Manuscript Em03-A@1 · Em03-A-v1.tex · lemma · 6d54627d

Lemma: Positive-frequency scattering

Geometry and exact exterior scattering › Constructive transmission probabilities · lines 516–644 · proof included or linked

Em03-A@1#lem:scattering, Em03-A@1#eq:ODE, Em03-A@1#eq:Volterra

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For every fixed and , the radial equation

has uniquely normalized Jost solutions and with

including the corresponding derivative asymptotics.

They construct a unitary scattering matrix . The horizon-to-infinity coefficient is

where

In particular,

All these coefficients are continuous on compact subsets of .

Proof. The outgoing right Jost solution is constructed by the Volterra equation

Successive iteration converges absolutely. Indeed, the -th iterated correction is bounded by

and consequently

The same Volterra estimate applied to a difference proves uniqueness. Differentiation of (eq:Volterra) gives (eq:ODE) and the derivative asymptotics at .

Expanding the sine in (eq:Volterra) gives, at the other end,

The omitted tails tend to zero because . Differentiating the same expressions gives the left derivative asymptotics.

For every solution of (eq:ODE), the current

is constant. For , its right-end value is , whereas its left-end value is

Thus , and the horizon-incident solution has asymptotics

This proves the transmission formula and its bounds.

The left Jost solution is obtained from the analogous Volterra equation integrated from . Its right incoming coefficient is likewise nonzero by current conservation, so it constructs the solution incident from infinity.

For arbitrary incoming amplitudes , the corresponding combination of and has outgoing amplitudes

Current conservation gives

for every pair of incoming amplitudes. Therefore , and the square matrix is unitary.

On a compact positive-frequency interval, the Volterra series have uniform majorants. Their terms and the coefficient integrals depend continuously on . Dominated convergence proves the last assertion.

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