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Discovery of millisecond pulsars in radio searches of southern Fermi Large Area Telescope sources

Identifieur interne : 000487 ( Istex/Corpus ); précédent : 000486; suivant : 000488

Discovery 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. Çelik ; 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. Wood

Source :

RBID : ISTEX:1964A26FA641ED7CF1D4DB5264DB117359A1C26C

English descriptors

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, PSR J1103−5403 (1FGL J1103.9−5355) and PSR J2241−5236 (1FGL J2241.9−5236), and a long‐period pulsar, PSR J1604−44 (1FGL J1604.7−4443). 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 PSR J1103−5403 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 PSR J1604−44 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.

Url:
DOI: 10.1111/j.1365-2966.2011.18464.x

Links to Exploration step

ISTEX:1964A26FA641ED7CF1D4DB5264DB117359A1C26C

Le document en format XML

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<name sortKey="Cheung, C C" sort="Cheung, C C" uniqKey="Cheung C" first="C. C." last="Cheung">C. C. Cheung</name>
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<term>1fgl</term>
<term>1fgl catalogue</term>
<term>1fgl sources</term>
<term>Abdo</term>
<term>Acceleration range</term>
<term>Arcmin</term>
<term>Australia telescope</term>
<term>Binary motion</term>
<term>Cent arcmin</term>
<term>Cent arcsec</term>
<term>Cent level</term>
<term>Centre</term>
<term>Circular polarization</term>
<term>Clock correction procedure</term>
<term>Cordes lazio</term>
<term>Count rate</term>
<term>Deep observations</term>
<term>Density limit</term>
<term>Diffuse emission components</term>
<term>Effective area</term>
<term>Electron density</term>
<term>Energetic pulsars</term>
<term>Energy bins</term>
<term>Energy loss</term>
<term>Energy range</term>
<term>Ephemeris</term>
<term>Excellent candidate</term>
<term>Fermi</term>
<term>Fermi satellite</term>
<term>Flux density</term>
<term>Galactic pulsar population</term>
<term>Gamma rays</term>
<term>Gammaray source</term>
<term>Gammaray source 1fgl</term>
<term>High precision timing experiments</term>
<term>Independent evidence</term>
<term>Instrument response functions</term>
<term>Istituto nazionale</term>
<term>Least digits</term>
<term>Likelihood ratio test</term>
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<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, PSR J1103−5403 (1FGL J1103.9−5355) and PSR J2241−5236 (1FGL J2241.9−5236), and a long‐period pulsar, PSR J1604−44 (1FGL J1604.7−4443). 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 PSR J1103−5403 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 PSR J1604−44 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>
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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, PSR J1103−5403 (1FGL J1103.9−5355) and PSR J2241−5236 (1FGL J2241.9−5236), and a long‐period pulsar, PSR J1604−44 (1FGL J1604.7−4443). 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 PSR J1103−5403 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 PSR J1604−44 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.</abstract>
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<head>ABSTRACT</head>
<p>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, PSR J1103
<emph>
<span></span>
</emph>
5403 (1FGL J1103.9
<emph>
<span></span>
</emph>
5355) and PSR J2241
<emph>
<span></span>
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5236 (1FGL J2241.9
<emph>
<span></span>
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5236), and a long‐period pulsar, PSR J1604
<emph>
<span></span>
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44 (1FGL J1604.7
<emph>
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4443). In addition, we searched for but did not detect any radio pulsations from six gamma‐ray pulsars discovered by the
<hi rend="italic">Fermi</hi>
satellite to a level of
<emph>
<span>∼0.04</span>
</emph>
 mJy (for pulsars with a 10 per cent duty cycle).</p>
<p>The timing of the millisecond pulsar PSR J1103
<emph>
<span></span>
</emph>
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
<emph>
<span></span>
</emph>
5355 is associated with the flat spectrum radio source PKS 1101
<emph>
<span></span>
</emph>
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 PSR J1604
<emph>
<span></span>
</emph>
44 is a chance discovery of a weak, long‐period pulsar and is unlikely to be associated with 1FGL J1604.7
<emph>
<span></span>
</emph>
4443. PSR J2241
<emph>
<span></span>
</emph>
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
<emph>
<span></span>
</emph>
5236 make it an excellent candidate for high precision timing experiments. The gamma rays of 1FGL J2241.9
<emph>
<span></span>
</emph>
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
<hi rend="italic">Chandra</hi>
have identified a coincident X‐ray source within 0.1 arcsec of the position of the pulsar obtained by radio timing.</p>
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5236</keyword>
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<p>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, PSR J1103
<span type="mathematics"></span>
5403 (1FGL J1103.9
<span type="mathematics"></span>
5355) and PSR J2241
<span type="mathematics"></span>
5236 (1FGL J2241.9
<span type="mathematics"></span>
5236), and a long‐period pulsar, PSR J1604
<span type="mathematics"></span>
44 (1FGL J1604.7
<span type="mathematics"></span>
4443). In addition, we searched for but did not detect any radio pulsations from six gamma‐ray pulsars discovered by the
<i>Fermi</i>
satellite to a level of
<span type="mathematics">∼0.04</span>
 mJy (for pulsars with a 10 per cent duty cycle).</p>
<p>The timing of the millisecond pulsar PSR J1103
<span type="mathematics"></span>
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
<span type="mathematics"></span>
5355 is associated with the flat spectrum radio source PKS 1101
