Functional form of the fractional-anomaly coefficients

Determine the functions \({\cal F}_j(\Phi^\dagger\Phi)\) governing the fractional anomalous determinant terms in the broken-phase chiral effective Lagrangian, including their dependence on the independent invariants of \(\Phi^\dagger\Phi\).

Background

The proposed broken-phase anomalous Lagrangian is an infinite sum involving coefficient functions Fj(Φ†Φ){\cal F}_j(\Phi^\dagger\Phi) multiplying fractional powers (det⁡Φ)j/Nc(\det\Phi)^{j/N_c}. The paper imposes symmetry and matching conditions on these functions but does not derive their explicit form.

The author emphasizes that the functions may depend on invariants beyond det⁡(Φ†Φ)\det(\Phi^\dagger\Phi), such as traces of powers of Φ†Φ\Phi^\dagger\Phi. Their determination is important for making quantitative predictions and for testing the proposed fractional-instanton description of the chiral transition.

References

It is not obvious what the functions ${\cal F}_j$ are.

— Fractional anomalous determinants and the chiral phase transition  (2610.00472 - Pisarski, 30 Sep 2026) in Section 3, “The large $N_c$ limit of Veneziano”; reiterated in Section 8, “Conclusions”