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Non-trapping obstacle

PDF p. 2: footnote 1; PDF p. 3: Remark 1

Definition

Let n≥2, and let Θ⊂Rn be a nonempty compact obstacle with smooth boundary and connected exterior Ω=Rn∖Θ. A complete generalized ray is the spatial projection x:R→Ω‾, parametrized by physical time at unit speed, of a complete admissible generalized bicharacteristic in the exterior, including reflected and glancing boundary behavior.

The obstacle is non-trapping if every such complete ray leaves every compact subset of Rn in finite forward time: for each ray x(t) and each compact set K⊂Rn, there is a finite t≥0 with x(t)∉K. The time may depend on both the ray and K. This is the non-trapping part of the article's standing hypothesis (H).

Justification

The geometry and the meanings of compactness, smooth boundary and connected exterior are fixed by Exterior and truncated obstacle domains. The generalized-ray convention is fixed independently by Independent generalized reflected-ray and GCC convention: it includes complete compressed reflected and glancing curves and identifies their spatial projections. The quantified curves have time domain R; the escape test uses their forward restrictions. A curve defined only on a finite interval or on [0,∞) is not automatically a complete ray in this predicate: applying the predicate to that curve requires a complete extension. The condition above is therefore a definite predicate on the obstacle and those admissible rays. It asks for a finite escape time separately for each ray and compact set; this definition does not assert a common escape time, uniqueness at infinite-order contact, or a geometric control theorem.

Source notes

The article's footnote on page 2 describes reflected geometric-optics rays leaving compact sets in finite time, and Remark 1 uses generalized bicharacteristics. The article is cited for attribution; the ray convention used here is supplied by the independent prerequisite.

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Used by · 45

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