2011MNRAS.414.1314M


Query : 2011MNRAS.414.1314M

2011MNRAS.414.1314M - Mon. Not. R. Astron. Soc., 414, 1314-1328 (2011/June-3)

On the pulse-width statistics in radio pulsars – I. Importance of the interpulse emission.

MACIESIAK K., GIL J. and RIBEIRO V.A.R.M.

Abstract (from CDS):

We performed Monte Carlo simulations of different properties of pulsar radio emission, such as pulsar periods, pulse widths, inclination angles and rates of occurrence of interpulse (IP) emission. We used recently available large data sets of the pulsar periods P, the pulse profile widths W and the magnetic inclination angle α. We also compiled the largest ever data base of pulsars with IP, divided into the double pole (DP-IP) and the single pole (SP-IP) cases. We identified 31 (about 2 per cent) and 13 (about 1 per cent) of the former and the latter, respectively, in the population of 1520 normal pulsars. Their distribution on the {img} diagram strongly suggests a secular alignment of the magnetic axis from the originally random orientation. We derived possible parent distribution functions of important pulsar parameters by means of the Kolmogorov–Smirnov significance test using the available data sets (P, W, α and IP), different models of pulsar radio beam ρ=ρ(P) as well as different trial distribution functions of pulsar period P and the inclination angles α. The best suited parent period distribution function is the lognormal distribution, although the gamma function distribution cannot be excluded. The strongest constraint on derived model distribution functions was the requirement that the numbers of IPs generated by means of Monte Carlo simulations (both DP-IP and SP-IP cases) were exactly (within 1σ errors) at the observed level of occurrences. We found that a suitable model distribution function for the inclination angle is the complicated trigonometric function which has two local maxima, one near 0° and the other near 90°. The former and the latter imply the right rates of IP, occurrence, single pole (almost aligned rotator) and double pole (almost orthogonal rotator), respectively. It is very unlikely that the pulsar beam deviates significantly from the circular cross-section. We found that the upper limit for the average beaming factor fb describing a fraction of the full sphere (called also beaming fraction) covered by a pulsar beam is about 10 per cent. This implies that the number of the neutron stars in the Galaxy might be underestimated.

Abstract Copyright: 2011 The Authors Monthly Notices of the Royal Astronomical Society2011 RAS

Journal keyword(s): stars: neutron - pulsars: general - stars: rotation

Simbad objects: 46

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Number of rows : 46
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 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
2 PSR J0627+0706 Psr 06 27 44.17200 +07 06 33.0000           ~ 33 0
3 PSR B0823+26 Psr 08 26 51.5068 +26 37 21.297           ~ 541 1
4 PSR B0826-34 Psr 08 28 16.6 -34 17 07           ~ 167 0
5 PSR J0831-4406 Psr 08 31 32.43 -44 06 11.9           ~ 16 0
6 PSR J0834-4159 Psr 08 34 16.3 -41 59 51           ~ 34 0
7 PSR B0840-48 Psr 08 42 05.44430 -48 51 20.6000           ~ 47 0
8 PSR J0905-5127 Psr 09 05 51.922 -51 27 48.71           ~ 51 0
9 PSR B0906-49 Psr 09 08 35.46000 -49 13 05.0000           ~ 168 0
10 PSR B0950+08 Psr 09 53 09.31210 +07 55 36.9000           ~ 806 2
11 PSR B1055-52 Psr 10 57 59.0450 -52 26 56.330           ~ 757 0
12 PSR J1107-5907 Psr 11 07 34.46 -59 07 18.7           ~ 42 0
13 PSR B1124-60 Psr 11 26 52.608 -60 54 39.96           ~ 27 0
14 PSR J1244-6531 Psr 12 44 38.3 -65 31 12           ~ 7 0
15 CPD-63 2495 HXB 13 02 47.6544015048 -63 50 08.626970292 10.34 10.72 9.98 10.03   O9.5Ve 852 0
16 PSR B1409-62 Psr 14 13 31.32000 -63 07 34.6000           ~ 38 0
17 PSR J1424-6438 Psr 14 24 59.20 -64 38 10.0           ~ 8 0
18 PSR J1549-4848 Psr 15 49 21.02700 -48 48 36.1000           ~ 55 0
19 PSR B1607-52 Psr 16 11 03.20 -52 09 23.6           ~ 48 0
20 PSR J1613-5234 Psr 16 13 57.49 -52 34 17.0           ~ 7 0
21 PSR J1627-4706 Psr 16 27 28.79 -47 06 49.3           ~ 18 0
22 PSR J1637-4450 Psr 16 37 53.15 -44 50 26.3           ~ 13 0
23 PSR B1634-45 Psr 16 37 58.710 -45 53 27.30           ~ 60 0
24 PSR B1702-19 Psr 17 05 36.09300 -19 06 39.2000           ~ 191 1
25 PSR J1713-3945 Psr 17 13 02.4438883512 -38 44 29.816068236           ~ 20 0
26 PSR B1719-37 Psr 17 22 59.17000 -37 12 03.0000           ~ 107 0
27 PSR B1734-35 Psr 17 37 40.039 -35 55 43.80           ~ 33 0
28 PSR B1736-29 Psr 17 39 34.28500 -29 03 03.9600           ~ 86 0
29 PSR B1803-19.3 Psr 18 06 06.6 -19 20 23           ~ 13 0
30 PSR J1808-1726 Psr 18 08 42.3 -17 26 27           ~ 9 0
31 PSR B1822-09 Psr 18 25 30.62000 -09 35 22.0000           ~ 382 0
32 PSR J1828-1101 Psr 18 28 18.849 -11 01 50.90           ~ 63 0
33 PSR J1842+0358 Psr 18 42 17.02 +03 58 35.3           ~ 14 0
34 PSR J1843-0702 Psr 18 43 22.44 -07 02 54.6           ~ 29 0
35 PSR J1849+0409 Psr 18 49 03.47 +04 09 42.3           ~ 20 0
36 PSR B1848+04 Psr 18 51 03.298 +04 18 12.00           ~ 45 0
37 PSR J1852-0118 Psr 18 52 17.15 -01 18 14.8           ~ 13 0
38 PSR J1903+0925 Psr 19 03 55.2 +09 25 55           ~ 14 0
39 PSR B1910+08.4 Psr 19 13 00.50 +08 32 05.1           ~ 25 0
40 PSR J1915+1410 Psr 19 15 35.42 +14 10 51.5           ~ 12 0
41 PSR B1929+10 Psr 19 32 14.0570 +10 59 33.380           ~ 801 0
42 PSR B1944+17 Psr 19 46 53.044 +18 05 41.24           ~ 252 0
43 PSR J2007+2722 Psr 20 07.0 +27 22           ~ 19 0
44 [MT91] 213 Psr 20 32 13.1247390384 +41 27 24.346666440 13.12 13.08 11.266     B0Vp 334 0
45 PSR J2047+5029 Psr 20 47 54.640 +50 29 38.17           ~ 18 0
46 PSR J2144-3939 Psr 21 44 12.01000 -39 33 58.4000           ~ 145 0

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