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We then continue this orbit segment until (29) is satisfied.
Hence, the orbit segment (u(s)) is always defined over the interval (s in [0,1]).
Fig. 2 Demonstration of the moving orthonormal coordinate system along an orbit segment.
Since this orbit segment was selected from the falling slope of the downward peak of the spike-adding mechanism, the orbit segment jumps straight down toward S 1 a, where it converges to the resting potential.
Equations (5) and (7) uniquely define the orbit segment u ON as a function of λ for fixed T ON.
We then extend this orbit segment by the flow until the end point reaches the section (varSigma _{1} = { z=30 } ).
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Such orbit segments are canard orbits as we discuss next.
All surfaces are rendered from the respective thick orbit segments.
Such orbit segments are canard orbits in (mathbb{R}^{4}), as was discussed Sect. 4.
Therefore, the family of orbit segments must include a subfamily of orbit segments that experience a lift-off from S 2 r.
This is a clear indication that the computed orbit segments are accurate approximations of canard orbits.
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