2022ApJ...940..110H


Query : 2022ApJ...940..110H

2022ApJ...940..110H - Astrophys. J., 940, 110 (2022/December-1)

Simulation for Distributions of Several Geometric Parameters in Nulling Pulsars.

HAN X.H. and YUEN R.

Abstract (from CDS):

We investigate the distributions of the obliquity angle and impact parameters of nulling pulsars of different duty cycles based on the simulation of more than 600,000 samples. We adopt a purely geometric approach for pulsar visibility, in which visible emission is emitted tangentially to the magnetic field line and parallel to the line-of-sight direction. The geometry is incorporated with the model for pulsar magnetospheres of multiple emission states, in which the plasma charge density is dependent on the emission state. We assume that an emission state can only exist between two limiting conditions described by the vacuum and corotation models, respectively. In this model, pulse nulling corresponds to emission switching to a state in which the plasma charge density is zero. The event is detectable only if the switching occurs at source points that lie on a trajectory, whose locus defines the locations of visible emission, within an open-field region. Our results show that detectable nulling is dependent on all three parameters, such that nulling pulsars prefer a small obliquity angle and duty cycle, and tend to have positive impact parameters. We find that the total population of nulling pulsars in our samples is around 23%, of which about 47% possess a duty cycle of 0.1 or smaller. The former implies that there are more nulling pulsars than currently known. Our model predicts that the number of nulling pulsars increases as the obliquity angle decreases, which also implies that the occurrence of nulling in a pulsar should evolve over time.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Radio pulsars

Simbad objects: 59

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Number of rows : 59
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 PSR B0148-06 Psr 01 51 22.7400 -06 35 03.900           ~ 105 0
2 PSR B0149-16 Psr 01 52 10.8520 -16 37 53.900           ~ 123 0
3 PSR B0301+19 Psr 03 04 33.115 +19 32 51.40           ~ 224 0
4 PSR B0329+54 Psr 03 32 59.3370698592 +54 34 45.028206408           ~ 645 1
5 PSR J0344-0901 Psr 03 44 37.471 -09 01 02.66           ~ 2 0
6 PSR B0450-18 Psr 04 52 34.1150 -17 59 23.300           ~ 187 0
7 PSR B0523+11 Psr 05 25 56.5000 +11 15 19.100           ~ 116 0
8 PSR B0525+21 Psr 05 28 52.308 +22 00 01.00     14.30     ~ 356 0
9 PSR B0538-75 Psr 05 36 30.8200 -75 43 54.800           ~ 68 0
10 PSR B0628-28 Psr 06 30 49.3710 -28 34 42.200           ~ 295 0
11 PSR B0656+14 Psr 06 59 48.1960 +14 14 19.400   24.85 24.90     ~ 869 1
12 PSR B0736-40 Psr 07 38 32.2620 -40 42 39.420           ~ 196 0
13 PSR B0809+74 Psr 08 14 59.500 +74 29 05.70           ~ 406 0
14 PSR B0818-13 Psr 08 20 26.4020 -13 50 56.400           ~ 211 0
15 PSR B0823+26 Psr 08 26 51.5068 +26 37 21.297           ~ 512 1
16 PSR B0826-34 Psr 08 28 16.6 -34 17 07           ~ 156 0
17 PSR B0834+06 Psr 08 37 05.642 +06 10 14.56           ~ 437 0
18 PSR B0835-41 Psr 08 37 21.1943 -41 35 14.563     12.69     ~ 136 0
19 PSR B0940-55 Psr 09 42 15.83 -55 52 52.3           ~ 86 0
20 PSR B1055-52 Psr 10 57 59.0450 -52 26 56.330           ~ 725 0
21 PSR B1133+16 Psr 11 36 03.0720 +15 51 15.500           ~ 668 0
22 PSR B1154-62 Psr 11 57 15.2070 -62 24 50.930           ~ 105 0
23 PSR B1237+25 Psr 12 39 40.386 +24 53 49.87           ~ 468 0
24 PSR B1451-68 Psr 14 56 00.0175876848 -68 43 40.034742348           ~ 186 0
25 PSR B1508+55 Psr 15 09 25.7 +55 31 33           ~ 301 1
26 PSR B1642-03 Psr 16 45 02.0330 -03 17 57.200           ~ 363 0
27 PSR B1700-32 Psr 17 03 22.5200 -32 41 48.300           ~ 106 0
28 PSR B1706-16 Psr 17 09 26.4470 -16 40 56.200           ~ 222 0
29 PSR B1718-32 Psr 17 22 02.9590 -32 07 45.300           ~ 90 0
30 PSR B1727-47 Psr 17 31 42.103 -47 44 34.56           ~ 148 0
31 PSR B1737+13 Psr 17 40 07.3455 +13 11 56.690           ~ 175 0
32 PSR B1738-08 Psr 17 41 22.5629 -08 40 31.711           ~ 86 0
33 PSR B1747-46 Psr 17 51 42.1960 -46 57 26.530           ~ 111 0
34 PSR B1749-28 Psr 17 52 58.7130 -28 06 33.900           ~ 261 0
35 PSR J1819+1305 Psr 18 19 56.226 +13 05 15.25           ~ 35 0
36 PSR B1819-22 Psr 18 22 59.0000 -22 56 38.000           ~ 113 0
37 PSR B1821+05 Psr 18 23 30.9731 +05 50 24.310           ~ 123 0
38 PSR B1839+09 Psr 18 41 55.9380 +09 12 08.300           ~ 122 0
39 PSR B1845-19 Psr 18 48 18.03 -19 52 31.0           ~ 71 0
40 PSR B1857-26 Psr 19 00 47.5440 -26 00 44.200           ~ 180 0
41 PSR B1907+03 Psr 19 10 09.06 +03 58 28.0     14.10     ~ 88 0
42 PSR B1911-04 Psr 19 13 54.1820 -04 40 47.600           ~ 173 0
43 PSR B1917+00 Psr 19 19 50.6820 +00 21 39.600           ~ 105 0
44 PSR B1918+19 Psr 19 21 03.799 +19 48 44.70           ~ 108 0
45 PSR B1919+21 Psr 19 21 44.815 +21 53 02.25           ~ 384 0
46 PSR B1929+10 Psr 19 32 14.0570 +10 59 33.380           ~ 753 0
47 PSR B1933+16 Psr 19 35 47.7011639352 +16 16 40.034899524           ~ 302 1
48 PSR B1942-00 Psr 19 45 28.39 -00 40 58.1           ~ 59 0
49 PSR B1946+35 Psr 19 48 25.0067 +35 40 11.057           ~ 168 0
50 PSR B2003-08 Psr 20 06 16.3650 -08 07 02.167           ~ 101 0
51 PSR B2016+28 Psr 20 18 03.8999255016 +28 39 54.940329468           ~ 356 0
52 PSR B2020+28 Psr 20 22 37.0671 +28 54 23.104           ~ 306 1
53 PSR B2044+15 Psr 20 46 39.3373 +15 40 33.558           ~ 98 0
54 PSR B2045-16 Psr 20 48 35.7700 -16 16 47.000           ~ 319 0
55 PSR B2111+46 Psr 21 13 24.3295 +46 44 08.844           ~ 208 1
56 PSR B2154+40 Psr 21 57 01.840 +40 17 45.89           ~ 146 0
57 PSR B2310+42 Psr 23 13 08.5976 +42 53 12.987           ~ 135 0
58 PSR B2319+60 Psr 23 21 55.213 +60 24 30.71     13.80     ~ 191 0
59 PSR J2338+4818 Psr 23 38 06.189 +48 18 32.19           ~ 2 0

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