HomogenizedExitTime #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
The homogenized exit time on a cube #
The comparator problem of Section 5.1 at the linear datum g(x) = x_i e_i is the
homogenized exit-time problem
-σ_n Δ w = 1 in y + □_n , w = 0 on ∂(y + □_n) ,
and exitTimeScale is the pre-T_r expression 3^{2n}/σ_n from display
(5.7). The conversion using (1 ± C γ^{1/2}|log γ|) to the definition of
T_r is deferred. This module proves that w and this scale are comparable,
with a dimensional constant:
C^{-1} ‖w‖_{L^∞(y+□_n)} ≤ T(3^n) ≤ C inf_{x ∈ y+□_{n-1}} w(x) .
The upper bound is the gradient bound of the comparator, which the interior
Schauder estimate supplies at the datum g in the form ‖∇w‖_∞ ≤ C σ_n^{-1}3^n,
together with the zero boundary values: a zero-trace function with a bounded
gradient is bounded by the gradient bound times half the side length. The lower
bound includes the coordinate sum and is d · Ksup · 3^n / 2. The lower bound
is the comparison with a bump barrier of height T(3^n)/K supported
strictly inside the cube and constant on a ball containing the inner cube.
Both bounds are stated for an arbitrary solution of the comparator problem and an arbitrary representative of it continuous on the cube: the solution is unique away from a null set, and its continuous representative is then unique at every point of the cube, so the two sides do not depend on either choice.
Main definitions #
exitTimeScale M n— the pre-T_rscale3^{2n}/σ_n.
Main results #
homogenized_exit_time_bounds— the two-sided comparison above.
References #
- ABK26, the exit-time comparison of Section 5.2.
1. The time scale #
The pre-T_r exit-time scale, 3^{2n}/σ_n.
Equations
- Algsuperdiff.Section5.Support.exitTimeScale M n = (3 ^ n) ^ 2 / ↑(Algsuperdiff.Section3.Annealed.sigmaBar M n)
Instances For
2. An elementary bridge #
3. The two-sided comparison #
The homogenized exit time is comparable to the time scale 3^{2n}/σ_n.
The constant depends only on the dimension.