Generality of the separable stationary and axisymmetric scalar profile
Determine whether a separable stationary and axisymmetric scalar field profile Φ(r,θ) of the form Φ(r,θ)=Φr(r)+Φθ(θ) is the most general real, massless scalar solution compatible with the stationary and axisymmetric Einstein–Scalar metrics constructed by rescaling only the non-Killing (r,θ) sector of a rotating vacuum seed (such as Kerr, Kerr–Newman–NUT, or Myers–Perry), or identify more general non-separable scalar configurations if they exist.
References
We note however, that we have not managed to show that our separable form of the scalar is not the most general stationary and axisymetric scalar solution.
— Rotating spacetimes with a free scalar field in four and five dimensions
(2501.10223 - Barrientos et al., 17 Jan 2025) in Section 4 (Closing remarks), footnote