Discovery of millisecond pulsars in radio searches of southern Fermi Large Area Telescope sources
Identifieur interne : 004318 ( PascalFrancis/Curation ); précédent : 004317; suivant : 004319Discovery of millisecond pulsars in radio searches of southern Fermi Large Area Telescope sources
Auteurs : M. J. Keith [Australie] ; S. Johnston [Australie] ; P. S. Ray [États-Unis] ; E. C. Ferrara [États-Unis] ; P. M. Saz Parkinson [États-Unis] ; Ö. Celik [États-Unis] ; A. Belfiore [États-Unis, Italie] ; D. Donato [États-Unis] ; C. C. Cheung [États-Unis] ; A. A. Abdo [États-Unis] ; F. Camilo [États-Unis] ; P. C. C. Freire [Allemagne] ; L. Guillemot [Allemagne] ; A. K. Harding [États-Unis] ; M. Kramer [Allemagne, Royaume-Uni] ; P. F. Michelson [États-Unis] ; S. M. Ransom [États-Unis] ; R. W. Romani [États-Unis] ; D. A. Smith [France] ; D. J. Thompson [États-Unis] ; P. Weltevrede [Royaume-Uni] ; K. S. Wood [États-Unis]Source :
- Monthly Notices of the Royal Astronomical Society [ 0035-8711 ] ; 2011.
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Abstract
Using the Parkes Radio Telescope, we have carried out deep observations of 11 unassociated gamma-ray sources. Periodicity searches of these data have discovered two millisecond pulsars, PSRJ1103-5403 (1FGLJ1103.9-5355) and PSRJ2241-5236 (1FGLJ2241.9-5236), and a long-period pulsar, PSRJ1604-44 (1FGLJ1604.7-4443). In addition, we searched for but did not detect any radio pulsations from six gamma-ray pulsars discovered by the Fermi satellite to a level of ˜0.04 mJy (for pulsars with a 10 per cent duty cycle). The timing of the millisecond pulsar PSRJ1103-5403 has shown that its position is 9 arcmin from the centroid of the gamma-ray source. Since these observations were carried out, independent evidence has shown that 1FGL J1103.9-5355 is associated with the flat spectrum radio source PKS 1101-536. It appears certain that the pulsar is not associated with the gamma-ray source, despite the seemingly low probability of a chance detection of a radio millisecond pulsar. We consider that PSRJ1604-44 is a chance discovery of a weak, long-period pulsar and is unlikely to be associated with 1FGL J1604.7-4443. PSR J2241-5236 has a spin period of 2.2 ms and orbits a very low mass companion with a 3.5-h orbital period. The relatively high flux density and low dispersion measure of PSR J2241-5236 make it an excellent candidate for high precision timing experiments. The gamma rays of 1FGL J2241.9-5236 have a spectrum that is well modelled by a power law with an exponential cut-off, and phase binning with the radio ephemeris results in a multipeaked gamma-ray pulse profile. Observations with Chandra have identified a coincident X-ray source within 0.1 arcsec of the position of the pulsar obtained by radio timing.
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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Discovery of millisecond pulsars in radio searches of southern Fermi Large Area Telescope sources</title>
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<affiliation wicri:level="1"><inist:fA14 i1="15"><s1>National Radio Astronomy Observatory (NRAO)</s1>
<s2>Charlottesville, VA 22903</s2>
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<affiliation wicri:level="1"><inist:fA14 i1="14"><s1>W. W. Hansen Experimental Physics Laboratory, Kavli Institute for Particle Astrophysics and Cosmology, Department of Physics and SLAC National Accelerator Laboratory, Stanford University</s1>
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<affiliation wicri:level="1"><inist:fA14 i1="16"><s1>Centre, d'Études Nucléaires de Bordeaux Gradignan, Université Bordeaux 1, CNRS/IN2p3</s1>
<s2>33175 Gradignan</s2>
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<sZ>19 aut.</sZ>
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<country>France</country>
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<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>NASA Goddard Space Flight Center</s1>
<s2>Greenbelt, MD 20771</s2>
<s3>USA</s3>
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<sZ>6 aut.</sZ>
<sZ>14 aut.</sZ>
<sZ>20 aut.</sZ>
