The pre-Schwarzian at an end of opening 2 * π #
Let f map the upper half-plane conformally onto a domain U, extend to a continuous injection
of the closed upper half-plane, and tend to infinity at infinity. Suppose that far out U
coincides with the exterior of the closed half-strip {0 ≤ re ζ, 0 ≤ im ζ ≤ π} in the coordinate
ζ = (z - c) / b: the two unbounded sides of U are parallel rays pointing in the same
direction, and U surrounds the half-strip between them, so its end at infinity has opening
2 * π. Then z * f''(z) / f'(z) → 1 as z tends to infinity in the upper half-plane
(TauCeti.tendsto_mul_logDeriv_deriv_upperHalfPlaneSet_of_halfStripExterior).
Unlike a sector or a half-strip, the exterior of a half-strip has no elementary straightening
coordinate. Instead f is compared with the explicit model map ζ ↦ ζ ^ 2 / 2 - log ζ + π * I,
which carries the far part of the closed upper half-plane injectively into that exterior, with
the far positive and negative real axes going to the two sides. The comparison map
f⁻¹ ∘ (c + b * model) fixes infinity, is real on the far real axis, and so is conformal across
infinity by Schwarz reflection; the model has ζ * model''(ζ) / model'(ζ) → 1, and
TauCeti.tendsto_mul_logDeriv_deriv_upperHalfPlaneSet_of_eqOn_comp_neg_inv transfers this limit
to f. For a Schwarz--Christoffel map the limit is the sum of the finite turning exponents.
References #
- L. Ahlfors, Complex Analysis, Ch. 6, Section 2.
- T. Driscoll and L. Trefethen, Schwarz--Christoffel Mapping, Ch. 2.
The model map #
The comparison with the model #
The pre-Schwarzian at an end of opening 2 * π. Let f map the upper half-plane
holomorphically onto U, extend to a continuous injection of the closed upper half-plane, and
tend to infinity at infinity, and let U coincide far from c with the exterior of the closed
half-strip {0 ≤ re ((z - c) / b), 0 ≤ im ((z - c) / b) ≤ π}. Then z * f''(z) / f'(z) → 1 as
z tends to infinity in the upper half-plane.
So the two parallel unbounded sides of U bound a vertex at infinity of opening 2 * π, and for
a Schwarz--Christoffel map the finite turning exponents then sum to 1.