Discovery of millisecond pulsars in radio searches of southern Fermi Large Area Telescope sources
Identifieur interne : 001C26 ( PascalFrancis/Corpus ); précédent : 001C25; suivant : 001C27Discovery of millisecond pulsars in radio searches of southern Fermi Large Area Telescope sources
Auteurs : M. J. Keith ; S. Johnston ; P. S. Ray ; E. C. Ferrara ; P. M. Saz Parkinson ; Ö. Celik ; A. Belfiore ; D. Donato ; C. C. Cheung ; A. A. Abdo ; F. Camilo ; P. C. C. Freire ; L. Guillemot ; A. K. Harding ; M. Kramer ; P. F. Michelson ; S. M. Ransom ; R. W. Romani ; D. A. Smith ; D. J. Thompson ; P. Weltevrede ; K. S. WoodSource :
- Monthly Notices of the Royal Astronomical Society [ 0035-8711 ] ; 2011.
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- Pascal (Inist)
English descriptors
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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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NO : | PASCAL 11-0287659 INIST |
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ET : | Discovery of millisecond pulsars in radio searches of southern Fermi Large Area Telescope sources |
AU : | KEITH (M. J.); JOHNSTON (S.); RAY (P. S.); FERRARA (E. C.); SAZ PARKINSON (P. M.); CELIK (Ö.); BELFIORE (A.); DONATO (D.); CHEUNG (C. C.); ABDO (A. A.); CAMILO (F.); FREIRE (P. C. C.); GUILLEMOT (L.); HARDING (A. K.); KRAMER (M.); MICHELSON (P. F.); RANSOM (S. M.); ROMANI (R. W.); SMITH (D. A.); THOMPSON (D. J.); WELTEVREDE (P.); WOOD (K. S.) |
AF : | Australia Telescope National Facility, CSIRO/Epping, NSW 1710/Australie (1 aut., 2 aut.); Space Science Division, Naval Research Laboratory/Washington, DC 20375/Etats-Unis (3 aut., 22 aut.); NASA Goddard Space Flight Center/Greenbelt, MD 20771/Etats-Unis (4 aut., 6 aut., 14 aut., 20 aut.); Santa Cruz Institute for Particle Physics, Department of Physics and Department of Astronomy and Astrophysics, University of California at Santa Cruz/Santa Cruz, CA 95064/Etats-Unis (5 aut., 7 aut.); Center for Research and Exploration in Space Science and Technology (CRESST) and NASA Goddard Space Flight Center/Greenbelt, MD 20771/Etats-Unis (6 aut., 8 aut.); Department of Physics and Center for Space Sciences and Technology, University of Maryland Baltimore County/Baltimore, MD 21250/Etats-Unis (6 aut.); INAF-Istituto di Astrofisica Spaziale e Fisica Cosmica/20133 Milano/Italie (7 aut.); Dipartimento di Fisica Teorica e Nucleare (DFNT), Università di Pavia/27100 Pavia/Italie (7 aut.); Departments of Physics and Gastronomy, University of Maryland/College Park, MD 20742/Etats-Unis (8 aut.); National Research Council Research Associate, National Academy of Sciences/Washington, DC 20001/Etats-Unis (9 aut., 10 aut.); Columbia Astrophysics Laboratory Columbia University/New York, NY 10027/Etats-Unis (11 aut.); Max-Planck-Institut für Radioastronomie, Auf dem Hiigel 69/53121 Bonn/Allemagne (12 aut., 13 aut., 15 aut.); Jodrell Bank Centre for Astrophysics, School of Physics and Astronomy, The University of Manchester/Manchester M13 9PL/Royaume-Uni (15 aut., 21 aut.); W. W. Hansen Experimental Physics Laboratory, Kavli Institute for Particle Astrophysics and Cosmology, Department of Physics and SLAC National Accelerator Laboratory, Stanford University/Stanford, CA 94305/Etats-Unis (16 aut., 18 aut.); National Radio Astronomy Observatory (NRAO)/Charlottesville, VA 22903/Etats-Unis (17 aut.); Centre, d'Études Nucléaires de Bordeaux Gradignan, Université Bordeaux 1, CNRS/IN2p3/33175 Gradignan/France (19 aut.) |
DT : | Publication en série; Niveau analytique |
SO : | Monthly Notices of the Royal Astronomical Society; ISSN 0035-8711; Coden MNRAA4; Etats-Unis; Da. 2011; Vol. 414; No. 2; Pp. 1292-1300; Bibl. 1/4 p. |
LA : | Anglais |
EA : | 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. |
CC : | 001E03 |
FD : | Pulsar milliseconde; Pulsar radio; Source Rγ; Périodicité; Pulsation radio; Rayonnement gamma; Timing; Position; Spectre radio; Probabilité; Orbite; Densité élevée; Densité flux; Mesure dispersion; Loi puissance; Forme impulsion |
ED : | Millisecond pulsar; Radiopulsar; Gamma ray source; Periodicity; Radio pulsation; Gamma radiation; Timing; Positions; Radio spectrum; Probability; Orbits; High density; Flux density; Dispersion measure; Power law; Pulse shape |
