1998
DOI: 10.1046/j.1365-8711.1998.01990.x
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Non-stationary pair plasma in a pulsar magnetosphere and the two-stream Instability

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Cited by 110 publications
(147 citation statements)
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“…This mechanism is consistent with other forms of indirect radiation mechanisms, where primary effects generate secondary electromagnetic effects (Melrose 1993;Asseo & Melikidze 1998;Melikidze et al 2000;Asseo & Riazuelo 2000). There are however two main differences.…”
Section: Introductionsupporting
confidence: 86%
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“…This mechanism is consistent with other forms of indirect radiation mechanisms, where primary effects generate secondary electromagnetic effects (Melrose 1993;Asseo & Melikidze 1998;Melikidze et al 2000;Asseo & Riazuelo 2000). There are however two main differences.…”
Section: Introductionsupporting
confidence: 86%
“…Second, the primary process is not strictly thermal, as seen in Paper I, but it might be a stochastic perturbation induced in the rest frame either directly by the quasiclassical process as described by da Costa & Kahn (1997), or other possible phenomena, as the presence of complex non-thermal plasma density distribution functions which will act to produce non-thermal phenomena similar to the one described by Asseo & Melikidze (1998).…”
Section: Introductionmentioning
confidence: 99%
“…Usov (1987) first pointed out that the nonstationarity associated with sparking discharges naturally leads to a two-stream instability as the result of mutual penetration between the slower and the faster plasma components. Asseo & Melikidze (1998) developed this idea further, calculated the growth rates, and demonstrated that the instability is very efficient in generating Langmuir plasma waves at distances of many stellar radii r ins $ 10 4 À10 5 ð Þ h CR ¼ 10 7 À10 8 cm, where h CR is the height of the acceleration region described by equation (21) (Melikidze et al 2000). This is exactly where pulsar's radio emission is supposed to originate (e.g., Kijak & Gil 1998).…”
Section: Discussionmentioning
confidence: 99%
“…[1]). Then the spark plasma escapes from the region, as discussed by Asseo & Melikidze (1998). However, during a short escaping timescale h/c $ 10 À8 s the thermionic ions still maintain the partial screening as determined by equation (6).…”
Section: Charge-depleted Inner Acceleration Regionmentioning
confidence: 96%
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