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<author><name sortKey="Weltevrede, P" sort="Weltevrede, P" uniqKey="Weltevrede P" first="P." last="Weltevrede">P. Weltevrede</name>
<affiliation wicri:level="1"><inist:fA14 i1="13"><s1>Jodrell Bank Centre for Astrophysics, School of Physics and Astronomy, The University of Manchester</s1>
<s2>Manchester M13 9PL</s2>
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<author><name sortKey="Wood, K S" sort="Wood, K S" uniqKey="Wood K" first="K. S." last="Wood">K. S. Wood</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Space Science Division, Naval Research Laboratory</s1>
<s2>Washington, DC 20375</s2>
<s3>USA</s3>
<sZ>3 aut.</sZ>
<sZ>22 aut.</sZ>
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<country>États-Unis</country>
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<series><title level="j" type="main">Monthly Notices of the Royal Astronomical Society</title>
<title level="j" type="abbreviated">Mon. Not. R. Astron. Soc.</title>
<idno type="ISSN">0035-8711</idno>
<imprint><date when="2011">2011</date>
</imprint>
</series>
</biblStruct>
</sourceDesc>
<seriesStmt><title level="j" type="main">Monthly Notices of the Royal Astronomical Society</title>
<title level="j" type="abbreviated">Mon. Not. R. Astron. Soc.</title>
<idno type="ISSN">0035-8711</idno>
</seriesStmt>
</fileDesc>
<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Dispersion measure</term>
<term>Flux density</term>
<term>Gamma radiation</term>
<term>Gamma ray source</term>
<term>High density</term>
<term>Millisecond pulsar</term>
<term>Orbits</term>
<term>Periodicity</term>
<term>Positions</term>
<term>Power law</term>
<term>Probability</term>
<term>Pulse shape</term>
<term>Radio pulsation</term>
<term>Radio spectrum</term>
<term>Radiopulsar</term>
<term>Timing</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Pulsar milliseconde</term>
<term>Pulsar radio</term>
<term>Source Rγ</term>
<term>Périodicité</term>
<term>Pulsation radio</term>
<term>Rayonnement gamma</term>
<term>Timing</term>
<term>Position</term>
<term>Spectre radio</term>
<term>Probabilité</term>
<term>Orbite</term>
<term>Densité élevée</term>
<term>Densité flux</term>
<term>Mesure dispersion</term>
<term>Loi puissance</term>
<term>Forme impulsion</term>
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<front><div type="abstract" xml:lang="en">Using the Parkes Radio Telescope, we have carried out deep observations of 11 unassociated gamma-ray sources. Periodicity searches of these data have discovered two millisecond pulsars, PSRJ1103-5403 (1FGLJ1103.9-5355) and PSRJ2241-5236 (1FGLJ2241.9-5236), and a long-period pulsar, PSRJ1604-44 (1FGLJ1604.7-4443). In addition, we searched for but did not detect any radio pulsations from six gamma-ray pulsars discovered by the Fermi satellite to a level of ˜0.04 mJy (for pulsars with a 10 per cent duty cycle). The timing of the millisecond pulsar PSRJ1103-5403 has shown that its position is 9 arcmin from the centroid of the gamma-ray source. Since these observations were carried out, independent evidence has shown that 1FGL J1103.9-5355 is associated with the flat spectrum radio source PKS 1101-536. It appears certain that the pulsar is not associated with the gamma-ray source, despite the seemingly low probability of a chance detection of a radio millisecond pulsar. We consider that PSRJ1604-44 is a chance discovery of a weak, long-period pulsar and is unlikely to be associated with 1FGL J1604.7-4443. PSR J2241-5236 has a spin period of 2.2 ms and orbits a very low mass companion with a 3.5-h orbital period. The relatively high flux density and low dispersion measure of PSR J2241-5236 make it an excellent candidate for high precision timing experiments. The gamma rays of 1FGL J2241.9-5236 have a spectrum that is well modelled by a power law with an exponential cut-off, and phase binning with the radio ephemeris results in a multipeaked gamma-ray pulse profile. Observations with Chandra have identified a coincident X-ray source within 0.1 arcsec of the position of the pulsar obtained by radio timing.</div>
</front>
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<fA08 i1="01" i2="1" l="ENG"><s1>Discovery of millisecond pulsars in radio searches of southern Fermi Large Area Telescope sources</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>KEITH (M. J.)</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>JOHNSTON (S.)</s1>
