1983
DOI: 10.1070/pu1983v026n11abeh004545
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Electrodynamics of the magnetosphere of pulsars

Abstract: Abslracl. In its 1990 rmommendations, ICRP published information on the fatal cancer risk of chronic exposure to radiation. Calculations of the same form were repeated in a report by the first author using health effeds information specific to a UK population. For wnstant annual doses over a complete lifetime, the UK estimates are broadly consistent with those given by ICRP and BEIR. However, because differences exisi in the methodologies used, this may not be true of more realistic exposure situations. For th… Show more

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Cited by 48 publications
(95 citation statements)
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“…Acceleration will then occur in a narrow region very close to the light surface with Δr/r L ∼ 1/M. This seems reminiscent of earlier results about particle acceleration in the presence of small longitudinal currents (Beskin et al 1983;Beskin & Rafikov 2000).…”
Section: Co-rotation Constraintssupporting
confidence: 60%
“…Acceleration will then occur in a narrow region very close to the light surface with Δr/r L ∼ 1/M. This seems reminiscent of earlier results about particle acceleration in the presence of small longitudinal currents (Beskin et al 1983;Beskin & Rafikov 2000).…”
Section: Co-rotation Constraintssupporting
confidence: 60%
“…(1) with C ≈ 0.8R √ I 45 [34]. As shown in [28], this result does not contradict to the model [32,33].…”
Section: Magnetic Fieldssupporting
confidence: 69%
“…According to the model by Beskin et al [32,33], the magnetodipole radiation is absent beyond the magnetosphere, while the slowdown of rotation is provided by the current energy losses. However, the the relation between B and PṖ remains similar.…”
Section: Magnetic Fieldsmentioning
confidence: 99%
“…Thinner gaps (with sizes h < r g ) can however exist as well and might also be expected in the context of degenerate, force-free outflows (i.e., in ideal MHD). As an example, we mention the null surface (located close to r g ) formed due to the frame-dragging effect (Beskin et al 1992;Hirotani & Okamoto 1998) and the stagnation surface (typically located at a few r g ) which divides MHD inflow from outflow regions (e.g., Globus & Levinson 2014;Broderick & Tchekhovskoy 2015). In these places, continuous charge replenishment (by particle creation or diffusion) has to occur in order to sustain the required Goldreich-Julian charge density ρ GJ = −e n GJ −Ω F B ⊥ /(2πc).…”
Section: Magnetospheric Emissionmentioning
confidence: 99%