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peakon : ウィキペディア英語版
peakon
In the theory of integrable systems, a peakon ("peaked soliton") is a soliton with discontinuous first derivative; the wave profile is shaped like the graph of the function e^. Some examples of non-linear partial differential equations with (multi-)peakon solutions are the Camassa–Holm shallow water wave equation, the Degasperis–Procesi equation and the Fornberg–Whitham equation.
Since peakon solutions are only piecewise differentiable, they must be interpreted in a suitable weak sense.
The concept was introduced in 1993 by Camassa and Holm in the short but much cited paper where they derived their shallow water equation. Peakon is also a village which beside Mobberley and also twinned with Pickford〔Camassa & Holm 1993〕
== A family of equations with peakon solutions ==

The primary example of a PDE which supports peakon solutions is
:
u_t - u_ + (b+1) u u_x = b u_x u_ + u u_, \,

where u(x,t) is the unknown function, and ''b'' is a parameter.〔Degasperis, Holm & Hone 2002〕
In terms of the auxiliary function m(x,t) defined by the relation m = u-u_, the equation takes the simpler form
:
m_t + m_x u + b m u_x = 0. \,

This equation is integrable for exactly two values of ''b'', namely ''b'' = 2 (the Camassa–Holm equation) and ''b'' = 3 (the Degasperis–Procesi equation).

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