Bilinear Airy estimates: Difference between revisions
From DispersiveWiki
Jump to navigationJump to search
No edit summary |
No edit summary |
||
Line 3: | Line 3: | ||
Much of the bilinear estimate theory for [[Airy equation]] rests on the following ``three-wave resonance identity'': | Much of the bilinear estimate theory for [[Airy equation]] rests on the following ``three-wave resonance identity'': | ||
<center><math>\xi_1^3 + \xi_2^3 + \xi_3^3 = 3 \xi_1 \xi_2 \xi_3 | <center><math>\xi_1^3 + \xi_2^3 + \xi_3^3 = 3 \xi_1 \xi_2 \xi_3</math> whenever <math>\xi_1 + \xi_2 + \xi_3 = 0</math></center> | ||
== Estimates == | == Estimates == |
Revision as of 05:00, 28 July 2006
Algebraic identity
Much of the bilinear estimate theory for Airy equation rests on the following ``three-wave resonance identity:
Estimates
The following bilinear estimates are known:
- The -3/4+ estimate references.html#KnPoVe1996 KnPoVe1996 on R:
- The above estimate fails at the endpoint -3/4. references.html#NaTkTs-p NaTkTs2001
- As a corollary of this estimate we have the -3/8+ estimate references.html#CoStTk1999 CoStTk1999 on R: If u and v have no low frequencies ( |\xi| <~ 1 ) then
- The -1/2 estimate references.html#KnPoVe1996 KnPoVe1996 on T: if u,v have mean zero, then for all s >= -1/2
- The above estimate fails for s < -1/2. Also, one cannot replace 1/2, -1/2 by 1/2+, -1/2+. references.html#KnPoVe1996 KnPoVe1996
- This estimate also holds in the large period case if one is willing to lose a power of \lambda^{0+} in the constant. references.html#CoKeStTaTk-p2 CoKeStTkTa-p2
- Remark: In principle, a complete list of bilinear estimates could be obtained from [[references.html#Ta-p2 Ta-p2]].