIFR]
hal.structure.identifierJodrell Bank Centre for Astrophysics
dc.contributor.authorKRAMER, M.
hal.structure.identifierCenter for Earth Observing and Space Research [Fairfax] [CEOSR]
dc.contributor.authorPARENT, D.
hal.structure.identifierNational Radio Astronomy Observatory [NRAO]
dc.contributor.authorM. RANSOM, S.
hal.structure.identifierSanta Cruz Institute for Particle Physics
dc.contributor.authorM. SAZ PARKINSON, P.
hal.structure.identifierGLAST
dc.contributor.authorSMITH, David Stanley
hal.structure.identifierJodrell Bank Centre for Astrophysics
dc.contributor.authorW. STAPPERS, B.
hal.structure.identifierUnité Scientifique de la Station de Nançay [USN]
hal.structure.identifierLaboratoire de Physique et Chimie de l'Environnement et de l'Espace [LPC2E]
dc.contributor.authorTHEUREAU, Gilles
dc.date.issued2012
dc.identifier.issn1745-3933
dc.description.abstractEnWe report the discovery of the millisecond pulsar PSR J2043+1711 in a search of a Fermi Large Area Telescope (LAT) source with no known associations, with the Nanc¸ay Radio Telescope. The new pulsar, confirmed with the Green Bank Telescope, has a spin period of 2.38 ms, is relatively nearby (d 2 kpc) and is in a 1.48-d orbit around a low-mass companion, probably an He-type white dwarf. Using an ephemeris based on Arecibo, Nanc¸ay and Westerbork timing measurements, pulsed gamma-ray emission was detected in the data recorded by the Fermi LAT. The gamma-ray light curve and spectral properties are typical of other gamma-ray millisecond pulsars seen with Fermi. X-ray observations of the pulsar with Suzaku and the Swift X-ray Telescope yielded no detection. At 1.4 GHz, we observe strong flux density variations because of interstellar diffractive scintillation; however, a sharp peak can be observed at this frequency during bright scintillation states. At 327 MHz, the pulsar is detected with a much higher signal-to-noise ratio and its flux density is far more steady. However, at that frequency the Arecibo instrumentation cannot yet fully resolve the pulse profile. Despite that, our pulse time-of-arrival measurements have a post-fit residual rms of 2 μs. This and the expected stability of this system have made PSR J2043+1711 one of the first new Fermi-selected millisecond pulsars to be added to pulsar gravitational wave timing arrays. It has also allowed a significant measurement of relativistic delays in the times of arrival of the pulses due to the curvature of space-time near the companion, but not yet with enough precision to derive useful masses for the pulsar and the companion. Nevertheless, a mass for the pulsar between 1.7 and 2.0M can be derived if a standard millisecond pulsar formation model is assumed. In this paper, we also present a comprehensive summary of pulsar searches in Fermi LAT sources with the Nanc¸ay Radio Telescope to date.
dc.language.isoen
dc.publisherOxford Journals
dc.title.enDiscovery of the millisecond pulsar PSR J2043+1711 in a Fermi source with the Nanc¸ay Radio Telescope
dc.typeArticle de revue
dc.identifier.doi10.1111/j.1365-2966.2012.20694.x
dc.subject.halPhysique [physics]/Astrophysique [astro-ph]/Phénomènes cosmiques de haute energie [astro-ph.HE]
dc.subject.halPlanète et Univers [physics]/Astrophysique [astro-ph]/Phénomènes cosmiques de haute energie [astro-ph.HE]
dc.subject.halPlanète et Univers [physics]
dc.subject.halPhysique [physics]/Astrophysique [astro-ph]
dc.subject.halPhysique [physics]
dc.identifier.arxiv1202.1128
bordeaux.journalMonthly Notices of the Royal Astronomical Society: Letters
bordeaux.page1294-1305
bordeaux.volume422
bordeaux.issue2
bordeaux.peerReviewedoui
hal.identifierin2p3-00685243
hal.version1
hal.popularnon
hal.audienceInternationale
hal.origin.linkhttps://hal.archives-ouvertes.fr//in2p3-00685243v1
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