SD : | Pulsar milisegundo; Pulsar radio; Fuente Rγ; Periodicidad; Pulsación radio; Espectro radio; Densidad elevada; Medida dispersión; Ley poder; Forma impulsión |
LO : | INIST-2067.354000190355760360 |
ID : | 11-0287659 |
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Pascal:11-0287659Le document en format XML
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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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<author><name sortKey="Celik, O" sort="Celik, O" uniqKey="Celik O" first="Ö." last="Celik">Ö. Celik</name>
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<affiliation><inist:fA14 i1="12"><s1>Max-Planck-Institut für Radioastronomie, Auf dem Hiigel 69</s1>
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<affiliation><inist:fA14 i1="03"><s1>NASA Goddard Space Flight Center</s1>
<s2>Greenbelt, MD 20771</s2>
<s3>USA</s3>
<sZ>4 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>14 aut.</sZ>
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<affiliation><inist:fA14 i1="12"><s1>Max-Planck-Institut für Radioastronomie, Auf dem Hiigel 69</s1>
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<s3>GBR</s3>
<sZ>15 aut.</sZ>
<sZ>21 aut.</sZ>
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<author><name sortKey="Michelson, P F" sort="Michelson, P F" uniqKey="Michelson P" first="P. F." last="Michelson">P. F. Michelson</name>
<affiliation><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>
<s2>Stanford, CA 94305</s2>
<s3>USA</s3>
<sZ>16 aut.</sZ>
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<author><name sortKey="Ransom, S M" sort="Ransom, S M" uniqKey="Ransom S" first="S. M." last="Ransom">S. M. Ransom</name>
<affiliation><inist:fA14 i1="15"><s1>National Radio Astronomy Observatory (NRAO)</s1>
<s2>Charlottesville, VA 22903</s2>
<s3>USA</s3>
<sZ>17 aut.</sZ>
</inist:fA14>
</affiliation>
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<author><name sortKey="Romani, R W" sort="Romani, R W" uniqKey="Romani R" first="R. W." last="Romani">R. W. Romani</name>
<affiliation><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>
<s2>Stanford, CA 94305</s2>
<s3>USA</s3>
<sZ>16 aut.</sZ>
<sZ>18 aut.</sZ>
</inist:fA14>
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<author><name sortKey="Smith, D A" sort="Smith, D A" uniqKey="Smith D" first="D. A." last="Smith">D. A. Smith</name>
<affiliation><inist:fA14 i1="16"><s1>Centre, d'Études Nucléaires de Bordeaux Gradignan, Université Bordeaux 1, CNRS/IN2p3</s1>
<s2>33175 Gradignan</s2>
<s3>FRA</s3>
<sZ>19 aut.</sZ>
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<author><name sortKey="Thompson, D J" sort="Thompson, D J" uniqKey="Thompson D" first="D. J." last="Thompson">D. J. Thompson</name>
<affiliation><inist:fA14 i1="03"><s1>NASA Goddard Space Flight Center</s1>
<s2>Greenbelt, MD 20771</s2>
<s3>USA</s3>
<sZ>4 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>14 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><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>
<s3>GBR</s3>
<sZ>15 aut.</sZ>
<sZ>21 aut.</sZ>
</inist:fA14>
</affiliation>
</author>
<author><name sortKey="Wood, K S" sort="Wood, K S" uniqKey="Wood K" first="K. S." last="Wood">K. S. Wood</name>
<affiliation><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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<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>
</TEI>
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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>
</fA11>
<fA11 i1="03" i2="1"><s1>RAY (P. S.)</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>FERRARA (E. C.)</s1>
</fA11>
<fA11 i1="05" i2="1"><s1>SAZ PARKINSON (P. M.)</s1>
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<fA11 i1="06" i2="1"><s1>CELIK (Ö.)</s1>
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<fA11 i1="07" i2="1"><s1>BELFIORE (A.)</s1>
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<fA11 i1="08" i2="1"><s1>DONATO (D.)</s1>
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<fA11 i1="09" i2="1"><s1>CHEUNG (C. C.)</s1>
