Systematic derivation of the conjugation relation between saddle-point parameters

Derive, in a rigorous and self-contained manner, the conjugation relation \(\tilde u = -\bar u\) for the saddle-point parameters in the large-\(k\) analysis of sparse non-Hermitian random matrices, starting from the general operator identity \(\tilde g = \operatorname{sign}(\hat C)\,\bar g\) where \(\hat C\) is defined by the kernel \(C(X,X') = k\,[1-\hat p\big(i\tilde X^{\dagger}X - iX^{\dagger}\tilde X\big)]\). Establish the conditions under which this relation holds and justify its use in obtaining the circular law and spectral-edge shapes for the ensembles considered.

Background

In the supersymmetry-based field-theoretic treatment, the averaged resolvent of sparse non-Hermitian ensembles reduces to a saddle-point equation for functions gg and g~\tilde g that are assumed superrotationally invariant. In the large-kk limit, these functions are approximated by linear forms g(X)=kuXXg(X)=k\,u\,X^{\dagger}X and g~(X)=ku~XX\tilde g(X)=k\,\tilde u\,X^{\dagger}X, leading to algebraic self-consistency conditions.

To complete the solution and recover the circular law (and more general spectral-edge shapes in later sections), the analysis assumes the conjugation relation u~=uˉ\tilde u = -\bar u. The authors note that a systematic derivation of this relation from the operator identity g~=sign(C^)gˉ\tilde g = \operatorname{sign}(\hat C)\,\bar g is currently missing and is left for future work, as its justification would strengthen the theoretical foundation and general applicability of the method.

References

We leave systematic derivation of this formula to future work, and we shall see below that it does not only allow us to rederive the circular law, but also much more sophisticated shapes of spectral edges for more complicated random matrix ensembles in the next section.

Random matrix theory of sparse neuronal networks with heterogeneous timescales (2512.12767 - Chotibut et al., 14 Dec 2025) in Section 2.4 (Low sparsity limit and the circular law)