2004ApJ...604..775G


Query : 2004ApJ...604..775G

2004ApJ...604..775G - Astrophys. J., 604, 775-790 (2004/April-1)

Role of beam geometry in population statistics and pulse profiles of radio and gamma-ray pulsars.

GONTHIER P.L., VAN GUILDER R. and HARDING A.K.

Abstract (from CDS):

We present results of a pulsar population synthesis study that incorporates a number of recent developments and some significant improvements over our previous study. We have included the results of the Parkes multibeam pulsar survey in our select group of nine radio surveys, doubling our sample of radio pulsars. More realistic geometries for the radio and γ-ray beams are included in our Monte Carlo computer code, which simulates the characteristics of the Galactic population of radio and γ-ray pulsars. We adopted with some modifications the radio-beam geometry of Arzoumanian, Chernoff, and Cordes. For the γ-ray beam, we have assumed the slot gap geometry described in the work of Muslimov and Harding. To account for the shape of the distribution of radio pulsars in the P{dot}-P diagram, we continue to find that decay of the magnetic field on a timescale of 2.8 Myr is needed. With all nine surveys, our model predicts that EGRET should have seen seven radio-quiet (below the sensitivity of these radio surveys) and 19 radio-loud γ-ray pulsars. AGILE (nominal sensitivity map) is expected to detect 13 radio-quiet and 37 radio-loud γ-ray pulsars, while GLAST, with greater sensitivity, is expected to detect 276 radio-quiet and 344 radio-loud γ-ray pulsars. When the Parkes multibeam pulsar survey is excluded, the ratio of radio-loud to radio-quiet γ-ray pulsars decreases, especially for GLAST. The decrease for EGRET is 45%, implying that some fraction of EGRET unidentified sources are radio-loud γ-ray pulsars. In the radio geometry adopted, short-period pulsars are core dominated. Unlike the EGRET γ-ray pulsars, our model predicts that when two γ-ray peaks appear in the pulse profile, a dominant radio core peak appears in between the γ-ray peaks. Our findings suggest that further improvements are required in describing both the radio and γ-ray geometries.

Abstract Copyright: ∼

Journal keyword(s): Gamma Rays: Theory - Magnetic Fields - Stars: Pulsars: General - Radiation Mechanisms: Nonthermal - Stars: Neutron

CDS comments: misprint : PSR J0205+6559 for PSR J0205+6449

Simbad objects: 14

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Number of rows : 14
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 SNR G130.7+03.1 SNR 02 05 35.73 +64 49 41.3           ~ 661 4
2 PSR J0205+6449 Psr 02 05 37.92 +64 49 42.8           ~ 268 1
3 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
4 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
5 PSR J0633+1746 Psr 06 33 54.153 +17 46 12.91           ~ 1308 0
6 PSR B0656+14 Psr 06 59 48.18800 +14 14 19.2000   24.85 24.90     ~ 943 1
7 NAME Vela Pulsar Psr 08 35 20.65525 -45 10 35.1545     15.10     ~ 2446 1
8 PSR B1046-58 Psr 10 48 13.10000 -58 32 03.0000           ~ 293 0
9 PSR B1055-52 Psr 10 57 59.0450 -52 26 56.330           ~ 757 0
10 PSR J1105-6107 Psr 11 05 26.1400 -61 07 48.940           ~ 129 0
11 PSR B1706-44 Psr 17 09 42.62000 -44 29 12.0000     13.30     ~ 670 1
12 SNR G011.2-00.3 SNR 18 11 28.9 -19 25 29           ~ 305 1
13 PSR J1811-1926 Psr 18 11 29.15 -19 25 25.4           ~ 136 1
14 PSR B1951+32 Psr 19 52 58.181 +32 52 40.98           ~ 615 2

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