1994
DOI: 10.1051/978-2-7598-0286-9
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Physique des plasmas (Vol. II)

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Cited by 43 publications
(27 citation statements)
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“…Note that the dimensional constant in front of ( 10) is (r 0 v 2 th ) 2 . The Rutherford cross-section (10) presents two singularities of very different nature: -first, the kinetic collision kernel, |v − v * | −3 , is singular as v − v * → 0. It is classical that kinetic singularities are well tractable from the mathematical point of view if they are locally integrable, see for instance the wellknown paper of DiPerna and Lions [14].…”
Section: Preliminary Discussionmentioning
confidence: 99%
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“…Note that the dimensional constant in front of ( 10) is (r 0 v 2 th ) 2 . The Rutherford cross-section (10) presents two singularities of very different nature: -first, the kinetic collision kernel, |v − v * | −3 , is singular as v − v * → 0. It is classical that kinetic singularities are well tractable from the mathematical point of view if they are locally integrable, see for instance the wellknown paper of DiPerna and Lions [14].…”
Section: Preliminary Discussionmentioning
confidence: 99%
“…Justifications for this screening assumption can be found in many physical textbooks on plasma physics, as [5,10]; from the mathematical point of view we are still far from understanding it. The screening will result in a less important role of collisions with a high impact parameter, therefore a less important role of grazing collisions.…”
Section: Preliminary Discussionmentioning
confidence: 99%
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