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

Identifieur interne : 004318 ( PascalFrancis/Curation ); précédent : 004317; suivant : 004319

Discovery 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 :

RBID : Pascal:11-0287659

Descripteurs français

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, 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.
pA  
A01 01  1    @0 0035-8711
A02 01      @0 MNRAA4
A03   1    @0 Mon. Not. R. Astron. Soc.
A05       @2 414
A06       @2 2
A08 01  1  ENG  @1 Discovery of millisecond pulsars in radio searches of southern Fermi Large Area Telescope sources
A11 01  1    @1 KEITH (M. J.)
A11 02  1    @1 JOHNSTON (S.)
A11 03  1    @1 RAY (P. S.)
A11 04  1    @1 FERRARA (E. C.)
A11 05  1    @1 SAZ PARKINSON (P. M.)
A11 06  1    @1 CELIK (Ö.)
A11 07  1    @1 BELFIORE (A.)
A11 08  1    @1 DONATO (D.)
A11 09  1    @1 CHEUNG (C. C.)
A11 10  1    @1 ABDO (A. A.)
A11 11  1    @1 CAMILO (F.)
A11 12  1    @1 FREIRE (P. C. C.)
A11 13  1    @1 GUILLEMOT (L.)
A11 14  1    @1 HARDING (A. K.)
A11 15  1    @1 KRAMER (M.)
A11 16  1    @1 MICHELSON (P. F.)
A11 17  1    @1 RANSOM (S. M.)
A11 18  1    @1 ROMANI (R. W.)
A11 19  1    @1 SMITH (D. A.)
A11 20  1    @1 THOMPSON (D. J.)
A11 21  1    @1 WELTEVREDE (P.)
A11 22  1    @1 WOOD (K. S.)
A14 01      @1 Australia Telescope National Facility, CSIRO @2 Epping, NSW 1710 @3 AUS @Z 1 aut. @Z 2 aut.
A14 02      @1 Space Science Division, Naval Research Laboratory @2 Washington, DC 20375 @3 USA @Z 3 aut. @Z 22 aut.
A14 03      @1 NASA Goddard Space Flight Center @2 Greenbelt, MD 20771 @3 USA @Z 4 aut. @Z 6 aut. @Z 14 aut. @Z 20 aut.
A14 04      @1 Santa Cruz Institute for Particle Physics, Department of Physics and Department of Astronomy and Astrophysics, University of California at Santa Cruz @2 Santa Cruz, CA 95064 @3 USA @Z 5 aut. @Z 7 aut.
A14 05      @1 Center for Research and Exploration in Space Science and Technology (CRESST) and NASA Goddard Space Flight Center @2 Greenbelt, MD 20771 @3 USA @Z 6 aut. @Z 8 aut.
A14 06      @1 Department of Physics and Center for Space Sciences and Technology, University of Maryland Baltimore County @2 Baltimore, MD 21250 @3 USA @Z 6 aut.
A14 07      @1 INAF-Istituto di Astrofisica Spaziale e Fisica Cosmica @2 20133 Milano @3 ITA @Z 7 aut.
A14 08      @1 Dipartimento di Fisica Teorica e Nucleare (DFNT), Università di Pavia @2 27100 Pavia @3 ITA @Z 7 aut.
A14 09      @1 Departments of Physics and Gastronomy, University of Maryland @2 College Park, MD 20742 @3 USA @Z 8 aut.
A14 10      @1 National Research Council Research Associate, National Academy of Sciences @2 Washington, DC 20001 @3 USA @Z 9 aut. @Z 10 aut.
A14 11      @1 Columbia Astrophysics Laboratory Columbia University @2 New York, NY 10027 @3 USA @Z 11 aut.
A14 12      @1 Max-Planck-Institut für Radioastronomie, Auf dem Hiigel 69 @2 53121 Bonn @3 DEU @Z 12 aut. @Z 13 aut. @Z 15 aut.
A14 13      @1 Jodrell Bank Centre for Astrophysics, School of Physics and Astronomy, The University of Manchester @2 Manchester M13 9PL @3 GBR @Z 15 aut. @Z 21 aut.
A14 14      @1 W. W. Hansen Experimental Physics Laboratory, Kavli Institute for Particle Astrophysics and Cosmology, Department of Physics and SLAC National Accelerator Laboratory, Stanford University @2 Stanford, CA 94305 @3 USA @Z 16 aut. @Z 18 aut.
A14 15      @1 National Radio Astronomy Observatory (NRAO) @2 Charlottesville, VA 22903 @3 USA @Z 17 aut.
A14 16      @1 Centre, d'Études Nucléaires de Bordeaux Gradignan, Université Bordeaux 1, CNRS/IN2p3 @2 33175 Gradignan @3 FRA @Z 19 aut.
A20       @1 1292-1300
A21       @1 2011
A23 01      @0 ENG
A43 01      @1 INIST @2 2067 @5 354000190355760360
A44       @0 0000 @1 © 2011 INIST-CNRS. All rights reserved.
A45       @0 1/4 p.
A47 01  1    @0 11-0287659
A60       @1 P
A61       @0 A
A64 01  1    @0 Monthly Notices of the Royal Astronomical Society
A66 01      @0 USA
C01 01    ENG  @0 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.
C02 01  3    @0 001E03
C03 01  X  FRE  @0 Pulsar milliseconde @5 26
C03 01  X  ENG  @0 Millisecond pulsar @5 26
C03 01  X  SPA  @0 Pulsar milisegundo @5 26
C03 02  X  FRE  @0 Pulsar radio @5 27
C03 02  X  ENG  @0 Radiopulsar @5 27
C03 02  X  SPA  @0 Pulsar radio @5 27
C03 03  X  FRE  @0 Source Rγ @5 28
C03 03  X  ENG  @0 Gamma ray source @5 28
C03 03  X  SPA  @0 Fuente Rγ @5 28
C03 04  X  FRE  @0 Périodicité @5 29
C03 04  X  ENG  @0 Periodicity @5 29
C03 04  X  SPA  @0 Periodicidad @5 29
C03 05  X  FRE  @0 Pulsation radio @5 30
C03 05  X  ENG  @0 Radio pulsation @5 30
C03 05  X  SPA  @0 Pulsación radio @5 30
C03 06  3  FRE  @0 Rayonnement gamma @5 31
C03 06  3  ENG  @0 Gamma radiation @5 31
C03 07  3  FRE  @0 Timing @5 32
C03 07  3  ENG  @0 Timing @5 32
C03 08  3  FRE  @0 Position @5 33
C03 08  3  ENG  @0 Positions @5 33
C03 09  X  FRE  @0 Spectre radio @5 34
C03 09  X  ENG  @0 Radio spectrum @5 34
C03 09  X  SPA  @0 Espectro radio @5 34
C03 10  3  FRE  @0 Probabilité @5 35
C03 10  3  ENG  @0 Probability @5 35
C03 11  3  FRE  @0 Orbite @5 36
C03 11  3  ENG  @0 Orbits @5 36
C03 12  X  FRE  @0 Densité élevée @5 37
C03 12  X  ENG  @0 High density @5 37
C03 12  X  SPA  @0 Densidad elevada @5 37
C03 13  3  FRE  @0 Densité flux @5 38
C03 13  3  ENG  @0 Flux density @5 38
C03 14  X  FRE  @0 Mesure dispersion @5 39
C03 14  X  ENG  @0 Dispersion measure @5 39
C03 14  X  SPA  @0 Medida dispersión @5 39
C03 15  X  FRE  @0 Loi puissance @5 40
C03 15  X  ENG  @0 Power law @5 40
C03 15  X  SPA  @0 Ley poder @5 40
C03 16  X  FRE  @0 Forme impulsion @5 41
C03 16  X  ENG  @0 Pulse shape @5 41
C03 16  X  SPA  @0 Forma impulsión @5 41
N21       @1 192
N44 01      @1 OTO
N82       @1 OTO

