2020
DOI: 10.48550/arxiv.2010.09723
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Scintillation of PSR B1508+55 -- the view from a 10,000-km baseline

V. R. Marthi,
D. Simard,
R. A. Main
et al.

Abstract: We report on the simultaneous Giant Metrewave Radio Telescope (GMRT) and Algonquin Radio Observatory (ARO) observations at 550-750 MHz of the scintillation of PSR B1508+55, resulting in a ∼10,000-km baseline. This regime of measurement lies between the shorter few 100-1000 km baselines of earlier multi-station observations and the much longer earth-space baselines. We measure a scintillation cross-correlation coefficient of 0.22, offset from zero time lag due to a ∼ 45 s traversal time of the scintillation pat… Show more

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Cited by 3 publications
(3 citation statements)
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“…The inverted arclets arise from mutual interference between the scattered images, and their sharpness is a signature of highly anisotropic scattering, where the scattered images of the pulsar lie along a (nearly) straight line (Walker et al 2004). Like in previous observations, we find that the arclets move along the scintillation arc at a constant speed for long periods of time (Hill et al 2005;Marthi et al 2020). This implies that the scattered images giving rise to the arclets must arise from a large group of parallel and elongated structures in the scattering screen, e.g., turbulence elongated along a given direction (Goldreich & Sridhar 1995), waves on a plasma sheet seen in projection as folds (Romani et al 1987;Pen & Levin 2014), or magnetic noodles of plasma stabilized by reconnection (Gwinn 2019).…”
Section: Observation and Pulsar Scintillationsupporting
confidence: 80%
“…The inverted arclets arise from mutual interference between the scattered images, and their sharpness is a signature of highly anisotropic scattering, where the scattered images of the pulsar lie along a (nearly) straight line (Walker et al 2004). Like in previous observations, we find that the arclets move along the scintillation arc at a constant speed for long periods of time (Hill et al 2005;Marthi et al 2020). This implies that the scattered images giving rise to the arclets must arise from a large group of parallel and elongated structures in the scattering screen, e.g., turbulence elongated along a given direction (Goldreich & Sridhar 1995), waves on a plasma sheet seen in projection as folds (Romani et al 1987;Pen & Levin 2014), or magnetic noodles of plasma stabilized by reconnection (Gwinn 2019).…”
Section: Observation and Pulsar Scintillationsupporting
confidence: 80%
“…The inverted arclets arise from mutual interference between the scattered images, and their sharpness is a signature of highly anisotropic scattering, where the scattered images of the pulsar lie along a (nearly) straight line (Walker et al 2004). Like in previous observations, we find that the arclets move along the scintillation arc at a constant speed for long periods of time (Hill et al 2005;Marthi et al 2020). This implies that the scattered images giving rise to the arclets must arise from a large group of parallel and elongated structures in the scattering screen, e.g., turbulence elongated along a given direction (Goldreich & Sridhar 1995), waves on a plasma sheet seen in projection as folds (Romani et al 1987;Pen & Levin 2014), or magnetic noodles of plasma stabilized by reconnection (Gwinn 2019).…”
Section: Observation and Pulsar Scintillationsupporting
confidence: 80%
“…Generally, DM events are more likely to be detected if the scattering/lensing direction is closely aligned with the pulsar's motion (c.f. scattering and proper motion alignment in PSR B1508+55, Wucknitz 2019; Marthi et al 2020).…”
Section: Mjdmentioning
confidence: 99%