2025ApJ...987..119M


Query : 2025ApJ...987..119M

2025ApJ...987..119M - Astrophys. J., 987, 119 (2025/July-2)

Polarization Properties of Energetic Pulsars at Meterwavelengths.

MITRA D., BASU R. and MELIKIDZE G.I.

Abstract (from CDS):

Polarization behavior shows a transition in the pulsar population, where energetic sources with higher spin-down energy loss, $\dot{E}\gt 1{0}^{34}$ erg s–1, often have fractional linear polarization (L/I) close to 100%, while below this range L/I is usually lower than 50%. The polarization behavior has been primarily studied at higher frequencies above 1 GHz, and in this work, we explore the single-pulse polarization behavior in pulsars with $\dot{E}\gt 5\,\times 1{0}^{33}$ erg s–1 at a lower frequency range of 300-750 MHz. The polarization behavior can be divided into two categories, the first with L/I > 70% where the polarization position angle (PPA) follows a single track, and a second group with L/I < 70% and scattered PPA behavior with or without orthogonal modes. However, there are some single pulses in the first category that also have lower L/I and exhibit the presence of two polarization modes along orthogonal tracks. The radio emission in pulsars arises due to coherent curvature radiation (CCR) from charge bunches, which develops due to nonlinear instabilities in the pulsar plasma forming charge separated envelope solitons. The CCR excites orthogonally polarized X and O modes oriented perpendicular and parallel to the magnetic field line planes, which detach in the plasma and propagate independently. The O mode is 7 times stronger than the X mode but gets damped in the medium. We show that incoherent mixing of the X and O modes with different levels of damping can reproduce the observed polarization features in the energetic pulsar population.

Abstract Copyright: © 2025. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Radio pulsars

Simbad objects: 38

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Number of rows : 38
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 PSR B0114+58 Psr 01 17 38.661 +59 14 38.39           ~ 96 0
2 PSR B0136+57 Psr 01 39 19.744 +58 14 31.73     13.41     ~ 163 0
3 PSR B0950+08 Psr 09 53 09.31210 +07 55 36.9000           ~ 806 2
4 PSR B1634-45 Psr 16 37 58.710 -45 53 27.30           ~ 60 0
5 PSR J1705-3950 Psr 17 05 29.84 -39 50 59.0           ~ 45 0
6 PSR B1706-44 Psr 17 09 42.62000 -44 29 12.0000     13.30     ~ 670 1
7 PSR J1718-3825 Psr 17 18 13.558 -38 25 17.83           ~ 108 0
8 PSR B1730-37 Psr 17 33 26.754 -37 16 54.60           ~ 54 0
9 PSR B1736-29 Psr 17 39 34.28500 -29 03 03.9600           ~ 86 0
10 PSR J1739-3023 Psr 17 39 39.85 -30 23 11.2           ~ 54 0
11 PSR J1740+1000 Psr 17 40 25.91 +10 00 06.0           ~ 110 0
12 PSR B1737-30.2 Psr 17 40 33.98000 -30 15 22.0000           ~ 236 0
13 PSR B1754-24 Psr 17 57 29.37000 -24 19 54.0000           ~ 102 0
14 PSR B1800-21 Psr 18 03 51.40000 -21 37 07.0000           ~ 278 1
15 PSR J1809-1917 Psr 18 09 43.147 -19 17 38.10           ~ 128 1
16 PSR B1821-19 Psr 18 24 00.43600 -19 45 44.5000           ~ 101 0
17 PSR B1823-13 Psr 18 26 13.06 -13 34 48.1           ~ 460 1
18 PSR B1833-10.3 Psr 18 35 57.44000 -10 19 51.0000           ~ 35 0
19 PSR B1839-03.8 Psr 18 41 38.68 -03 48 42.6           ~ 44 0
20 PSR B1844-04 Psr 18 47 22.8222581784 -04 02 13.031112264           ~ 125 0
21 PSR B1853+01 Psr 18 56 10.65 +01 13 21.3           ~ 211 1
22 PSR J1913+0904 Psr 19 13 21.06 +09 04 45.4           ~ 31 0
23 PSR B1913+10 Psr 19 15 29.99300 +10 09 43.5800           ~ 102 0
24 PSR J1921+0812 Psr 19 21 47.704 +08 12 51.86           ~ 14 0
25 PSR J1922+1733 Psr 19 22 53.2180 +17 33 23.470           ~ 10 0
26 PSR B1930+20 Psr 19 32 08.023 +20 20 46.41           ~ 87 0
27 PSR B1929+10 Psr 19 32 14.0570 +10 59 33.380           ~ 801 0
28 PSR B1930+22 Psr 19 32 22.8565447656 +22 20 52.063074024     14.52     ~ 149 0
29 PSR J1935+2025 Psr 19 35 41.941 +20 25 40.10           ~ 39 0
30 PSR J1938+2213 Psr 19 38 14.180 +22 13 12.68           ~ 24 0
31 PSR B2000+32 Psr 20 02 04.424 +32 17 18.31           ~ 51 0
32 PSR J2006+3102 Psr 20 05.8 +30 51           ~ 19 0
33 PSR B2011+38 Psr 20 13 10.367 +38 45 43.31           ~ 78 0
34 PSR J2043+2740 Psr 20 43 43.5 +27 40 56           ~ 137 0
35 PSR J2144-3939 Psr 21 44 12.01000 -39 33 58.4000           ~ 145 0
36 PSR B2148+52 Psr 21 50 37.7499 +52 47 49.556           ~ 46 0
37 PSR J2229+6114 Psr 22 29 05.262 +61 14 08.48           ~ 252 2
38 PSR B2334+61 Psr 23 37 05.779 +61 51 01.69           ~ 206 1

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