“…In other words, we change our viewpoint, from thinking of the CH equation (63) as a differential equation for u(x, t), to considering (63) as an integro-differential equation for m. This approach has proved to be crucial for the analytic study of the CH equation: it has been used to determine whether solutions to CH are global in time or represent breaking waves [13,15,36], and it appears prominently in Lenells' construction of conservation laws [33], in the study of (multi)peakon dynamics and weak solutions [5,10,14], in the scattering/inverse scattering approach to CH [4,5,17], and also in a rigorous proof that the "least action principie" holds for CH [16].…”