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Issue partly solved, see below.
1D Greens Functions converge badly when drawing a new center of mass (drawR) after a SINGLE_REACTION or a IV_REACTION with a large domain size L. Where L is large as in L^2/(D t) >> 1. Both these events can return very small dt's (for a small IV domain or large dissociation constant).
Because for D t << L^2, the particle "doesn't see" the absorbing boundary and we can use the free 1D greens function. So, just as with the 3D functions, we could use different greens functions for particles far away from the boundary(s).
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