Cubic NLW/NLKG on R3
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- Scaling is .
- LWP for by Strichartz estimates (see e.g. LbSo1995; earlier references exist)
- When the time of existence depends on the profile of the data and not just on the norm.
- One can improve the critical space to a slightly weaker Besov space [Pl-p2].
- For one has instantaneous blowup in the focusing case, and unbounded growth of H^s norms in the defocusing case [CtCoTa-p2]
- GWP for KnPoVe-p2 for defocussing NLKG.(An alternate proof is in GalPl2003).
- For this is clear from energy conservation (for both NLKG and NLW).
- One also has GWP and scattering for data with small norm for general cubic non-linearities (and for either NLKG or NLW).
- In the defocussing case one has scattering for large data BaeSgZz1990, see also [Hi-p3].
- Improvement is certainly possible, both in lowering the s index and in replacing NLKG with NLW.
- In the focussing case there is blowup from large data by the ODE method.
- For periodic defocussing NLKG there is a weak turbulence effect in Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle H^s} for Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle s > 5} (low frequencies decay in time) but a symplectic non-squeezing effect in H^{1/2} Kuk1995b.In particular Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle H^s} cannot be a symplectic phase space for Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\displaystyle s > 5} .