Tangency principle in backwards light cones for the relativistic heat equation

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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,w′∈C12(UT)∩C(UT‾)w,w'\in C^2_1(U_T)\cap C(\overline{U_T}) satisfy

wt−Q~w≤wt′−Q~w′w_t-\widetilde{Q}w\leq w'_t-\widetilde{Q}w'

and w≤w′w\leq w' in U(x,t)U_{(x,t)}. If w(x,t)=w′(x,t)w(x,t)=w'(x,t), then w≡w′w\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.

References

Primary source

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

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