2021A&A...654A..43G


Query : 2021A&A...654A..43G

2021A&A...654A..43G - Astronomy and Astrophysics, volume 654A, 43-43 (2021/10-1)

Follow-up of 27 radio-quiet gamma-ray pulsars at 110-190 MHz using the international LOFAR station FR606.

GRIESSMEIER J.-M., SMITH D.A., THEUREAU G., JOHNSON T.J., KERR M., BONDONNEAU L., COGNARD I. and SERYLAK M.

Abstract (from CDS):


Context. The Fermi Large Area Telescope has detected over 260 gamma-ray pulsars. About one quarter of these are labeled as radio-quiet, that is they either have radio flux densities < 30 µJy at 1400 MHz, or they are not detected at all in the radio domain. In the population of nonrecycled gamma-ray pulsars, the fraction of radio-quiet pulsars is higher, about one half.
Aims. Most radio observations of gamma-ray pulsars have been performed at frequencies between 300 MHz and 2 GHz. However, pulsar radio fluxes increase rapidly with decreasing frequency, and their radio beams often broaden at low frequencies. As a consequence, some of these pulsars might be detectable at low radio frequencies even when no radio flux is detected above 300 MHz. Our aim is to test this hypothesis with low-frequency radio observations.
Methods. We have observed 27 Fermi-discovered gamma-ray pulsars with the international LOw Frequency ARray (LOFAR) station FR606 in single-station mode. We used the LOFAR high band antenna band (110-190 MHz), with an average observing time of 13 h per target. Part of the data had to be discarded due to radio frequency interference. On average, we kept 9 h of observation per target after the removal of affected datasets, resulting in a sensitivity for pulse-averaged flux on the order of 1-10 mJy.
Results. We do not detect radio pulsations from any of the 27 sources, and we establish stringent upper limits on their low-frequency radio fluxes. These nondetections are compatible with the upper limits derived from radio observations at other frequencies. We also determine the pulsars' geometry from the gamma-ray profiles to see for which pulsars the low-frequency radio beam is expected to cross Earth.
Conclusions. This set of observations provides the most constraining upper limits on the flux density at 150 MHz for 27 radio-quiet gamma-ray pulsars. In spite of the beam-widening expected at low radio frequencies, most of our nondetections can be explained by an unfavorable viewing geometry; for the remaining observations, especially those of pulsars detected at higher frequencies, the nondetection is compatible with insufficient sensitivity.

Abstract Copyright: © J.-M. Grießmeier et al. 2021

Journal keyword(s): pulsars: general - telescopes - ISM: general

Simbad objects: 29

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Number of rows : 29
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2023
#notes
1 PSR J0002+6216 Psr 00 02 58.17 +62 16 09.4           ~ 28 0
2 PSR J0007+7303 Psr 00 06 34.20 +73 11 06.6           ~ 167 1
3 PSR J0106+4855 Psr 01 06 25.030 +48 55 52.01           ~ 41 0
4 PSR B0105+68 Psr 01 08 29.500 +69 05 52.63           ~ 29 0
5 PSR J0357+32 Psr 03 57 52.161 +32 05 23.63           ~ 89 0
6 PSR J0359+5414 Psr 03 59 26.01 +54 14 55.7           ~ 17 0
7 PSR J0554+3107 Psr 05 54 11.5 +31 07 03           ~ 18 0
8 PSR J0622+3749 Psr 06 22 10.411 +37 49 14.60           ~ 40 1
9 PSR J0631+0646 Psr 06 31 52.38 +06 46 14.2           ~ 14 0
10 PSR J0633+0632 Psr 06 33 44.136 +06 32 29.48           ~ 73 1
11 NAME Geminga Psr 06 33 54.153 +17 46 12.91           ~ 1193 0
12 PSR J1836+5925 Psr 18 36 13.661 +59 25 29.77           ~ 136 1
13 PSR J1838-0537 Psr 18 38 56.02 -05 37 09.0           ~ 39 0
14 PSR J1846+0919 Psr 18 46 25.864 +09 19 48.99           ~ 29 0
15 PSR J1906+0722 Psr 19 06 31.20 +07 22 55.8           ~ 25 0
16 PSR J1907+06 Psr 19 07 54.751 +06 02 15.79           ~ 122 0
17 PSR J1932+1916 Psr 19 32 19.775 +19 16 38.06           ~ 23 0
18 PSR J1954+2836 Psr 19 54 19.144 +28 36 04.84           ~ 48 0
19 PSR J1957+5033 Psr 19 57 38.391 +50 33 21.24           ~ 33 0
20 PSR J1958+2846 Psr 19 58 40.1015582448 +28 45 54.108736344           ~ 65 0
21 PSR J2017+3625 Psr 20 17 55.84 +36 25 07.9           ~ 24 0
22 PSR J2021+4026 Psr 20 21 30.496 +40 26 53.56           ~ 269 2
23 PSR J2028+3332 Psr 20 28 19.876 +33 32 04.23           ~ 58 0
24 PSR J2030+4415 Psr 20 30 51.396 +44 15 38.73           ~ 52 0
25 [MT91] 213 Be* 20 32 13.1247390384 +41 27 24.346666440 13.12 13.08 11.266     B0Vp 275 0
26 PSR J2055+25 Psr 20 55 48.948 +25 39 58.93           ~ 47 0
27 PSR J2111+4606 Psr 21 11 24.125 +46 06 30.66           ~ 36 0
28 PSR J2139+4716 Psr 21 39 55.878 +47 16 13.12           ~ 29 0
29 PSR J2238+5903 Psr 22 38 28.089 +59 03 43.37           ~ 29 0

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2023.10.04-18:14:30

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