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<fA11 i1="10" i2="1"><s1>ABDO (A. A.)</s1>
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<fA11 i1="11" i2="1"><s1>CAMILO (F.)</s1>
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<fA11 i1="13" i2="1"><s1>GUILLEMOT (L.)</s1>
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<fA11 i1="14" i2="1"><s1>HARDING (A. K.)</s1>
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<fA11 i1="15" i2="1"><s1>KRAMER (M.)</s1>
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<fA11 i1="16" i2="1"><s1>MICHELSON (P. F.)</s1>
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<fA11 i1="17" i2="1"><s1>RANSOM (S. M.)</s1>
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<fA11 i1="18" i2="1"><s1>ROMANI (R. W.)</s1>
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<fA11 i1="19" i2="1"><s1>SMITH (D. A.)</s1>
</fA11>
<fA11 i1="20" i2="1"><s1>THOMPSON (D. J.)</s1>
</fA11>
<fA11 i1="21" i2="1"><s1>WELTEVREDE (P.)</s1>
</fA11>
<fA11 i1="22" i2="1"><s1>WOOD (K. S.)</s1>
</fA11>
<fA14 i1="01"><s1>Australia Telescope National Facility, CSIRO</s1>
<s2>Epping, NSW 1710</s2>
<s3>AUS</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
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<fA14 i1="02"><s1>Space Science Division, Naval Research Laboratory</s1>
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<sZ>3 aut.</sZ>
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<fA14 i1="03"><s1>NASA Goddard Space Flight Center</s1>
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<sZ>4 aut.</sZ>
<sZ>6 aut.</sZ>
<sZ>14 aut.</sZ>
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<fA14 i1="04"><s1>Santa Cruz Institute for Particle Physics, Department of Physics and Department of Astronomy and Astrophysics, University of California at Santa Cruz</s1>
<s2>Santa Cruz, CA 95064</s2>
<s3>USA</s3>
<sZ>5 aut.</sZ>
<sZ>7 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>
<s2>Greenbelt, MD 20771</s2>
<s3>USA</s3>
<sZ>6 aut.</sZ>
<sZ>8 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>
<s2>27100 Pavia</s2>
<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>
<s2>New York, NY 10027</s2>
<s3>USA</s3>
<sZ>11 aut.</sZ>
</fA14>
<fA14 i1="12"><s1>Max-Planck-Institut für Radioastronomie, Auf dem Hiigel 69</s1>
<s2>53121 Bonn</s2>
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<sZ>12 aut.</sZ>
<sZ>13 aut.</sZ>
<sZ>15 aut.</sZ>
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<fA14 i1="13"><s1>Jodrell Bank Centre for Astrophysics, School of Physics and Astronomy, The University of Manchester</s1>
<s2>Manchester M13 9PL</s2>
<s3>GBR</s3>
<sZ>15 aut.</sZ>
<sZ>21 aut.</sZ>
</fA14>
<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>
<s2>Stanford, CA 94305</s2>
<s3>USA</s3>
<sZ>16 aut.</sZ>
<sZ>18 aut.</sZ>
</fA14>
<fA14 i1="15"><s1>National Radio Astronomy Observatory (NRAO)</s1>
<s2>Charlottesville, VA 22903</s2>
<s3>USA</s3>
<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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<s1>© 2011 INIST-CNRS. All rights reserved.</s1>
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<fA47 i1="01" i2="1"><s0>11-0287659</s0>
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<fA64 i1="01" i2="1"><s0>Monthly Notices of the Royal Astronomical Society</s0>
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<fA66 i1="01"><s0>USA</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>
</fC03>
<fC03 i1="01" i2="X" l="ENG"><s0>Millisecond pulsar</s0>
<s5>26</s5>
</fC03>
<fC03 i1="01" i2="X" l="SPA"><s0>Pulsar milisegundo</s0>
<s5>26</s5>
</fC03>
<fC03 i1="02" i2="X" l="FRE"><s0>Pulsar radio</s0>
<s5>27</s5>
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<fC03 i1="02" i2="X" l="ENG"><s0>Radiopulsar</s0>
<s5>27</s5>
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<fC03 i1="02" i2="X" l="SPA"><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>
<s5>28</s5>
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<fC03 i1="03" i2="X" l="SPA"><s0>Fuente Rγ</s0>
<s5>28</s5>
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<fC03 i1="04" i2="X" l="FRE"><s0>Périodicité</s0>
<s5>29</s5>
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<s5>29</s5>
</fC03>
