Existence of critical-mass ground states

Determine whether the mass-constrained critical nonlinear Schrödinger energy on the product of Euclidean space and a compact metric graph admits a ground state at the threshold mass \(\mu_{\mathrm{ex}^*}(\mathbb R^N\times G,2_*)\), including graphs with a terminal edge or a cycle covering.

Background

For the L2L^2-critical exponent p=2∗=2+4/(N+1)p=2_* = 2+4/(N+1), the paper establishes graph-dependent thresholds separating finite and unbounded-below energy regimes. The threshold μex∗(RN×G,2∗)\mu_{\mathrm{ex}^*}(\mathbb R^N\times G,2_*) lies between the critical masses associated with R+N+1\mathbb R^{N+1}_+ and RN+1\mathbb R^{N+1}, and it coincides with the Euclidean critical mass when the graph admits a cycle covering and with the half-space critical mass when the graph contains a terminal edge.

The results prove existence below the threshold and nonexistence or unboundedness above appropriate comparison thresholds, but do not settle attainment exactly at μ=μex∗(RN×G,2∗)\mu=\mu_{\mathrm{ex}^*}(\mathbb R^N\times G,2_*).

References

Nonetheless, also in these cases the existence of ground states in the limit case \mu=\mu_{ex}*\bigl(\mathbb RN\times G,2_*\bigr) remains open.

— The nonlinear Schrödinger equation on products of $\mathbb{R}^N$ and compact metric graphs  (2609.18698 - Soave et al., 16 Sep 2026) in Section 1, discussion following Theorem 1.1 (theorem labelled “caso sottocritico e critico”)