<span type="mathematics"></span>
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 PSR J1604
<span type="mathematics"></span>
44 is a chance discovery of a weak, long‐period pulsar and is unlikely to be associated with 1FGL J1604.7
<span type="mathematics"></span>
4443. PSR J2241
<span type="mathematics"></span>
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
<span type="mathematics"></span>
5236 make it an excellent candidate for high precision timing experiments. The gamma rays of 1FGL J2241.9
<span type="mathematics"></span>
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
<i>Chandra</i>
have identified a coincident X‐ray source within 0.1 arcsec of the position of the pulsar obtained by radio timing.</p>
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<affiliation>E-mail: mkeith@pulsarastronomy.net</affiliation>
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<namePart type="given">P. S.</namePart>
<namePart type="family">Ray</namePart>
<affiliation>Space Science Division, Naval Research Laboratory, Washington, DC 20375, USA</affiliation>
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<name type="personal">
<namePart type="given">E. C.</namePart>
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<namePart type="given">P. M.</namePart>
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<affiliation>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, USA</affiliation>
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<namePart type="given">Ö.</namePart>
<namePart type="family">Çelik</namePart>
<affiliation>NASA Goddard Space Flight Center, Greenbelt, MD 20771, USA</affiliation>
<affiliation>Center for Research and Exploration in Space Science and Technology (CRESST) and NASA Goddard Space Flight Center, Greenbelt, MD 20771, USA</affiliation>
<affiliation>Department of Physics and Center for Space Sciences and Technology, University of Maryland Baltimore County, Baltimore, MD 21250, USA</affiliation>
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<namePart type="given">A.</namePart>
<namePart type="family">Belfiore</namePart>
<affiliation>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, USA</affiliation>
<affiliation>INAF‐Istituto di Astrofisica Spaziale e Fisica Cosmica, I‐20133 Milano, Italy</affiliation>
<affiliation>Dipartimento di Fisica Teorica e Nucleare (DFNT), Università di Pavia, I‐27100 Pavia, Italy</affiliation>
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<roleTerm type="text">author</roleTerm>
</role>
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<name type="personal">
<namePart type="given">D.</namePart>
<namePart type="family">Donato</namePart>
<affiliation>Center for Research and Exploration in Space Science and Technology (CRESST) and NASA Goddard Space Flight Center, Greenbelt, MD 20771, USA</affiliation>
<affiliation>Departments of Physics and Astronomy, University of Maryland, College Park, MD 20742, USA</affiliation>
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<namePart type="given">C. C.</namePart>
<namePart type="family">Cheung</namePart>
<affiliation>National Research Council Research Associate, National Academy of Sciences, Washington, DC 20001, USA</affiliation>
<affiliation>E‐mail: Resident at Naval Research Laboratory, Washington, DC 20375, USA.</affiliation>
<affiliation>E-mail: mkeith@pulsarastronomy.net</affiliation>
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<affiliation>National Research Council Research Associate, National Academy of Sciences, Washington, DC 20001, USA</affiliation>
<affiliation>E‐mail: Resident at Naval Research Laboratory, Washington, DC 20375, USA.</affiliation>
<affiliation>E-mail: mkeith@pulsarastronomy.net</affiliation>
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<namePart type="family">Camilo</namePart>
<affiliation>Columbia Astrophysics Laboratory, Columbia University, New York, NY 10027, USA</affiliation>
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<namePart type="family">Kramer</namePart>
<affiliation>Max‐Planck‐Institut für Radioastronomie, Auf dem Hügel 69, 53121 Bonn, Germany</affiliation>
<affiliation>Jodrell Bank Centre for Astrophysics, School of Physics and Astronomy, The University of Manchester, Manchester M13 9PL</affiliation>
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<roleTerm type="text">author</roleTerm>
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<name type="personal">
<namePart type="given">P. F.</namePart>
<namePart type="family">Michelson</namePart>
<affiliation>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, USA</affiliation>
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<roleTerm type="text">author</roleTerm>
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<name type="personal">
<namePart type="given">S. M.</namePart>
<namePart type="family">Ransom</namePart>
<affiliation>National Radio Astronomy Observatory (NRAO), Charlottesville, VA 22903, USA</affiliation>
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<name type="personal">
<namePart type="given">R. W.</namePart>
<namePart type="family">Romani</namePart>
<affiliation>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, USA</affiliation>
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<affiliation>Jodrell Bank Centre for Astrophysics, School of Physics and Astronomy, The University of Manchester, Manchester M13 9PL</affiliation>
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<namePart type="given">K. S.</namePart>
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<abstract 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, PSR J1103−5403 (1FGL J1103.9−5355) and PSR J2241−5236 (1FGL J2241.9−5236), and a long‐period pulsar, PSR J1604−44 (1FGL J1604.7−4443). 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 PSR J1103−5403 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 PSR J1604−44 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.</abstract>
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