Uniqueness of weak DLSS solutions in dimensions four and higher

Establish uniqueness for weak solutions of the Derrida–Lebowitz–Speer–Spohn equation in dimensions d≥4, and thereby determine whether the contraction semigroup constructed in L² coincides with weak solutions generated by the approximation schemes of Jüngel–Pinnau, Gualdani–Jüngel–Toscani, and Jüngel–Matthes.

Background

The paper constructs a canonical contraction semigroup for the DLSS equation in the square-root variable on a bounded convex domain with Neumann boundary conditions, for arbitrary nonnegative L² initial data and in every space dimension. It identifies this semigroup with the established weak-solution theory only in dimensions d≤3, using Fischer’s uniqueness theorem in the relevant regularity class and, for the Neumann setting, an additional conditional boundary-adaptation issue.

For dimensions d≥4, no uniqueness theory for the relevant weak solutions is available. Consequently, it is unresolved whether the canonical semigroup solution agrees with weak solutions obtained through the earlier approximation schemes; resolving this would connect the paper’s operator-theoretic construction to those approximation-based weak formulations in higher dimensions.

References

For $d\ge4$ no uniqueness theory for weak solutions is available, and the question remains open; what our results do give in every dimension is that one distinguished, canonically determined solution exists, depends continuously on the datum, and is characterized by the equivalent formulations listed above.

Maximal monotonicity and contraction semigroup for the quantum drift-diffusion (Derrida-Lebowitz-Speer-Spohn) equation  (2608.16792 - Matthes et al., 17 Aug 2026) in Introduction, paragraph “What is new?”, limitation paragraph