The parabolic-boundary bound for a scalar on the meridional half-disc #
A scalar field g of class C¹ on the unit cylinder, read along the meridional
embedding, is bounded on the parabolic boundary axisParabolicBoundary R_* t_η s of
CIV.axisMaximumPrinciple by max (M_b, M_i): the lateral bound M_b on the
half-circle {r² + z² = R_*²} for t_η < t ≤ s, the initial bound M_i on the open
ball at t = t_η, and, at the corner where the two pieces meet, the initial bound again,
carried to the boundary sphere by continuity along the radial segment c ↦ c·(r, z).
This is the scalar form of the swirl-profile boundary bound of CIV/Closure/SwirlBound.lean,
stripped of the (−t)^η weight and of the component selection, so that the circulation
instantiation of lem:aniso:axis can consume it directly.
At a corner point of the parabolic boundary — radius exactly R_*, time exactly the
initial time τ — the initial bound M_i, which is hypothesised on the open ball only,
still holds, by continuity of g (·, τ) along the radial segment.
The parabolic-boundary bound: on axisParabolicBoundary R_* t_η s, the meridional
reading of g is bounded by max (M_b, M_i).