1968
DOI: 10.1016/0031-8914(68)90016-5
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On the motion of charged particles in a slightly damped sinusoidal potential wave

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Cited by 44 publications
(19 citation statements)
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“…(Here K and E are the complete elliptic integrals of the first and second kind, respectively; cf., e.g., Ref. [19].) Since the generating function of the canonical transformation ðx; pÞ !…”
Section: (A)]mentioning
confidence: 99%
“…(Here K and E are the complete elliptic integrals of the first and second kind, respectively; cf., e.g., Ref. [19].) Since the generating function of the canonical transformation ðx; pÞ !…”
Section: (A)]mentioning
confidence: 99%
“…This action integral can be expressed in terms of complete elliptic integrals (see, e.g., Ref. [10] or p. 65 of Ref.…”
Section: The Amplitude Is Assumed To Have the Form A(q/l) ^Aofiq/l)mentioning
confidence: 99%
“…Since then, the adiabatic invariant has proved itself to be a very versatile tool especially in the study of the motion of a charged particle in an electromagnetic field (Best, 1968;Aamodt, 1971Aamodt, , 1972Tennyson 1979;Littlejohn, 1983;Caryet al, 1984;Menyuk, 1985) with applications to plasma physics and high energy accelerators.…”
Section: Introductionmentioning
confidence: 99%
“…It was soon realized (Best, 1968) that, except for the obvious discontinuity forced by the definition of the adiabatic invariant, thisinvariant does not change "much" for "most" of the trajectories crossing the critical curve. This "not much" was apparently estimated as c:(log C 1 )2 for the pendulum in an unpublished work of Gardner quoted by Aamodt (1971Aamodt ( -1972.…”
Section: Introductionmentioning
confidence: 99%