2000
DOI: 10.1046/j.1365-8711.2000.03250.x
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Very-high-energy gamma radiation associated with the unshocked wind of the Crab pulsar

Abstract: We show that the relativistic wind of the Crab pulsar, which is commonly thought to be invisible in the region upstream of the termination shock at rrS∼0.1 pc, in fact could be directly observed through its inverse Compton (IC) γ‐ray emission. This radiation is caused by illumination of the wind by low‐frequency photons emitted by the pulsar, and consists of two, pulsed and unpulsed, components associated with the non‐thermal (pulsed) and thermal (unpulsed) low‐energy radiation of the pulsar, respectively. The… Show more

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Cited by 81 publications
(99 citation statements)
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References 30 publications
(47 reference statements)
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“…Nevertheless, they are (potentially) visible owing to the characteristic inverse Compton radiation of the ultrarelativistic electrons of the wind (Bogovalov & Aharonian 2000). For isolated pulsars, a sharp gamma-ray line can be produced at Comptonization of the electron-positron wind by thermal X-rays arriving from the surface of the neutron star.…”
Section: Astrophysical Vhe Gamma-ray Lines?mentioning
confidence: 99%
See 1 more Smart Citation
“…Nevertheless, they are (potentially) visible owing to the characteristic inverse Compton radiation of the ultrarelativistic electrons of the wind (Bogovalov & Aharonian 2000). For isolated pulsars, a sharp gamma-ray line can be produced at Comptonization of the electron-positron wind by thermal X-rays arriving from the surface of the neutron star.…”
Section: Astrophysical Vhe Gamma-ray Lines?mentioning
confidence: 99%
“…For isolated pulsars, a sharp gamma-ray line can be produced at Comptonization of the electron-positron wind by thermal X-rays arriving from the surface of the neutron star. The mechanism can be effective only if the conversion of the Poynting flux to kinetic energy of the bulk motion ("acceleration" of the wind) takes place close to the light cylinder (Bogovalov & Aharonian 2000). In the case of pulsars with bright nonthermal broad-band magnetospheric emission, e.g.…”
Section: Astrophysical Vhe Gamma-ray Lines?mentioning
confidence: 99%
“…In fact, synchrotron self-absorption has not been computed within the considered jet region to account roughly for the radio emission produced outside it. We compute the synchrotron (Pacholczyk 1970) as well as the inverse Compton emission, and the latter is calculated by taking into account KN and angular effects (Bogovalov & Aharonian 2000;Dermer & Böttcher 2006) in the interaction between electrons and photons. The photon-photon opacities due to the ambient photon field are also computed, taking into account angular effects for stellar photons (Gould & Schréder 1967) and adopting the point-like approximation for the stellar radiation (CD photon field is isotropic when dominant).…”
Section: Modeling Radiative Processes In Ls I +61 303mentioning
confidence: 99%
“…Within these models one can explain the gamma-ray emission of the blazar 1ES 229+200 at z = 0.139 with the spectrum extending up to several TeV [7] and sub-TeV gamma-ray emission from 3C 279 at z = 0.536 [8] (Γ s ∼ 1). Formally, much harder spectra can be expected in the case of Comptonization of an ultrarelativistic outflow [9], in analogy with the cold electron-positron winds in pulsars [10]. Although it is not clear how the ultrarelativistic MHD outflows could form in AGN with a bulk motion Lorentz factor γ ∼ 10 6 , such a scenario, leading to the Klein-Nishina gamma-ray linetype emission [11], cannot be excluded ab initio.…”
Section: Introductionmentioning
confidence: 99%