Modified Korteweg-de Vries on T: Difference between revisions

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** One has GWP for random data whose Fourier coefficients decay like 1/|k| (times a Gaussian random variable) [[references.html#Bo1995c Bo1995c]]. Indeed one has an invariant measure. Note that such data barely fails to be in H<span class="GramE">^{</span>1/2}, however one can modify the local well-<span class="SpellE">posedness</span> theory to go below H^{1/2} provided that one has a decay like O(|k|^{-1+\eps}) on the Fourier coefficients (which is indeed the case almost surely).
** One has GWP for random data whose Fourier coefficients decay like 1/|k| (times a Gaussian random variable) [[references.html#Bo1995c Bo1995c]]. Indeed one has an invariant measure. Note that such data barely fails to be in H<span class="GramE">^{</span>1/2}, however one can modify the local well-<span class="SpellE">posedness</span> theory to go below H^{1/2} provided that one has a decay like O(|k|^{-1+\eps}) on the Fourier coefficients (which is indeed the case almost surely).


[[Category:Integrability]]
[[Category:Airy]]
[[Category:Equations]]
[[Category:Equations]]

Revision as of 07:41, 31 July 2006

The local and global well-posedness theory for the modified Korteweg-de Vries equation on the torus is as follows.

  • Scaling is s_c = -1/2.
  • C^0 LWP in L^2 in the defocusing case [KpTp-p2]
  • C^0 GWP in L^2 in the defocusing case [KpTp-p2]
    • Analytic GWP in H^s for s >= 1/2 [[references.html#CoKeStTaTk-p2 CoKeStTkTa-p2]], via the KdV theory and the Miura transform, for both the focussing and defocussing cases.
    • Was proven for s >= 1 in references.html#KnPoVe1993 KnPoVe1993, references.html#Bo1993b Bo1993b.
    • One has GWP for random data whose Fourier coefficients decay like 1/|k| (times a Gaussian random variable) references.html#Bo1995c Bo1995c. Indeed one has an invariant measure. Note that such data barely fails to be in H^{1/2}, however one can modify the local well-posedness theory to go below H^{1/2} provided that one has a decay like O(|k|^{-1+\eps}) on the Fourier coefficients (which is indeed the case almost surely).