The drift hypotheses of the finite-axis limit equation #
The lifted drift B_n = (V_n X/R, W_n) of eq:drift:Bn:def and its divergence
div_{X,Z} B_n = 2 V_n / R (continued to the axis by 2 ∂_R V_n), at the moving axis points
(0, z_n) of eq:aniso:zoom:finite:variables, have the three properties from which the admissible
limiting drift of eq:aniso:zoom:finite:limit is extracted:
- continuity on every compact subset of
ℝ⁵ × (-∞, -1], for all largen; - for every compact set of times in
(-∞, -1], one constant boundingB_n,div B_nand their spatial Lipschitz constants on every ball, for all largen(the footnote toeq:drift:Bn:def); - on every time slice,
div B_nis the weak divergence ofB_n(div_{X,Z} B_n = 2 V_n/Roff the axis, the axis being a null set crossed by a Lipschitz field).
A function Lipschitz in space, uniformly in time, and continuous in time at every point, is jointly continuous.
The lifted drift and divergence are continuous in time at a fixed lifted point, on a set of times at which the zoomed point stays in the cylinder.
For every radius and compact set of times in (-∞, -1], eventually the zoom maps the
rectangle [0, 2r] × [-r, r] into the cylinder at every such time.
The uniform bounds and Lipschitz bounds of the lifted drift and divergence on every ball.
The lifted drift and divergence are eventually continuous on every compact subset of
ℝ⁵ × (-∞, -1].
On one time slice, div B_n = 2 V_n / R is the weak divergence of the lifted drift. The drift
is Lipschitz across the axis (norm_zoomDrift_sub_le), so Rademacher's integration by parts
applies to (a Lipschitz extension of) each component, and its classical divergence off the null
axis is 2 V_n / R (zoomDriftDivergence_eq).
F2-H: the three hypotheses of the drift extraction for the lifted finite-axis drift at the
moving axis points: eventual continuity on compacts, uniform bounds and Lipschitz bounds on every
ball, and the slice weak divergence.