2001
DOI: 10.1086/321365
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On Optical Synchrotron Emission of Radio Pulsars

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Cited by 34 publications
(29 citation statements)
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“…Models for the optical emission from the Crab pulsar based on the synchrotron mechanism often aim at reproducing the maximum frequency in the optical range (ν m ∼ 5 × 10 14 Hz, eg., Stoneham 1981;Mavlov & Machabeli 2001;Lyne & Graham-Smith 1998). This is mainly based on the observations by Oke (1969), and is not supported by the more recent observations presented in Sollerman et al (2000).…”
Section: The Pulsarmentioning
confidence: 74%
“…Models for the optical emission from the Crab pulsar based on the synchrotron mechanism often aim at reproducing the maximum frequency in the optical range (ν m ∼ 5 × 10 14 Hz, eg., Stoneham 1981;Mavlov & Machabeli 2001;Lyne & Graham-Smith 1998). This is mainly based on the observations by Oke (1969), and is not supported by the more recent observations presented in Sollerman et al (2000).…”
Section: The Pulsarmentioning
confidence: 74%
“…Non-thermal models for the optical radiation of slower pulsars like the Crab ascribe it to synchrotron emission (see Pacini 1971 andPacini &Salvati 1987) by relativistic particles near the light cylinder radius at very small pitch angles (Ψ 1/γ, where the Lorentz factor may be γ ∼ 10 2 −10 3 ; Crusius-Wätzel et al 2001). Malov & Machabeli (2001) show that finite pitch angles of the plasma particles appear in the outer magnetosphere near the light cylinder due to an instability associated with the cyclotron resonance condition being fulfilled there. They further show that pulsars with shorter periods such as the MSPs attain harder spectra and higher peak frequencies.…”
Section: Discussionmentioning
confidence: 91%
“…As we already mentioned in the introduction, the timescale is very short for the transit to the ground Landau state that provides quasi-one-dimensional motion of electrons along the field lines without radiation. As investigated in a series of papers (Machabeli & Usov 1979;Malov & Machabeli 2001), the cyclotron instability of the electron-positron plasma under certain conditions, may however "create" pitch angles, which activate the subsequent synchrotron process. We consider the plasma to consist of two components: (a) the electron-positron plasma component with the Lorentz factor, γ p and (b) highly relativistic electrons, the so-called beam component with the Lorentz factor, γ b (γ b γ p ).…”
Section: Main Considerationmentioning
confidence: 99%