1993
DOI: 10.1086/172130
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Particle acceleration and nonthermal radio emission in binaries of early-type stars

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Cited by 351 publications
(492 citation statements)
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“…The models were aimed to describe the symbiotic systems and gamma-ray binaries, and also binary systems with O-type and Wolf-Rayet stars including the enigmatic object in η-Carinae. The colliding wind binaries were long known to be sources of non-thermal radio emission Eichler and Usov (1993), Dougherty et al (2005), Pittard and Dougherty (2006), De Becker (2007) and the catalog of colliding wind binaries with non-thermal particle acceleration compiled by De Becker and Raucq (2013) contains 43 objects.…”
Section: Colliding Wind Binariesmentioning
confidence: 99%
“…The models were aimed to describe the symbiotic systems and gamma-ray binaries, and also binary systems with O-type and Wolf-Rayet stars including the enigmatic object in η-Carinae. The colliding wind binaries were long known to be sources of non-thermal radio emission Eichler and Usov (1993), Dougherty et al (2005), Pittard and Dougherty (2006), De Becker (2007) and the catalog of colliding wind binaries with non-thermal particle acceleration compiled by De Becker and Raucq (2013) contains 43 objects.…”
Section: Colliding Wind Binariesmentioning
confidence: 99%
“…For Cyg OB2 #8A, we adopted a radial dependence of the magnetic field (Eichler & Usov, 1993). The collision zone is indeed closer to the stars than in the case considered by Benaglia et al (2001).…”
Section: Cyg Ob2 #8a In the Context Of This Scenariomentioning
confidence: 99%
“…The acceleration of relativistic electrons responsible for non-thermal emission (radio, X-rays, γ-rays) is believed to occur within the interaction zone of the colliding winds of the binary system (Eichler & Usov, 1993). The IC scattering of UV photons of Cyg OB2 #8A is expected to account for 8-10 % of the γ-ray luminosity of the unidentified EGRET source 3EG J2033+4118.…”
Section: Prospects and Conclusionmentioning
confidence: 99%
“…With momentum ratio η ∼ 10, the opening angle of the cone-like shock is ∼ 50 − 60 • (c.f. Eichler & Usov 1993;Canto et al 1996), which corresponds to ∼ 0.15 orbital phase. Because the emission is concentrated in the forward direction of the flow, therefore, we expect that double peaks due to the Doppler effect appear at ∼ 0.15 phase before and after the phase of radio eclipse, which is consistent with the observation.…”
Section: Discussionmentioning
confidence: 99%