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<fA11 i1="03" i2="1"><s1>RAY (P. S.)</s1>
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<fA11 i1="04" i2="1"><s1>FERRARA (E. C.)</s1>
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<fA11 i1="05" i2="1"><s1>SAZ PARKINSON (P. M.)</s1>
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<fA11 i1="19" i2="1"><s1>SMITH (D. A.)</s1>
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<fA11 i1="20" i2="1"><s1>THOMPSON (D. J.)</s1>
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<fA11 i1="21" i2="1"><s1>WELTEVREDE (P.)</s1>
</fA11>
<fA11 i1="22" i2="1"><s1>WOOD (K. S.)</s1>
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<fA14 i1="01"><s1>Australia Telescope National Facility, CSIRO</s1>
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<sZ>5 aut.</sZ>
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<fA14 i1="05"><s1>Center for Research and Exploration in Space Science and Technology (CRESST) and NASA Goddard Space Flight Center</s1>
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<sZ>6 aut.</sZ>
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<fA14 i1="06"><s1>Department of Physics and Center for Space Sciences and Technology, University of Maryland Baltimore County</s1>
<s2>Baltimore, MD 21250</s2>
<s3>USA</s3>
<sZ>6 aut.</sZ>
</fA14>
<fA14 i1="07"><s1>INAF-Istituto di Astrofisica Spaziale e Fisica Cosmica</s1>
<s2>20133 Milano</s2>
<s3>ITA</s3>
<sZ>7 aut.</sZ>
</fA14>
<fA14 i1="08"><s1>Dipartimento di Fisica Teorica e Nucleare (DFNT), Università di Pavia</s1>
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<s3>ITA</s3>
<sZ>7 aut.</sZ>
</fA14>
<fA14 i1="09"><s1>Departments of Physics and Gastronomy, University of Maryland</s1>
<s2>College Park, MD 20742</s2>
<s3>USA</s3>
<sZ>8 aut.</sZ>
</fA14>
<fA14 i1="10"><s1>National Research Council Research Associate, National Academy of Sciences</s1>
<s2>Washington, DC 20001</s2>
<s3>USA</s3>
<sZ>9 aut.</sZ>
<sZ>10 aut.</sZ>
</fA14>
<fA14 i1="11"><s1>Columbia Astrophysics Laboratory Columbia University</s1>
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<sZ>11 aut.</sZ>
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<fA14 i1="12"><s1>Max-Planck-Institut für Radioastronomie, Auf dem Hiigel 69</s1>
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<sZ>15 aut.</sZ>
<sZ>21 aut.</sZ>
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<fA14 i1="14"><s1>W. W. Hansen Experimental Physics Laboratory, Kavli Institute for Particle Astrophysics and Cosmology, Department of Physics and SLAC National Accelerator Laboratory, Stanford University</s1>
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<s3>USA</s3>
<sZ>16 aut.</sZ>
<sZ>18 aut.</sZ>
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<fA14 i1="15"><s1>National Radio Astronomy Observatory (NRAO)</s1>
<s2>Charlottesville, VA 22903</s2>
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<sZ>17 aut.</sZ>
</fA14>
<fA14 i1="16"><s1>Centre, d'Études Nucléaires de Bordeaux Gradignan, Université Bordeaux 1, CNRS/IN2p3</s1>
<s2>33175 Gradignan</s2>
<s3>FRA</s3>
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<fA64 i1="01" i2="1"><s0>Monthly Notices of the Royal Astronomical Society</s0>
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<fC01 i1="01" l="ENG"><s0>Using the Parkes Radio Telescope, we have carried out deep observations of 11 unassociated gamma-ray sources. Periodicity searches of these data have discovered two millisecond pulsars, PSRJ1103-5403 (1FGLJ1103.9-5355) and PSRJ2241-5236 (1FGLJ2241.9-5236), and a long-period pulsar, PSRJ1604-44 (1FGLJ1604.7-4443). In addition, we searched for but did not detect any radio pulsations from six gamma-ray pulsars discovered by the Fermi satellite to a level of ˜0.04 mJy (for pulsars with a 10 per cent duty cycle). The timing of the millisecond pulsar PSRJ1103-5403 has shown that its position is 9 arcmin from the centroid of the gamma-ray source. Since these observations were carried out, independent evidence has shown that 1FGL J1103.9-5355 is associated with the flat spectrum