2021
DOI: 10.1093/mnras/stab2976
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Radio modelling of the brightest and most luminous non-thermal colliding-wind binary Apep

Abstract: Apep is the brightest and most luminous non-thermal colliding-wind binary by over an order of magnitude. It has been suggested from infrared observations that one of the Wolf-Rayet stars in Apep is launching an anisotropic wind. Here we present radio observations of Apep from 0.2 to 20 GHz taken over 33 years. The spectrum reveals an extremely steep turnover in the flux density at low frequencies, where the flux density decreases by two orders of magnitude over only 325 MHz of bandwidth. This exponential decli… Show more

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Cited by 5 publications
(12 citation statements)
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“…In particular, by modelling the IR spiral plume, Han et al (2020) found the following orbital parameters for the Apep system: inclination i = 25 • ± 5 • , argument of periastron ω = 0 • ± 5 • , and true anomaly at 2018 epoch ν = −173 • ± 15 • . Similar values (within errors) were also obtained by Bloot et al (2021) by modelling the lightcurve at radio wavelengths. We can derive the corresponding projection angle for these parameters as ψ = arctan ( x 2 + y 2 /z), where x = D cos (ω − ν) cos (i), y = D sin (ω − ν), and z = D cos (ω − ν) sin (i) are the coordinates of the secondary star.…”
Section: Radio Emission Mapssupporting
confidence: 87%
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“…In particular, by modelling the IR spiral plume, Han et al (2020) found the following orbital parameters for the Apep system: inclination i = 25 • ± 5 • , argument of periastron ω = 0 • ± 5 • , and true anomaly at 2018 epoch ν = −173 • ± 15 • . Similar values (within errors) were also obtained by Bloot et al (2021) by modelling the lightcurve at radio wavelengths. We can derive the corresponding projection angle for these parameters as ψ = arctan ( x 2 + y 2 /z), where x = D cos (ω − ν) cos (i), y = D sin (ω − ν), and z = D cos (ω − ν) sin (i) are the coordinates of the secondary star.…”
Section: Radio Emission Mapssupporting
confidence: 87%
“…Dougherty et al 2003). Thus, we expect that the actual impact of the wind anisotropies in the radio SED to be less significant than implied by Bloot et al (2021). With respect to the spherical wind approximation in our model, depending on the geometry of the system and the winds anisotropy, the anisotropy in the winds could potentially increase the opacity in the direction of the line of sight for photons coming from close to the bright apex of the WCR.…”
Section: Radio Spectral Energy Distributionmentioning
confidence: 89%
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