Diamantis–Rolen odd-part containment conjecture for derivative period polynomials

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Let kk be an even weight, let f∈Sk(SL2(Z))f\in S_k(\mathrm{SL}_2(\mathbb Z)) be a normalized Hecke eigenform, and let m≥0m\geq 0 be an integer. Define the derivative period polynomial Qf,mQ_{f,m} and its odd part Qf,m−Q^-_{f,m} by

Qf,m(z)=∑j=0k−2(k−2j)i1−jΛf(m)(j+1)zk−2−j,Q_{f,m}(z)=\sum_{j=0}^{k-2}\binom{k-2}{j}i^{1-j}\Lambda_f^{(m)}(j+1)z^{k-2-j}, Qf,m−(z)=Qf,m(z)−Qf,m(−z)2.Q^-_{f,m}(z)=\frac{Q_{f,m}(z)-Q_{f,m}(-z)}{2}.

Let T={z∈C:∣z∣=1}\mathbb T=\{z\in\mathbb C:|z|=1\} and let Z(P)\mathcal Z(P) denote the set of distinct zeros of a polynomial PP.

Diamantis–Rolen odd-part containment conjecture. There is a real number b=b(f,m,k)>0b=b(f,m,k)>0 such that

Z(Qf,m−)⊆T∪{0,±b,±b−1}.\mathcal Z(Q^-_{f,m})\subseteq\mathbb T\cup\{0,\pm b,\pm b^{-1}\}.

The exceptional real reciprocal orbit may be absent.

This predicts that, apart from the forced zero at the origin, every zero of the odd part of a derivative period polynomial lies on the unit circle except possibly for a real reciprocal orbit. The statement extends the known rigid zero geometry for the odd period polynomial when m=0m=0; its validity for all even weights, normalized Hecke eigenforms, and m≥0m\geq0 remains open.

References

Primary source

Seokho Jin, “Odd Parts of Derivative Period Polynomials and a Logarithmic Transition Scale”, arXiv:2607.12378 (2026).

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