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Dispersion measure variability for 36 millisecond pulsars at 150 MHz with LOFAR
- Source :
- Astronomy and Astrophysics, Astronomy and Astrophysics-A&A, Astronomy and Astrophysics-A&A, EDP Sciences, 2020, 644, pp.A153. ⟨10.1051/0004-6361/202039517⟩, Astronomy & Astrophysics
- Publication Year :
- 2020
-
Abstract
- Radio pulses from pulsars are affected by plasma dispersion, which results in a frequency-dependent propagation delay. Variations in the magnitude of this effect lead to an additional source of red noise in pulsar timing experiments, including pulsar timing arrays that aim to detect nanohertz gravitational waves. We aim to quantify the time-variable dispersion with much improved precision and characterise the spectrum of these variations. We use the pulsar timing technique to obtain highly precise dispersion measure (DM) time series. Our dataset consists of observations of 36 millisecond pulsars, which were observed for up to 7.1 years with the LOFAR telescope at a centre frequency of ~150 MHz. Seventeen of these sources were observed with a weekly cadence, while the rest were observed at monthly cadence. We achieve a median DM precision of the order of 10^-5 cm^-3 pc for a significant fraction of our sources. We detect significant variations of the DM in all pulsars with a median DM uncertainty of less than 2x10^-4 cm^-3 pc. The noise contribution to pulsar timing experiments at higher frequencies is calculated to be at a level of 0.1-10 us at 1.4 GHz over a timespan of a few years, which is in many cases larger than the typical timing precision of 1 us or better that PTAs aim for. We found no evidence for a dependence of DM on radio frequency for any of the sources in our sample. The DM time series we obtained using LOFAR could in principle be used to correct higher-frequency data for the variations of the dispersive delay. However, there is currently the practical restriction that pulsars tend to provide either highly precise times of arrival (ToAs) at 1.4 GHz or a high DM precision at low frequencies, but not both, due to spectral properties. Combining the higher-frequency ToAs with those from LOFAR to measure the infinite-frequency ToA and DM would improve the result.<br />Comment: 16 pages, 8 figures, 2 tables
- Subjects :
- ISM: structure
Astrophysics::High Energy Astrophysical Phenomena
FOS: Physical sciences
Astrophysics
01 natural sciences
law.invention
Telescope
Pulsar
Millisecond pulsar
law
pulsars: general
0103 physical sciences
Dispersion (optics)
010303 astronomy & astrophysics
Physics
High Energy Astrophysical Phenomena (astro-ph.HE)
[PHYS]Physics [physics]
010308 nuclear & particles physics
Gravitational wave
Astrophysics::Instrumentation and Methods for Astrophysics
Astronomy and Astrophysics
LOFAR
Astrophysics - Astrophysics of Galaxies
gravitational waves
Space and Planetary Science
[SDU]Sciences of the Universe [physics]
Astrophysics of Galaxies (astro-ph.GA)
ddc:520
Radio frequency
Astrophysics - High Energy Astrophysical Phenomena
[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]
Noise (radio)
Subjects
Details
- ISSN :
- 00046361
- Database :
- OpenAIRE
- Journal :
- Astronomy and Astrophysics, Astronomy and Astrophysics-A&A, Astronomy and Astrophysics-A&A, EDP Sciences, 2020, 644, pp.A153. ⟨10.1051/0004-6361/202039517⟩, Astronomy & Astrophysics
- Accession number :
- edsair.doi.dedup.....2a4e92372b414bfc499dee76c8d23e59
- Full Text :
- https://doi.org/10.1051/0004-6361/202039517⟩