Korteweg-de Vries equation on T: Difference between revisions

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* Scaling is <span class="SpellE">s_c</span> = -3/2.
* Scaling is <span class="SpellE">s_c</span> = -3/2.
* C^0 LWP in <span class="SpellE">H^s</span> for s >= -1, assuming u is real [<span class="SpellE">KpTp</span>-p]
* C^0 LWP in <span class="SpellE">H^s</span> for s >= -1, assuming u is real [[KpTp-p]]
** C^0 LWP in <span class="SpellE">H^s</span> for s >= -5/8 follows (at least in principle) from work on the <span class="SpellE">mKdV</span> equation by [Takaoka and <span class="SpellE">Tsutsumi</span>?]
** C^0 LWP in <span class="SpellE">H^s</span> for s >= -5/8 follows (at least in principle) from work on the <span class="SpellE">mKdV</span> equation by [Takaoka and Tsutsumi?]
** Analytic LWP in <span class="SpellE">H^s</span> for s >= -1/2, in the complex case [[KnPoVe1996]]. In addition to the usual bilinear estimate, one needs a linear estimate to keep the solution in <span class="SpellE">H^s</span> for t>0.
** Analytic LWP in <span class="SpellE">H^s</span> for s >= -1/2, in the complex case [[KnPoVe1996]]. In addition to the usual bilinear estimate, one needs a linear estimate to keep the solution in <span class="SpellE">H^s</span> for t>0.
** Analytic LWP was proven for s >= 0 in [[Bo1993b]].
** Analytic LWP was proven for s >= 0 in [[Bo1993b]].
** Analytic ill <span class="SpellE">posedness</span> at s<-1/2, even in the real case [[Bo1997]]
** Analytic ill <span class="SpellE">posedness</span> at s<-1/2, even in the real case [[Bo1997]]
*** This has been refined to failure of uniform continuity at s<-1/2 [<span class="SpellE">CtCoTa</span>-p]
*** This has been refined to failure of uniform continuity at s<-1/2 [[CtCoTa-p]]
** Remark: s=-1/2 is the <span class="SpellE">symplectic</span> regularity, and so the machinery of infinite-dimensional <span class="SpellE">symplectic</span> geometry applies once one has a continuous flow, although there are some technicalities involving approximating <span class="SpellE">KdV</span> by a suitable <span class="SpellE">symplectic</span> finite-dimensional flow. In particular one has <span class="SpellE">symplectic</span> non-squeezing [[CoKeStTkTa-p9]], [[Bo1999]].
** Remark: s=-1/2 is the <span class="SpellE">symplectic</span> regularity, and so the machinery of infinite-dimensional <span class="SpellE">symplectic</span> geometry applies once one has a continuous flow, although there are some technicalities involving approximating <span class="SpellE">KdV</span> by a suitable <span class="SpellE">symplectic</span> finite-dimensional flow. In particular one has <span class="SpellE">symplectic</span> non-squeezing [[CoKeStTkTa-p9]], [[Bo1999]].
* C^0 GWP in <span class="SpellE">H^s</span> for s >= -1, in the real case [<span class="SpellE">KpTp</span>-p].
* C^0 GWP in <span class="SpellE">H^s</span> for s >= -1, in the real case [[KpTp-p]].
** Analytic GWP in <span class="SpellE">H^s</span> in the real case for s >= -1/2 [[CoKeStTkTa2003]]; see also [[CoKeStTkTa-p3]].
** Analytic GWP in <span class="SpellE">H^s</span> in the real case for s >= -1/2 [[CoKeStTkTa2003]]; see also [[CoKeStTkTa-p3]].
** A short proof for the s > -3/10 case is in [[CoKeStTkTa2001]]
** A short proof for the s > -3/10 case is in [[CoKeStTkTa2001]]
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*** ''Remark''<nowiki>: measures have the same scaling as H</nowiki><span class="GramE">^{</span>-1/2}, but neither space includes the other. (Measures are in H<span class="GramE">^{</span>-1/2-\eps} though).
*** ''Remark''<nowiki>: measures have the same scaling as H</nowiki><span class="GramE">^{</span>-1/2}, but neither space includes the other. (Measures are in H<span class="GramE">^{</span>-1/2-\eps} though).
** One has GWP for real random data whose Fourier coefficients decay like 1/|k| (times a Gaussian random variable) [[Bo1995c]]. Indeed one has an invariant measure.
** One has GWP for real random data whose Fourier coefficients decay like 1/|k| (times a Gaussian random variable) [[Bo1995c]]. Indeed one has an invariant measure.
** [[Solitons]] are asymptotically H^1 stable [[MtMe-p3]], [[MtMe-p]]. Indeed, the solution decouples into a finite sum of <span class="SpellE">solitons</span> plus dispersive radiation [[EckShr1988]]
** [[Solitons]] are asymptotically H^1 stable [[MtMe-p3]], [[MtMe-p]]. Indeed, the solution decouples into a finite sum of <span class="SpellE">solitons</span> plus dispersive radiation [[EckShr1983]].


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

Latest revision as of 22:51, 14 August 2006

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

  • Scaling is s_c = -3/2.
  • C^0 LWP in H^s for s >= -1, assuming u is real KpTp-p
    • C^0 LWP in H^s for s >= -5/8 follows (at least in principle) from work on the mKdV equation by [Takaoka and Tsutsumi?]
    • Analytic LWP in H^s for s >= -1/2, in the complex case KnPoVe1996. In addition to the usual bilinear estimate, one needs a linear estimate to keep the solution in H^s for t>0.
    • Analytic LWP was proven for s >= 0 in Bo1993b.
    • Analytic ill posedness at s<-1/2, even in the real case Bo1997
      • This has been refined to failure of uniform continuity at s<-1/2 CtCoTa-p
    • Remark: s=-1/2 is the symplectic regularity, and so the machinery of infinite-dimensional symplectic geometry applies once one has a continuous flow, although there are some technicalities involving approximating KdV by a suitable symplectic finite-dimensional flow. In particular one has symplectic non-squeezing CoKeStTkTa-p9, Bo1999.
  • C^0 GWP in H^s for s >= -1, in the real case KpTp-p.
    • Analytic GWP in H^s in the real case for s >= -1/2 CoKeStTkTa2003; see also CoKeStTkTa-p3.
    • A short proof for the s > -3/10 case is in CoKeStTkTa2001
    • Was proven for s >= 0 in Bo1993b.
    • GWP for real initial data which are measures of small norm Bo1997 The small norm restriction is presumably technical.
      • Remark: measures have the same scaling as H^{-1/2}, but neither space includes the other. (Measures are in H^{-1/2-\eps} though).
    • One has GWP for real random data whose Fourier coefficients decay like 1/|k| (times a Gaussian random variable) Bo1995c. Indeed one has an invariant measure.
    • Solitons are asymptotically H^1 stable MtMe-p3, MtMe-p. Indeed, the solution decouples into a finite sum of solitons plus dispersive radiation EckShr1983.