Box and loop orbits in axisymmetric potentials remain distinct at finite angular momentum, separated by a critical third integral I3crit(E) whose location can be computed; a modified Staeckel Fudge handles the singular frequencies near the critical action Jzcrit.
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Actions of highly eccentric orbits
Box and loop orbits in axisymmetric potentials remain distinct at finite angular momentum, separated by a critical third integral I3crit(E) whose location can be computed; a modified Staeckel Fudge handles the singular frequencies near the critical action Jzcrit.