1964
DOI: 10.1103/physrev.133.b1352
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Generalization of the Runge-Lenz Vector in the Presence of an Electric Field

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Cited by 51 publications
(26 citation statements)
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“…The Runge-Lenz type scalar K z is proportional to the projection of the Runge-Lenz vector on the electric field, augmented with a correction term [19], 3. General polynomial solutions to (2.14) are obtained [20] for any integer n = 0, ±1, .…”
Section: Further Separable Perturbationsmentioning
confidence: 99%
“…The Runge-Lenz type scalar K z is proportional to the projection of the Runge-Lenz vector on the electric field, augmented with a correction term [19], 3. General polynomial solutions to (2.14) are obtained [20] for any integer n = 0, ±1, .…”
Section: Further Separable Perturbationsmentioning
confidence: 99%
“…Fortunately, for the reasons mentioned earlier, the dynamics of the orbit with the asymmetric wind are remarkably similar to the Kepler problem. Redmond (1964) found a generalization of the Runge–Lenz vector in the presence of an external force ( F = F 1 ). Specifically, the generalized Runge–Lenz vector is given by where M is the total mass of the binary, μ is the reduced mass of the binary, L is the orbital angular momentum, r is the relative position of the two stars and p is their relative momentum.…”
Section: Calculationsmentioning
confidence: 99%
“…The quantum pendulum [123] is described by the replacement rn + Z (I-moment of inertia), Z e 2 + Zg, (g-gravitational acceleration) and E = b = 0.…”
Section: )mentioning
confidence: 99%