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New hemisystems of the Hermitian surface

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Abstract

Constructing hemisystems of the Hermitian surface is a well known, apparently difficult, problem in Finite geometry. So far, a few infinite families and some sporadic examples have been constructed. One of the different approaches relies on the Fuhrmann-Torres maximal curve and provides a hemisystem in \(PG(3,p^2)\) for every prime p of the form \(p=1+4a^2\), a even. Here we show that this approach also works in \(PG(3,p^2)\) for every prime \(p=1+4a^2\), a odd. The resulting hemisystem gives rise to two weight linear codes and strongly regular graphs whose properties are also investigated.

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Acknowledgements

The research of Vincenzo Pallozzi Lavorante was partially supported by the Italian National Group for Algebraic and Geometric Structures and their Applications (GNSAGA - INdAM) and by the National Science Foundation under Grant No. 2127742.

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Correspondence to Vincenzo Pallozzi Lavorante.

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Appendix A

Appendix A

We provide a proof of Proposition 6.7. Since our proof relies on cyclotomic fields from algebraic number theory, we present it in the form of an appendix.

Let \({\mathbb {Q}}(\zeta _m)\) the cyclotomic field of mth roots of unity with \(\zeta _m=e^{2\pi i /m} \in {\mathbb {C}}\). In particular, the cyclotomic field \({\mathbb {Q}}(\zeta _{16})\) contains \(\sqrt{2}\) as an integer. Let \({\mathfrak {b}}\) a prime ideal of \({\mathbb {Q}}(\zeta _{16})\) such that \({\mathfrak {b}}\) contains p (i.e. \({\mathfrak {b}} \mid p\)). The extension \({\mathfrak {b}} \mid p\) is unramified and \({\mathbb {Z}}[\zeta _{16}]/{\mathfrak {b}} \cong {\mathbb {F}}_{p^4}\); see [12, Proposition 13.2.5] and [11, Section 4.5]. Note that \(h=\pm \sqrt{2} \pmod {{\mathfrak {b}}}\). We may assume \(h \equiv \sqrt{2} \pmod {{\mathfrak {b}}}\).

Proof of Proposition 6.7

We do the computation for \(q \equiv 13 \pmod {16}\), the proofs for the other cases being analogous.

$$\begin{aligned} \begin{aligned} (1+h)^\frac{q+1}{2}h^\frac{q-1}{2}&\equiv (1+\sqrt{2})^\frac{q+1}{2} (\sqrt{2})^\frac{q-1}{2} \pmod {{\mathfrak {b}}} \\&=(\sqrt{2}+2)^\frac{q+1}{2} \frac{1}{\sqrt{2}}\\&=(\zeta _8+\zeta _8^{-1}+2)^\frac{q+1}{2}\frac{1}{\sqrt{2}}\\&=(\zeta _{16}+\zeta _{16}^{-1})^{q+1}\frac{1}{\sqrt{2}}\\&\equiv (\zeta _{16}+\zeta _{16}^{-1})(\zeta _{16}^{13}+\zeta _{16}^{-13}) \frac{1}{\sqrt{2}} \pmod {{\mathfrak {b}}}\\&\equiv (\zeta _{16}+\zeta _{16}^{-1})(\zeta _{16}^{-3}+\zeta _{16}^{3}) \frac{1}{\sqrt{2}} \pmod {{\mathfrak {b}}}\\&=(\zeta _{16}^4+\zeta _{16}^{-2}+\zeta _{16}^2+\zeta _{16}^{-4})\frac{1}{\sqrt{2}}\\&=(\zeta _8+\zeta _8^{-1})\frac{1}{\sqrt{2}}=1 \square \end{aligned} \end{aligned}$$

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Pallozzi Lavorante, V., Smaldore, V. New hemisystems of the Hermitian surface. Des. Codes Cryptogr. 91, 293–307 (2023). https://doi.org/10.1007/s10623-022-01107-2

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