Camassa–Holm equation

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Dispersionless (or quasi-classical) limits of integrable partial differential equations (PDE) arise in various problems of mathematics and physics and are intensively studied in the recent literature (see, f.i., [1]-[5]).

Examples

Dispersionless KP equation

The dispersionless Kadomtsev–Petviashvili equation (dKPE) has the form

(ut+uux)x+uyy=0,(1)

It arises from the commutation

[L1,L2]=0.(2)

of the following pair of 1-parameter families of vector fields

L1=y+λxuxλ,(3a)
L2=t+(λ2+u)x+(λux+uy)λ,(3b)

where λ is a spectral parameter. The dKPE is the x-dispersionless limit of the celebrated Kadomtsev–Petviashvili equation.

Dispersionless Korteweg–de Vries equation

The dispersionless Korteweg–de Vries equation (dKdVE) reads as

ut=32uux.(4)

It is the dispersionless or quasiclassical limit of the Korteweg–de Vries equation.

Dispersionless Davey–Stewartson equation

Dispersionless Novikov–Veselov equation

The dispersionless Novikov-Veselov equation is most commonly written as the following equation on function v=v(x1,x2,t):

tv=z(vw)+z¯(vw¯),z¯w=3zv,

where the following standard notation of complex analysis is used: z=12(x1ix2), z¯=12(x1+ix2). The function w here is an auxiliary function defined via v up to a holomorphic summand. The function v is generally assumed to be a real-valued function.

Dispersionless Hirota equation

See also

References

  • Kodam Y., Gibbons J. "Integrability of the dispersionless KP hierarchy"
  • Zakharov V.E. "Dispersionless limit of integrable systems in 2+1 dimensions"
  • Takasaki K., Takebe T. Rev. Math. Phys., 7, 743 (1995)
  • Konopelchenko B.G. "Quasiclassical generalized Weierstrass representation and dispersionless DS equation", ArXiv: 0709.4148
  • Konopelchenko B.G., Moro A. "Integrable Equations in Nonlinear Geometrical Optics", Studies in Applied Mathematics, 113(4), pp. 325–352 (2004)
  • Dunajski M. "Interpolating integrable system". ArXiv: 0804.1234

External links