The characteristics solve and , starting with on the initial hypersurface and . The non-characteristic hypersurface condition at a point is , where is any nonzero normal there. It makes the map from initial-surface coordinates and characteristic time to locally invertible. Local uniqueness for the ordinary differential equations and the inverse function theorem then give a unique local solution near that point, for the stated coefficients and data.
Along the characteristics, is constant. Since , the amplitude equation gives . Matching the initial value at yields
Differentiation directly verifies both the partial differential equation and the initial data.
The solution is constant on characteristics . On the initial curve this invariant is for and for . This is a bijection of , with everywhere positive derivative. Its inverse is
Therefore The inverse is even at zero, so for data this is a global solution. Every characteristic meets the initial curve exactly once.
The new characteristics have invariant . On the initial curve it is for and for . The latter branch folds at , attaining its maximum . Some characteristics meet the initial curve twice or more; generic values of at those intersections disagree, so no global solution constant along characteristics can exist.
At every initial point except , the curve is non-characteristic, and the local existence and uniqueness theorem applies. At , tangency requires , but this is not sufficient. The fold tangency obstruction for characteristic data requires locally with continuously differentiable: equal invariant values must have equal data, and must have a finite continuous limit. For example satisfies and agrees across the fold, but would force an infinite derivative of at .
If the full compatibility condition holds, can be extended to invariant values above to give a local solution. Those values are not specified by the initial curve, so local uniqueness then fails.

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