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<s5>29</s5>
</fC03>
<fC03 i1="05" i2="X" l="FRE"><s0>Pulsation radio</s0>
<s5>30</s5>
</fC03>
<fC03 i1="05" i2="X" l="ENG"><s0>Radio pulsation</s0>
<s5>30</s5>
</fC03>
<fC03 i1="05" i2="X" l="SPA"><s0>Pulsación radio</s0>
<s5>30</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Rayonnement gamma</s0>
<s5>31</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Gamma radiation</s0>
<s5>31</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Timing</s0>
<s5>32</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Timing</s0>
<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>
<server><NO>PASCAL 11-0287659 INIST</NO>
<ET>Discovery of millisecond pulsars in radio searches of southern Fermi Large Area Telescope sources</ET>
<AU>KEITH (M. J.); JOHNSTON (S.); RAY (P. S.); FERRARA (E. C.); SAZ PARKINSON (P. M.); CELIK (Ö.); BELFIORE (A.); DONATO (D.); CHEUNG (C. C.); ABDO (A. A.); CAMILO (F.); FREIRE (P. C. C.); GUILLEMOT (L.); HARDING (A. K.); KRAMER (M.); MICHELSON (P. F.); RANSOM (S. M.); ROMANI (R. W.); SMITH (D. A.); THOMPSON (D. J.); WELTEVREDE (P.); WOOD (K. S.)</AU>
<AF>Australia Telescope National Facility, CSIRO/Epping, NSW 1710/Australie (1 aut., 2 aut.); Space Science Division, Naval Research Laboratory/Washington, DC 20375/Etats-Unis (3 aut., 22 aut.); NASA Goddard Space Flight Center/Greenbelt, MD 20771/Etats-Unis (4 aut., 6 aut., 14 aut., 20 aut.); Santa Cruz Institute for Particle Physics, Department of Physics and Department of Astronomy and Astrophysics, University of California at Santa Cruz/Santa Cruz, CA 95064/Etats-Unis (5 aut., 7 aut.); Center for Research and Exploration in Space Science and Technology (CRESST) and NASA Goddard Space Flight Center/Greenbelt, MD 20771/Etats-Unis (6 aut., 8 aut.); Department of Physics and Center for Space Sciences and Technology, University of Maryland Baltimore County/Baltimore, MD 21250/Etats-Unis (6 aut.); INAF-Istituto di Astrofisica Spaziale e Fisica Cosmica/20133 Milano/Italie (7 aut.); Dipartimento di Fisica Teorica e Nucleare (DFNT), Università di Pavia/27100 Pavia/Italie (7 aut.); Departments of Physics and Gastronomy, University of Maryland/College Park, MD 20742/Etats-Unis (8 aut.); National Research Council Research Associate, National Academy of Sciences/Washington, DC 20001/Etats-Unis (9 aut., 10 aut.); Columbia Astrophysics Laboratory Columbia University/New York, NY 10027/Etats-Unis (11 aut.); Max-Planck-Institut für Radioastronomie, Auf dem Hiigel 69/53121 Bonn/Allemagne (12 aut., 13 aut., 15 aut.); Jodrell Bank Centre for Astrophysics, School of Physics and Astronomy, The University of Manchester/Manchester M13 9PL/Royaume-Uni (15 aut., 21 aut.); W. W. Hansen Experimental Physics Laboratory, Kavli Institute for Particle Astrophysics and Cosmology, Department of Physics and SLAC National Accelerator Laboratory, Stanford University/Stanford, CA 94305/Etats-Unis (16 aut., 18 aut.); National Radio Astronomy Observatory (NRAO)/Charlottesville, VA 22903/Etats-Unis (17 aut.); Centre, d'Études Nucléaires de Bordeaux Gradignan, Université Bordeaux 1, CNRS/IN2p3/33175 Gradignan/France (19 aut.)</AF>
<DT>Publication en série; Niveau analytique</DT>
<SO>Monthly Notices of the Royal Astronomical Society; ISSN 0035-8711; Coden MNRAA4; Etats-Unis; Da. 2011; Vol. 414; No. 2; Pp. 1292-1300; Bibl. 1/4 p.</SO>
<LA>Anglais</LA>
<EA>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.</EA>
<CC>001E03</CC>
<FD>Pulsar milliseconde; Pulsar radio; Source Rγ; Périodicité; Pulsation radio; Rayonnement gamma; Timing; Position; Spectre radio; Probabilité; Orbite; Densité élevée; Densité flux; Mesure dispersion; Loi puissance; Forme impulsion</FD>
<ED>Millisecond pulsar; Radiopulsar; Gamma ray source; Periodicity; Radio pulsation; Gamma radiation; Timing; Positions; Radio spectrum; Probability; Orbits; High density; Flux density; Dispersion measure; Power law; Pulse shape</ED>
<SD>Pulsar milisegundo; Pulsar radio; Fuente Rγ; Periodicidad; Pulsación radio; Espectro radio; Densidad elevada; Medida dispersión; Ley poder; Forma impulsión</SD>
<LO>INIST-2067.354000190355760360</LO>
<ID>11-0287659</ID>
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