2005
DOI: 10.1016/j.nima.2005.07.054
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Longitudinal cooling force due to magnetized electrons

Abstract: We study effects of the tails of the longitudinal velocity distribution function of cooling electrons on dependencies of the longitudinal magnetized electron cooling force on ion velocities. For the case, when ions move parallel to the guiding magnetic field of the cooling device we calculate the longitudinal cooling force beyond the logarithmic approximation. r

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Cited by 2 publications
(3 citation statements)
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“…( 34)) are very convenient for numerical calculations since they involve one-dimensional integrals with finite range. Similar expressions have been obtained by Pestrikov [39] where, however, the drag force involves an integral with infinite range. But up to the definition of the Coulomb logarithm (i.e., U = Λ(κ) in our case and U = U C in Ref.…”
Section: B Some Limiting Cases Of Eqs (18) and (19)supporting
confidence: 79%
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“…( 34)) are very convenient for numerical calculations since they involve one-dimensional integrals with finite range. Similar expressions have been obtained by Pestrikov [39] where, however, the drag force involves an integral with infinite range. But up to the definition of the Coulomb logarithm (i.e., U = Λ(κ) in our case and U = U C in Ref.…”
Section: B Some Limiting Cases Of Eqs (18) and (19)supporting
confidence: 79%
“…But up to the definition of the Coulomb logarithm (i.e., U = Λ(κ) in our case and U = U C in Ref. [39]) both expressions are identical. This can be easily shown after changing the variable ζ in (41)…”
Section: B Some Limiting Cases Of Eqs (18) and (19)mentioning
confidence: 72%
“…Up to the definition of the Coulomb logarithm (i.e., U ¼ Λϰ ðÞ versus U ¼ U C ), the expressions are identical to those obtained by Pestrikov [59].…”
Section: Some Limiting Cases Of Eq (11)supporting
confidence: 55%