Lin34 Centred Correction #
Part of the Caffarelli–Kohn–Nirenberg partial regularity proof.
Centring the nonlinearity against the Hessian of a test function #
The paper's nonlinearity is introduced in singly centred form
U_ij = -u_i (u_j - c_j) and then rewritten in the doubly centred form
Û_ij = -(u_i - c_i)(u_j - c_j) of eq:Uhat. The difference between the two
tensors is U_ij - Û_ij = -c_i (u_j - c_j), and the point of the present file is
that this difference pairs to zero against the Hessian of every smooth compactly
supported test function. This is purely a calculus fact: the Hessian of a test
function is a divergence, so its pairing with a constant vector field vanishes,
and its pairing with the weakly divergence-free field u vanishes by hypothesis.
The file records the two elementary integration-by-parts facts (the integral of a spatial derivative, and of a mixed second derivative, of a compactly supported smooth function) and then assembles the cancellation for the centred pairing.
The integral over all of Vec3 of a spatial partial derivative of a smooth
compactly supported function vanishes. This is integration by parts against the
constant test function 1, whose derivative is zero.
The integral over all of Vec3 of a mixed second derivative of a smooth
compactly supported function vanishes: it is the spatial derivative of the smooth
compactly supported function ∂_j G, so the previous integration-by-parts fact
applies.
The correction U_ij - Û_ij = -c_i (u_j - c_j) relating the singly and doubly
centred nonlinearities of eq:Uhat of paper/ckn.tex pairs to zero against the
Hessian of every smooth compactly supported test function F supported in Ω.
Indeed the constant vector field b is divergence free, so the b_i b_j part of
the pairing vanishes termwise, while the b_i u_j part is the divergence-free
pairing ∫_Ω ∑_j u_j ∂_j ∂_i F supplied by hdiv; the two groups are related by
the symmetry ∂_i ∂_j F = ∂_j ∂_i F of the Hessian.