KP-II equation: Difference between revisions
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* GWP for s1 > -1/14, s2 = 0 [[IsMj2003]]. | * GWP for s1 > -1/14, s2 = 0 [[IsMj2003]]. | ||
** For s1 > -1/64 this is also in [[IsMj2001]]. | ** For s1 > -1/64 this is also in [[IsMj2001]]. | ||
* GWP for s1 > -1/78, s2 = 0 [[ | * GWP for s1 > -1/78, s2 = 0 [[Tk2000]] assuming a moment condition. | ||
** A similar result, with a slightly stricter constraint on s1 but no moment condition, was obtained in [[Tz-p]]. | ** A similar result, with a slightly stricter constraint on s1 but no moment condition, was obtained in [[Tz-p]]. | ||
** For s1 = s2 ³ 0 this was proven in [[Bo1993c]], and this argument also applies to the periodic setting. Heuristically this result is indicated by the local smoothing estimates in [[Sau1993]]. | ** For s1 = s2 ³ 0 this was proven in [[Bo1993c]], and this argument also applies to the periodic setting. Heuristically this result is indicated by the local smoothing estimates in [[Sau1993]]. |
Revision as of 05:05, 15 March 2007
The KP-II equation is the special case of the Kadomtsev-Petviashvili equation when the parameter is positive.
- Scaling is s1 + 2s2 + 1/2 = 0.
- GWP for s1 > -1/14, s2 = 0 IsMj2003.
- For s1 > -1/64 this is also in IsMj2001.
- GWP for s1 > -1/78, s2 = 0 Tk2000 assuming a moment condition.
LWP for s1 > -1/3, s2 = 0 TkTz-p4, IsMj2001
- Weak solutions in a weighted L2 space were constructed in Fa1990.
- For s1 < -1/3 the natural bilinear estimate fails TkTz-p4.
- Remark: Unlike KP-I, KP-II does not admit soliton solutions.
The KP-II equation can be generalized to three dimensions (replace partial_yy with partial_yy + partial_zz), with s_1 regularity in the x direction and s_2 in the y,z directions. Scaling is now s_1 + 2s_2 – ½ = 0. In isotropic spaces, local well-posedness in H^s with s > 3/2 was established assuming the low frequency condition that partial_x^{-1} u is also in H^s Tz1999. Anisotropically, local well-posedness in the space s_1 > 1, s_2 > 0 was established in IsLopMj-p.