Pointwise bounds for the tiny source contract #
Pure pointwise (in (t, x)) calculus for the last-iterate error e_{m-1}:
e = -B ∇VwhereV = T_{N*} - T_{N*-1}is the last increment andB = K_m - κ_{m-1} I + s_{m-1};- the Leibniz expansion of
∇(∇ · (B ∇V))into the words of length≤ 2applied toV, with the coefficient jets ofB(sc_gradDiv_abs_le); - the pointwise bound of the nondivergence part
∑_k ξ_{m,k} χTilde_{m,k} · (∇X ∘ X⁻¹) ∇(∇ · e)by|∇(∇ · e)|(sc_nd_sq_le).
Only products of coordinate bounds are used; the constants are crude since the source (7900–7925)
leaves an enormous amount of room (N_* large).
|∇ ∇·(A ∇v)| in terms of ordered Leibniz splits of the words [k, i].
Each term of the expanded flux of ∇ ∇·(A ∇v) is bounded by the coefficient jets times
the gradient of a word of length ≤ 2 applied to v.
Pointwise bound of ∇ ∇·(A ∇v) by the coefficient jets of A (orders ≤ 2) and the
gradients of the words of length ≤ 2 applied to v.
|∇ ∇·(A ∇v)|² is bounded by the sum of the squares of the word gradients.
Pointwise bound of the nondivergence part of tiny by |∇(∇·e)|.
The coefficient matrix of the last-iterate error.
Equations
Instances For
e_{m-1} = -B ∇V for the last increment V = T_{N*} - T_{N*-1}.
Pointwise L² bound of e_{m-1} by the gradient of the last increment.
∇(∇·e) is minus the gradient of the divergence of the flux B ∇V.
Pointwise bound of the nondivergence part of tiny by the word gradients of the last
increment, from the coefficient jets of B of orders ≤ 2.