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note
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u = π, and heteroclinic orbits linking Δθ= (2m - 1 ) π and Δθ= (2m + 1) π, m = . . . , - 2, - 1,0,1,2, . . . , appear at the bifurcation point K = 3|ω|/2. This picture can be extended to the case of Eq. (1), though the latter case is more complicated and it is impossible to compute the explicit form of the heteroclinic orbits.
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