Tangency principle in backwards light cones for the relativistic heat equation

Let UTU_T be the spacetime domain, let U(x,t)U_{(x,t)} be the backwards light cone of (x,t)UT(x,t)\in U_T, and let Q~\widetilde{Q} be the spatial operator in the relativistic heat equation. Tangency principle. Suppose w,wC12(UT)C(UT)w,w'\in C^2_1(U_T)\cap C(\overline{U_T}) satisfy

wtQ~wwtQ~ww_t-\widetilde{Q}w\leq w'_t-\widetilde{Q}w'

and www\leq w' in U(x,t)U_{(x,t)}. If w(x,t)=w(x,t)w(x,t)=w'(x,t), then www\equiv w' in U(x,t)U_{(x,t)}. This proposed strengthening of comparison and uniqueness would assert rigidity when two ordered sub- and supersolutions touch at the tip of a relativistic backwards light cone; the paper presents it as an expected principle requiring further techniques, so it remains open.

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Primary source

Evan Miller and Ari Stern, “Maximum principles for the relativistic heat equation”, arXiv:1507.05030 (2015).

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