2024ApJ...970...78G


Query : 2024ApJ...970...78G

2024ApJ...970...78G - Astrophys. J., 970, 78 (2024/July-3)

Discovery and Follow-up of a Quasiperiodically Nulling and Subpulse Drifting Pulsar with the Murchison Widefield Array.

GROVER G., BHAT N.D.R., McSWEENEY S.J., LEE C.P., MEYERS B.W., TAN C.M. and KUDALE S.S.

Abstract (from CDS):

The phenomenon of pulsar nulling, where pulsars temporarily and stochastically cease their radio emission, is thought to be indicative of a “dying” pulsar, where radio emission ceases entirely. Here we report the discovery of a long-period pulsar, PSR J0452-3418, from the ongoing Southern-sky MWA Rapid Two-meter pulsar survey. The pulsar has a rotation period of ∼1.67 s and a dispersion measure of 19.8 pc cm–3, and it exhibits both quasiperiodic nulling and subpulse drifting. Periodic nulling is uncommon, reported in only <1% of the pulsar population, with even a smaller fraction showing periodic nulling and subpulse drifting. We describe the discovery and follow-up of the pulsar, including a positional determination using high-resolution imaging with the upgraded Giant Metrewave Radio Telescope (uGMRT), initial timing analysis using the combination of Murchison Widefield Array (MWA) and uGMRT data, and detailed characterization of the nulling and drifting properties in the MWA's frequency band (140-170 MHz). Our analysis suggests a nulling fraction of 34% ± 6% and a nulling periodicity of ${42}_{-1.3}^{+1.5}$ pulses. We measure the phase (P2) and time modulation (P3) caused by the subpulse drifting, with an average P2 of 7.1${}_{-3.1}^{+26.3}$ degrees and a P3 of 4.8${}_{-0.9}^{+1.5}$ pulses. We compare and contrast the observed properties with those of other pulsars that exhibit subpulse drifting and quasiperiodic nulling phenomena, and find that the majority of these objects tend to be in the “death valley” in the period-period derivative (P-$\dot{P}$) diagram. We also discuss some broader implications for pulsar emission physics and the detectability of similar objects using next-generation pulsar surveys.

Abstract Copyright: © 2024. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Pulsars - Radio pulsars - Time domain astronomy - High energy astrophysics

Simbad objects: 26

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Number of rows : 26
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 J0026-1955 Psr 00 26.0 -19 55           ~ 7 0
2 PSR B0031-07 Psr 00 34 08.9100 -07 21 56.000           ~ 350 0
3 PSR J0036-1033 Psr 00 36 15.01 -10 33 14.2           ~ 3 0
4 PSR B0301+19 Psr 03 04 33.115 +19 32 51.40           ~ 247 0
5 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 1032 0
6 PSR J0448-2757 Psr 04 48 41.567 -27 49 46.74           ~ 27 0
7 PSR J0452-3418 Psr 04 52 00.7 -34 18 42           ~ 3 0
8 PSR B0834+06 Psr 08 37 05.64620 +06 10 15.8700           ~ 472 0
9 PSR B0932-52 Psr 09 34 28.23700 -52 49 27.3000           ~ 55 0
10 PSR B0950+08 Psr 09 53 09.31210 +07 55 36.9000           ~ 806 2
11 PSR J1047-6711 Psr 10 47 28.28500 -67 09 51.6100           ~ 34 0
12 PSR B1237+25 Psr 12 39 40.386 +24 53 49.87           ~ 497 1
13 PSR B1322-66 Psr 13 26 02.70600 -67 00 50.1000           ~ 55 0
14 PSR J1357-2530 Psr 13 57 24.0 -25 30 39           ~ 1 0
15 PSR J1631+1252 Psr 16 31 43 +12 52.1           ~ 5 0
16 PSR B1658-37 Psr 17 01 18.45000 -37 26 27.2000           ~ 45 0
17 PSR J1727-2739 Psr 17 27 30.98000 -27 38 53.0000           ~ 51 0
18 PSR B1738-08 Psr 17 41 22.5629 -08 40 31.711           ~ 98 0
19 PSR B1819-22 Psr 18 22 58.95000 -22 56 29.0000           ~ 123 0
20 PSR B1918+19 Psr 19 21 03.799 +19 48 44.70           ~ 119 0
21 PSR B1944+17 Psr 19 46 53.044 +18 05 41.24           ~ 252 0
22 PSR B2003-08 Psr 20 06 16.36500 -08 07 02.1600           ~ 113 0
23 PSR B2045-16 Psr 20 48 35.74000 -16 16 45.0000           ~ 344 0
24 PSR B2303+30 Psr 23 05 58.3212 +31 00 01.281           ~ 216 0
25 PSR B2310+42 Psr 23 13 08.5976 +42 53 12.987           ~ 147 0
26 PSR B2319+60 Psr 23 21 55.213 +60 24 30.71     13.80     ~ 200 0

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