A priori periodic H1H^1 bound

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Let (u,p,u0,f,T,L)(u,p,u_0,f,T,L) be a smooth periodic, normalised-pressure solution, with periodic H1H^1 data norm H1(u0,f,T,L){\mathcal H}^1(u_0,f,T,L) finite. A priori periodic H1H^1 bound. There exists a function F:R+×R+×R+→R+F:\mathbf{R}^+\times\mathbf{R}^+\times\mathbf{R}^+\to\mathbf{R}^+ such that, whenever 0<T<T0<∞0<T<T_0<\infty and H1(u0,f,T,L)≤A<∞{\mathcal H}^1(u_0,f,T,L)\leq A<\infty, one has

∥u∥Lt∞Hx1([0,T]×R3/LZ3)≤F(A,L,T0).\|u\|_{L^\infty_tH^1_x([0,T]\times\mathbf{R}^3/L\mathbf{Z}^3)}\leq F(A,L,T_0).

Such a bound would quantitatively control periodic solutions on bounded time intervals and is presented as a quantitative form of global regularity; the source gives no resolution.

References

Primary source

Terence Tao, “Localisation and compactness properties of the Navier-Stokes global regularity problem”, arXiv:1108.1165 (2012).

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