J/MNRAS/328/17      Parkes Multi-Beam Pulsar Survey          (Manchester+, 2001)

The Parkes Multi-Beam Pulsar Survey. I. Observing and data analysis systems, discovery and timing of 100 pulsars. Manchester R.N., Lyne A.G., Camilo F., Bell J.F., Kaspi V.M., D'Amico N., McKay N.P.F., Crawford F., Stairs I.H., Possenti A., Kramer M., Sheppard D.C. <Mon. Not. R. Astron. Soc. 328, 17 (2001)> =2001MNRAS.328...17M 2001MNRAS.328...17M
ADC_Keywords: Pulsars Keywords: methods: observational - pulsars: general Abstract: The Parkes multi-beam pulsar survey is a sensitive survey of a strip along the Galactic plane with |b|<5° and l=260° to l=50°. It uses a 13-beam receiver on the 64-m Parkes radio telescope, receiving two polarizations per beam over a 288-MHz bandwidth centred on 1374MHz. The receiver and data acquisition systems are described in some detail. For pulsar periods in the range 0.1-2s and dispersion measures of less than 300cm-3pc, the nominal limiting flux density of the survey is about 0.2mJy. At shorter or longer periods or higher dispersions, the sensitivity is reduced. Timing observations are carried out for pulsars discovered in the survey for 12-18 months after confirmation to obtain accurate positions, spin parameters, dispersion measures, pulse shapes and mean flux densities. The survey is proving to be extremely successful, with more than 600 pulsars discovered so far. We expect that, when complete, this one survey will come close to finding as many pulsars as all previous pulsar surveys put together. The newly discovered pulsars tend to be young, distant and of high radio luminosity. They will form a valuable sample for studies of pulsar emission properties, the Galactic distribution and evolution of pulsars, and as probes of interstellar medium properties. This paper reports the timing and pulse shape parameters for the first 100 pulsars timed at Parkes, including three pulsars with periods of less than 100ms which are members of binary systems. These results are briefly compared with the parameters of the previously known population. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file table4.dat 96 100 Positions, flux densities and widths for 100 pulsars discovered in the Parkes Multi-Beam Pulsar Survey table5.dat 108 100 Period parameters and dispersion measures table7.dat 50 100 Derived parameters -------------------------------------------------------------------------------- See also: J/MNRAS/335/275 : Parkes Multi-Beam Pulsar Survey. II. (Morris+, 2002) J/MNRAS/342/1299 : Parkes Multi-Beam Pulsar Survey. III. (Kramer+, 2003) J/MNRAS/352/1439 : Parkes Multi-Beam Pulsar Survey. IV. (Hobbs+, 2004) J/MNRAS/372/777 : Parkes Multibeam Pulsar Survey. VI. (Lorimer+, 2006) Byte-by-byte Description of file: table4.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 9 A9 --- PSRJ Pulsar name 11- 12 I2 h RAh Right ascension (J2000) 14- 15 I2 min RAm Right ascension (J2000) 17- 23 F7.4 s RAs Right ascension (J2000) 25- 29 F5.4 s e_RAs rms uncertainty on RA 31 A1 --- DE- Declination sign (J2000) 32- 33 I2 deg DEd Declination (J2000) 35- 36 I2 arcmin DEm Declination (J2000) 38- 43 F6.3 arcsec DEs Declination (J2000) 45- 50 F6.3 arcsec e_DEs rms uncertainty on DE 52- 57 F6.2 deg GLON Galactic longitude 59- 63 F5.2 deg GLAT Galactic latitude 65- 66 I2 --- Beam Beam in which the pulsar was detected 68- 71 F4.2 --- bDist Radial distance of the pulsar from the beam centre in units of the beam radius 73- 77 F5.1 --- S/N Signal-to-noise ratio of the discovery observation from the final time-domain folding in the search process 79- 82 F4.2 mJy S1400MHz Mean flux density at 1400MHz 84- 85 I2 10-2mJy e_S1400MHz rms uncertainty on S1400MHz 87- 92 F6.2 ms W50 Pulse width at 50% of the peak of the mean pulse profile 94- 96 I3 ms W10 ? Pulse width at 10% of the peak of the mean pulse profile -------------------------------------------------------------------------------- Byte-by-byte Description of file: table5.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 9 A9 --- PSRJ Pulsar name 11- 27 F17.15 s Per Period 29- 44 F16.15 s e_Per rms uncertainty on Per 46- 57 F12.7 10-15 dP/dt Period derivative 59- 66 F8.7 10-15 e_dP/dt rms uncertainty on dP/dt 68- 74 F7.1 d Epoch MJD of the epoch of the period 76- 77 I2 --- NTOA Number of time-of-arrival in the timing solution 79- 83 I5 d ObsBeg MJD range covered by the timing observations 84 A1 --- --- [-] 85- 89 I5 d ObsEnd MJD range covered by the timing observations 91- 94 I4 us Res Residual rms timing residual (in µs) 96-102 F7.2 pc/cm3 DM Dispersion measure 104-108 F5.2 pc/cm3 e_DM rms uncertainty on DM -------------------------------------------------------------------------------- Byte-by-byte Description of file: table7.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 9 A9 --- PSRJ Pulsar name 11 A1 --- l_log(tauc) Limit flag on log(tauc) 12- 15 F4.2 [yr] log(tauc) Characteristic age, tauc = P/2(dP/dt) 17 A1 --- l_log(Bs) Limit flag on log(Bs) 18- 22 F5.2 [10-4T] log(Bs) Surface dipole magnetic field, Bs=3.2*1019[(P.dP/dt)1/2] 24 A1 --- l_log(dE/dt) Limit flag on log(dE/dt) 25- 29 F5.2 [10-7W] log(dE/dt) Rate of loss of rotational energy (1) 31 A1 --- l_Dist Limit flag on Dist 32- 35 F4.1 kpc Dist Distance 37 A1 --- l_Z Limit flag on Z 38- 42 F5.2 kpc Z Galactic Z-distance 44 A1 --- l_L1400MHz Limit flag on L1400MHz 45- 50 F6.1 mJy/kpc2 L1400MHz Radio luminosity at L1400MHz -------------------------------------------------------------------------------- Note (1): dE/dt = 4π2IP*P-3, where a neutron-star moment of inertia I=1045g.cm2 is assumed. -------------------------------------------------------------------------------- History: From electronic version of the journal References: Morris et al., Paper II 2002MNRAS.335..275M 2002MNRAS.335..275M, Cat. J/MNRAS/335/275 Kramer et al., Paper III 2003MNRAS.342.1299K 2003MNRAS.342.1299K, Cat. J/MNRAS/342/1299 Hobbs et al., Paper IV 2004MNRAS.352.1439H 2004MNRAS.352.1439H, Cat. J/MNRAS/352/1439 Faulkner et al., Paper V 2004MNRAS.355..147F 2004MNRAS.355..147F Lorimer et al., Paper VI 2006MNRAS.372..777L 2006MNRAS.372..777L, Cat. J/MNRAS/372/777
(End) James Marcout, Patricia Bauer [CDS] 30-Jan-2002
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