Growth #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
Linear growth of the stream matrix #
On a cube of scale ℓ the normalized field splits as
k = (k_ℓ - k_ℓ(0)) + Σ_{n > ℓ} (j_n - j_n(0)). The first summand is bounded by
twice the descending value sum on □_ℓ, the second by the diameter 3^{ℓ} of
the cube times the ascending gradient sum on □_ℓ. The quantitative condition
of the carrier bounds the first by C 3^{ℓ} and the second by C, so the size
of the field on □_ℓ is at most a dimensional multiple of C 3^{ℓ}.
Choosing the smallest cube containing the ball of radius R turns this into the
linear bound ‖k‖_{L^∞(B_R)} ≤ C_k (1 + R) for R ≥ 1, with the sample constant
C_k displayed explicitly. The true growth of the source field is R^{γ};
the linear statement is the one the process theory consumes.
Main definitions #
streamTailConst ω— the sample constant supplied by the carrier.streamFieldGrowthConst ω— the explicit linear-growth constant.
Main results #
matrixOperatorNorm_streamField_le_on_cube— the cube form.matrixOperatorNorm_streamField_le— the linear growth on balls.
References #
- ABK26, the stream matrix; the almost sure bound
‖k‖_{L^∞(U_m)} ≲ 3^{γ m}.
1. The matrix norm through the entries #
2. The sample constant #
The sample constant of the quantitative two-leg condition.
Equations
Instances For
3. The two legs on one cube #
4. The bound on a cube #
The size of the field on the origin cube of scale ℓ.
5. Linear growth on balls #
The explicit linear-growth constant of the normalized field: a dimensional factor times the sample constant of the carrier.
Equations
- Algsuperdiff.Section5.Field.streamFieldGrowthConst M omega = 6 * (↑d ^ 2 * (↑(Algsuperdiff.Section5.Field.streamTailConst M omega) * (2 + ↑d / 2)))
Instances For
Linear growth: ‖k‖_{L^∞(B_R)} ≤ C_k (1 + R) for every R ≥ 1, with the
sample constant C_k of streamFieldGrowthConst.
Linear growth on Euclidean balls, the form of the source's
‖k‖_{L^∞(B_R)} ≤ C_k (1 + R): the ambient supremum norm of Vec d is
dominated by the Euclidean norm, so the ball statement follows from the cube
statement with the same constant.