References
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By rescalingt, x andu it is possible to multiply each term in eq. (1) by a different constant. The form (1) that we use here is chosen for convenience;c=0 corresponds to the usual KdV equation, while the term proportional toc accounts, forc<0, for (Landau) damping. Hereafter we assumec>-0.
Note thatHf∃’=(Hf)∃’; here, and in the following, primes appended to functions indicate differentiation.
For all the solutions considered in this paper this constant of motion vanishes.
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A prime appended to a sum indicates that the singular term must be omitted when summing.
Dots indicate time differentiation.
Clearly the case when allx j ∃’s are in the lower half-plane is trivially related, by complex conjugation, to that treated here; while the results of AMM (see below) indicate that, at least for finiten, no solutions of (8) and (9) exists (forc≠0) unless the polesx j are all located in the same half-plane.
Forc=0,i.e. in the usual KdV case, these solutions belong to the similarity classu(x, t)=(t∃-t 0)∃-2/3F[x/(t∃-t0)1/3].
Of appropriately scaled size; see AMM.
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Calogero, F., Olshanetsky, M.A. & Perelomov, A.M. Rational solutions of the KdV equation with damping. Lett. Nuovo Cimento 24, 97–100 (1979). https://doi.org/10.1007/BF02725599
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DOI: https://doi.org/10.1007/BF02725599