The growth bound is . A characteristic curve through solves
The field is locally Lipschitz in space, giving local existence and uniqueness. On either direction of a bounded time interval the Gronwall inequality gives . Thus no trajectory can escape to infinity at finite time. On the resulting compact space-time region, local ordinary differential equation existence continues it, proving global definition for all .
Uniqueness gives the flow composition law and inverse . Differentiation with respect to solves the variational equation, making each map a diffeomorphism. Its positive Jacobian determinant is
These facts constitute the global characteristic flow under linear growth. A uniform global bound on is not required; its bounds on each compact characteristic tube suffice.

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