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The characteristic initial value problem in general relativity in a double null foliation

In a Paper by Rendall, it is shown that the characteristic initial value problem for the Einstein equations is well-posed. In fact, if the data are specified in some coordinates, then one can extend these coordinates to be harmonic in the future development. In work of Christodoulou on the formation of trapped surfaces, Christodoulou seems to use a version of this result to set up his initial data. However, the coordinates he gets for his solution are what he calls "canonical coordinates." In short, if he chooses coordinates $v,\theta$ on one null hypersurface and $u,\theta$ on the other, then it seems to me like $\frac{\partial}{\partial v}$ should be a null geodesic for the solution, and that the coordinate $\theta$ should be transported from coordinates on the intersection of the initial surfaces via $\frac{\partial}{\partial v}$.

My question is this: (1) is my interpretation accurate? and if so, (2) what's the idea of the proof? The theorem of Rendall is argued by using harmonic coordinates and reduction to the Cauchy problem (which has long been solved). If one tries a similar approach to the initial data of Christodoulou, one ends up trying to solve the null Bianchi equations, which are not of hyperbolic character and don't appear to have a general theory, so even obtaining a local existence theorem seems like very hard work.