Gath's conjecture for Cygan--Korányi ball discrepancy

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Let q≥3q\ge3, let Hq\mathbb H^q be the Heisenberg group, and let Bt=δtB1\mathcal B_t=\delta_t\mathcal B_1 be the Cygan--Korányi ball. Write the lattice-point error term as

Eq(t):=#(Z2q+1∩δtB1)−vol⁡(B1)t2q+2.\mathcal E_q(t):=\#\left(\mathbb Z^{2q+1}\cap\delta_t\mathcal B_1\right)-\operatorname{vol}(\mathcal B_1)t^{2q+2}.

Gath's conjecture. The optimal order of the error term is 2q−12q-1; that is, the infimum of the exponents κ\kappa for which ∣Eq(t)∣≲tκ|\mathcal E_q(t)|\lesssim t^\kappa holds equals 2q−12q-1. For q=1q=1 the corresponding order is known to be optimal, while for q≥3q\ge3 the source gives an upper bound of order t2q−23t^{2q-\frac23}, a lower bound of order t2q−1(log⁡t)14(log⁡log⁡t)18t^{2q-1}(\log t)^{\frac14}(\log\log t)^{\frac18}, and a sharp second-moment estimate of magnitude t2q−1t^{2q-1}. The conjecture therefore remains open in the stated range.

References

Primary source

Sheng-Chen Mao and Sibei Yang, “Lattice point counting in Cygan–Korányi balls on Heisenberg groups”, arXiv:2607.10971 (2026).

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