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Pascal:11-0287659

Le document en format XML

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<name sortKey="Guillemot, L" sort="Guillemot, L" uniqKey="Guillemot L" first="L." last="Guillemot">L. Guillemot</name>
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<name sortKey="Harding, A K" sort="Harding, A K" uniqKey="Harding A" first="A. K." last="Harding">A. K. Harding</name>
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<name sortKey="Kramer, M" sort="Kramer, M" uniqKey="Kramer M" first="M." last="Kramer">M. Kramer</name>
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<name sortKey="Michelson, P F" sort="Michelson, P F" uniqKey="Michelson P" first="P. F." last="Michelson">P. F. Michelson</name>
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<name sortKey="Ransom, S M" sort="Ransom, S M" uniqKey="Ransom S" first="S. M." last="Ransom">S. M. Ransom</name>
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<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>
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<term>Timing</term>
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<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>
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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, 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>
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</fA11>
<fA11 i1="18" i2="1">
<s1>ROMANI (R. W.)</s1>
</fA11>
<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>
</fA14>
<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>
</fA14>
<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>
<sZ>20 aut.</sZ>
</fA14>
<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>
</fA14>
<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>
</fA14>
<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>
<s3>DEU</s3>
<sZ>12 aut.</sZ>
<sZ>13 aut.</sZ>
<sZ>15 aut.</sZ>
</fA14>
<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>
<sZ>19 aut.</sZ>
</fA14>
<fA20>
<s1>1292-1300</s1>
</fA20>
<fA21>
<s1>2011</s1>
</fA21>
<fA23 i1="01">
<s0>ENG</s0>
</fA23>
<fA43 i1="01">
<s1>INIST</s1>
<s2>2067</s2>
<s5>354000190355760360</s5>
</fA43>
<fA44>
<s0>0000</s0>
<s1>© 2011 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45>
<s0>1/4 p.</s0>
</fA45>
<fA47 i1="01" i2="1">
<s0>11-0287659</s0>
</fA47>
<fA60>
<s1>P</s1>
</fA60>
<fA61>
<s0>A</s0>
</fA61>
<fA64 i1="01" i2="1">
<s0>Monthly Notices of the Royal Astronomical Society</s0>
</fA64>
<fA66 i1="01">
<s0>USA</s0>
</fA66>
<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>
</fC03>
<fC03 i1="02" i2="X" l="ENG">
<s0>Radiopulsar</s0>
<s5>27</s5>
</fC03>
<fC03 i1="02" i2="X" l="SPA">
<s0>Pulsar radio</s0>
<s5>27</s5>
</fC03>
<fC03 i1="03" i2="X" l="FRE">
<s0>Source Rγ</s0>
<s5>28</s5>
</fC03>
<fC03 i1="03" i2="X" l="ENG">
<s0>Gamma ray source</s0>
<s5>28</s5>
</fC03>
<fC03 i1="03" i2="X" l="SPA">
<s0>Fuente Rγ</s0>
<s5>28</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE">
<s0>Périodicité</s0>
<s5>29</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG">
<s0>Periodicity</s0>
<s5>29</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA">
<s0>Periodicidad</s0>
<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>
</inist>
</record>

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