Documentation

LeanPool.Superdiffusion.Algsuperdiff.Section5.Support.LinearExitDatum

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 #

Main results #

References #

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 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.