LinearExitDatum #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
The linear datum of the exit-time problem #
The exit-time comparison of Section 5.2 writes the constant right-hand side 1
as the divergence of the linear vector field g(x) = x_1 e_1, so that the
exit-time equation becomes an instance of the localized Dirichlet problem
-∇·a∇w = ∇·g of Section 5.1, whose homogenization is the injection estimate.
Two facts are needed about that datum: its 1/2-Hölder seminorm on a cube of
side 3^n is at most 3^{n/2}, so that the injection estimate's right-hand
side is C ε 3^{n/2} · 3^{n/2} = C ε 3^n; and its weak form is the constant
forcing, ∫ a∇w·∇φ = ∫ φ, which is the equation -∇·a∇w = 1.
The sign #
IsDirichletSolutionAt renders -∇·a∇u = ∇·g as ∫ a∇u·∇φ = -∫ g·∇φ. With
g(x) = x_1 e_1 the right side is -∫ x_1 ∂_1φ = +∫ φ, one integration by
parts against a zero-trace test function; so the datum g carries the positive
constant forcing and the solution is the (nonnegative) exit-time profile, not its
negative.
Main definitions #
linearAxisDatum i— the fieldx ↦ x_i e_i.
Main results #
vecFieldDiv_linearAxisDatum—∇·g = 1.holderSeminormOn_linearAxisDatum_le—[g]_{C^{0,1/2}(y+□_n)} ≤ 3^{n/2}.isDirichletSolutionAt_linearAxisDatum_iff— the weak form of the datum is the constant forcing∫ a∇u·∇φ = ∫ φ.
References #
- ABK26, the exit-time comparison of Section 5.2.
1. The field and its divergence #
The linear datum g(x) = x_i e_i, whose divergence is the constant
1.
Equations
Instances For
Each component of the linear datum is C¹.
∇·g = 1 for the linear datum g(x) = x_i e_i.
2. The Hölder seminorm of the linear datum #
The 1/2-Hölder bound for the linear datum on a cube of side 3^n.
The dimensional constant is 1: the increment of g is one coordinate
increment, which the supremum norm dominates.
The ℝ≥0∞ form of the Hölder bound for the linear datum.
3. The weak form: the constant forcing #
The linear datum tests as the constant 1.
The divergence-form equation at the linear datum is the constant forcing
-∇·a∇u = 1.
The localized Dirichlet problem at the linear datum: zero boundary values and the constant forcing.