Let hk be the orthonormal Hermite polynomials for the standard Gaussian weight, and let a(w)=∑j≥0ajwj be a real power series with radius of convergence greater than 1, a(0)=0, no zeros on the unit circle and only simple zeros in the unit disk. For all large n the polynomial ∑j=0najhn−j has exactly as many nonreal zeros as a has in the disk, but the known proof gives the onset by compactness. We make it explicit: if a has no zeros in {1−d≤∣w∣≤1}, with d below an explicit threshold, the count is exact as soon as n exceeds a polynomial in 1/d and in the inverses of ∣a(0)∣, min∣w∣=1∣a∣, min∣w∣=1−d∣a∣ and min[−1+d,1−d]max(∣a∣,∣a′∣); no separation of the nonreal zeros of a is needed. By an exact identity this applies to the random Weyl polynomials Gn with independent standard Gaussian coefficients under the backward heat flow Gn,t=exp(−2nt∂z2)Gn, whose real-rooting time converges in distribution to T∗=R∗−2, where R∗ is the smallest modulus of a nonreal zero of the Gaussian power series q(w)=∑jηjwj. We show that the convergence holds with the rate n−α on [1+ε,∞) for every α<503, an exponent that does not depend on ε; the dependence on ε is removed by a super-exponential tail for the number of zeros of q in a disk. Under a coupling of the degrees that shares the top coefficients, the real-rooting time Λn satisfies ∣Λn−T∗∣≤K/n for n≥n0, with K and n0 depending on q. We bound K and n0 by polynomials in condition parameters of q, with absolute degrees and, when T∗≥1+ε, coefficients polynomial in 1/ε. For the Gaussian power series this gives, on the event {T∗≥1+ε}, a power tail with exponent 1/900 for the largest scaled displacement D of the final collision of zeros, and without restriction the tail bound exp(−c(logx/loglogx)1/2); the inputs include closed forms of the two-point correlation functions of the zeros of q.
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Version history
v1Submitted by Bingo BagginsInitial depositCurrentOct 22, 2026