Resonant Brézis–Nirenberg case

Establish whether the critical ball-mass equation -Δu + Φu(|x|)|u|^{p-2}u = λ|u|^{β-2}u + |u|^{2*−2}u in ℝ^N has a nontrivial weak radial solution when λ equals a scaled eigenvalue λ_k.

Background

The Brézis–Nirenberg-type theorem establishes a nontrivial weak radial solution for positive parameters λ lying strictly between consecutive scaled eigenvalues, and also for 0 < λ < λ_1. It does not cover the resonant values λ = λ_k. The authors explain that the linking geometry and index computation persist at resonance, but they cannot ensure that the associated minimax level remains below the compactness threshold S{N/2}/N.

References

Whether equation bn-eq has a nontrivial weak radial solution when \lambda = \lambda_k is an open problem.

— A unifying zero-mass equation  (2609.26585 - Perera, 22 Sep 2026) in Remark 2.14 (Remark \ref{rmk:resonant}); Section 6, item 1

Whether Theorem \ref{thm:sps-bn} holds for $N = 3$, in particular in the physical case $p = 2$, is open.

— A unifying zero-mass equation  (2609.26585 - Perera, 22 Sep 2026) in Section 6, item 2; Remark \ref{rmk:sps-bn}

When $\beta = 2{p,q}_{b,\ast}$, as in the Chern-Simons-Schrödinger case, Theorem \ref{thm:bm-eigenvalues} does not apply. Is there a general theory of scaled eigenvalues in the borderline case $\beta = 2{p,q}_{b,\ast}$?

— A unifying zero-mass equation  (2609.26585 - Perera, 22 Sep 2026) in Section 6, item 6