Prove that the operators J_{2n} are conserved for all n
Prove that the operators J_{2n}=[J_{2n+1},a_0^†], with J_{2n+1} defined recursively by J_{2n+1}=[J_{2n−1},H] and J_1=a_0, commute with the Gérard–Grellier Hamiltonian H for all n, i.e., establish [H,J_{2n}]=0 as an analytic theorem.
References
We have not been able to prove analytically that (\ref{J2n}) are conserved, though we have run extensive checks that the corresponding matrices commute with the Hamiltonian within individual $(N,M)$-blocks.
— A superintegrable quantum field theory
(2511.03373 - Clerck et al., 5 Nov 2025) in Section “Quantum Lax pair and conservation laws” (around equations (oddJs) and (J2n))