radio source PKS 1101-536. It appears certain that the pulsar is not associated with the gamma-ray source, despite the seemingly low probability of a chance detection of a radio millisecond pulsar. We consider that PSRJ1604-44 is a chance discovery of a weak, long-period pulsar and is unlikely to be associated with 1FGL J1604.7-4443. PSR J2241-5236 has a spin period of 2.2 ms and orbits a very low mass companion with a 3.5-h orbital period. The relatively high flux density and low dispersion measure of PSR J2241-5236 make it an excellent candidate for high precision timing experiments. The gamma rays of 1FGL J2241.9-5236 have a spectrum that is well modelled by a power law with an exponential cut-off, and phase binning with the radio ephemeris results in a multipeaked gamma-ray pulse profile. Observations with Chandra have identified a coincident X-ray source within 0.1 arcsec of the position of the pulsar obtained by radio timing.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001E03</s0>
</fC02>
<fC03 i1="01" i2="X" l="FRE"><s0>Pulsar milliseconde</s0>
<s5>26</s5>
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<fC03 i1="01" i2="X" l="ENG"><s0>Millisecond pulsar</s0>
<s5>26</s5>
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<fC03 i1="01" i2="X" l="SPA"><s0>Pulsar milisegundo</s0>
<s5>26</s5>
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<fC03 i1="02" i2="X" l="FRE"><s0>Pulsar radio</s0>
<s5>27</s5>
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<fC03 i1="03" i2="X" l="FRE"><s0>Source Rγ</s0>
<s5>28</s5>
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<fC03 i1="03" i2="X" l="ENG"><s0>Gamma ray source</s0>
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<fC03 i1="03" i2="X" l="SPA"><s0>Fuente Rγ</s0>
<s5>28</s5>
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<s5>29</s5>
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<fC03 i1="05" i2="X" l="FRE"><s0>Pulsation radio</s0>
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<s5>30</s5>
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<s5>30</s5>
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<s5>31</s5>
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<s5>31</s5>
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<s5>32</s5>
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<s5>32</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Position</s0>
<s5>33</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Positions</s0>
<s5>33</s5>
</fC03>
<fC03 i1="09" i2="X" l="FRE"><s0>Spectre radio</s0>
<s5>34</s5>
</fC03>
<fC03 i1="09" i2="X" l="ENG"><s0>Radio spectrum</s0>
<s5>34</s5>
</fC03>
<fC03 i1="09" i2="X" l="SPA"><s0>Espectro radio</s0>
<s5>34</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Probabilité</s0>
<s5>35</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG"><s0>Probability</s0>
<s5>35</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Orbite</s0>
<s5>36</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Orbits</s0>
<s5>36</s5>
</fC03>
<fC03 i1="12" i2="X" l="FRE"><s0>Densité élevée</s0>
<s5>37</s5>
</fC03>
<fC03 i1="12" i2="X" l="ENG"><s0>High density</s0>
<s5>37</s5>
</fC03>
<fC03 i1="12" i2="X" l="SPA"><s0>Densidad elevada</s0>
<s5>37</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Densité flux</s0>
<s5>38</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Flux density</s0>
<s5>38</s5>
</fC03>
<fC03 i1="14" i2="X" l="FRE"><s0>Mesure dispersion</s0>
<s5>39</s5>
</fC03>
<fC03 i1="14" i2="X" l="ENG"><s0>Dispersion measure</s0>
<s5>39</s5>
</fC03>
<fC03 i1="14" i2="X" l="SPA"><s0>Medida dispersión</s0>
<s5>39</s5>
</fC03>
<fC03 i1="15" i2="X" l="FRE"><s0>Loi puissance</s0>
<s5>40</s5>
</fC03>
<fC03 i1="15" i2="X" l="ENG"><s0>Power law</s0>
<s5>40</s5>
</fC03>
<fC03 i1="15" i2="X" l="SPA"><s0>Ley poder</s0>
<s5>40</s5>
</fC03>
<fC03 i1="16" i2="X" l="FRE"><s0>Forme impulsion</s0>
<s5>41</s5>
</fC03>
<fC03 i1="16" i2="X" l="ENG"><s0>Pulse shape</s0>
<s5>41</s5>
</fC03>
<fC03 i1="16" i2="X" l="SPA"><s0>Forma impulsión</s0>
<s5>41</s5>
</fC03>
<fN21><s1>192</s1>
</fN21>
<fN44 i1="01"><s1>OTO</s1>
</fN44>
<fN82><s1>OTO</s1>
</fN82>
</pA>
</standard>
</inist>
</record>
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