Lipschitz bounds for ∂_R V_n and for V_n / R up to the axis #
Inputs to the admissibility of the lifted drift of eq:drift:Bn:def in Step 2 of the proof of
prop:aniso:small. On a rectangle [Ra, Rb] × [Za, Zb] mapped into the unit cylinder at a time
τ ≤ -1, the radial derivative ∂_R V_n is Lipschitz with a constant independent of n
(eq:aniso:zoom:derivatives at order two; the mixed derivative is taken in either order by the
symmetry of the Cartesian mixed partials), and the quotient V_n / R, continued to the axis by
∂_R V_n (the axis value of div_{X,Z} B_n / 2), is Lipschitz on [0, Rb] × [Za, Zb], since
V_n vanishes on the axis.
∂_R V_n differentiated in the radial variable along the slice through p.
∂_R V_n differentiated in the vertical variable along the slice through p; the derivative
is ∂_R ∂_Z V_n by the symmetry of the Cartesian mixed partials.
The radial derivative ∂_R V_n is Lipschitz on a rectangle mapped into the cylinder at a time
τ ≤ -1: |∂_R V_n(y₁) - ∂_R V_n(y₂)| ≤ C (|R₁ - R₂| + |Z₁ - Z₂|).
The quotient V_n / R, continued to the axis by ∂_R V_n.
Equations
Instances For
The standing hypotheses of this section, for a rectangle [0, Rb] × [Za, Zb].
The quotient is Lipschitz along a radial slice through [0, Rb], with constant 2C.
The quotient is Lipschitz along a vertical slice, with constant C.
The quotient is Lipschitz on the rectangle [0, Rb] × [Za, Zb], with constant 2C for the sum
of the coordinate increments.