For a finite field Fq\mathbb{F}_q, the Ihara constant A(q)A(q) measures the asymptotically maximal ratio of rational points to genus on algebraic curves over Fq\mathbb{F}_q. It equals q−1\sqrt{q}-1 when qq is a square, but for nonsquare qq its exact value is unknown. The current best lower bounds for the two smallest nonsquare cases, A(2)≥0.316999…A(2)\geq 0.316999\ldots and A(3)≥0.492876…A(3)\geq 0.492876\ldots, were obtained by Duursma and Mak (2013) via a variant of Serre's class field tower method with explicit ray class field conductor control, and the authors explicitly flag the bottlenecks of their technique: exact conductor-degree data for the characters of the ray class field extension, the search for better base function fields, and the combinatorial optimization of conductor sets, conductor exponents, and splitting sets. The records remain the best known and the flagged bottlenecks remain open, so the problem of proving a strictly larger lower bound for A(2)A(2) or A(3)A(3) — or determining either constant exactly, anywhere up to the Drinfeld–Vlăduţ ceilings 2−1≈0.414214\sqrt{2}-1\approx 0.414214 and 3−1≈0.732051\sqrt{3}-1\approx 0.732051 — is open.

Background

Let Fq\mathbb{F}_q be the finite field with qq elements and let X/Fq\mathcal{X}/\mathbb{F}_q be a projective, nonsingular, geometrically irreducible curve of genus g(X)g(\mathcal{X}) (the genus is the dimension of the space of holomorphic differentials, a birational invariant measuring arithmetic complexity). Write N(X)N(\mathcal{X}) for the number of Fq\mathbb{F}_q-rational points of X\mathcal{X}. The Hasse–Weil bound N(X)≤q+1+2gqN(\mathcal{X})\leq q+1+2g\sqrt{q} is far from sharp when gg is large relative to qq, so one studies Nq(g)=max⁡N(X)N_q(g)=\max N(\mathcal{X}) over genus-gg curves and its asymptotic slope, the Ihara constant

A(q)=lim sup⁡g→∞Nq(g)g.A(q)=\limsup_{g\to\infty}\frac{N_q(g)}{g}.

This quantity governs, among other things, the asymptotic performance of algebraic-geometry (Goppa) error-correcting codes and of arithmetic secret-sharing schemes built from curves. A theorem of Drinfeld and Vlăduţ gives A(q)≤q−1A(q)\leq\sqrt{q}-1 for every qq, and work of Ihara and of Tsfasman–Vlăduţ–Zink on modular and Shimura curves shows A(q)=q−1A(q)=\sqrt{q}-1 whenever qq is a square. For nonsquare qq — starting with q=2q=2 and q=3q=3 — the exact value of A(q)A(q) is unknown, and the Drinfeld–Vlăduţ bound remains the best known upper bound.

The leading technique for lower bounds when qq is prime is Serre's class field tower method, transported to function fields via the curve–function field dictionary (rational points of the curve correspond to degree-one places of its function field). One starts from a base function field k/Fqk/\mathbb{F}_q of genus gg with tt rational places, forms a suitable class field tower above it, and proves the tower is infinite using the Golod–Shafarevich criterion — a group-theoretic inequality saying that a nontrivial finite pp-group GG must satisfy r(G)>d(G)2/4r(G)>d(G)^2/4, where d(G)d(G) is the minimal number of generators and r(G)r(G) the minimal number of defining relations; if the generator and relation ranks established for the Galois group of the tower contradict this inequality, the group cannot be finite and the tower is infinite. An infinite tower in which the tt rational places split completely yields, by the Hurwitz genus formula (which relates the genus of an extension to the degree and ramification divisor), a lower bound A(q)≥t/(g−1)A(q)\geq t/(g-1), refined by controlled ramification. Temkine and others generalized the ramification analysis; Kuhnt's thesis (as documented by Duursma and Mak) considered towers over a finite Galois pp-extension K/kK/k with wild ramification concentrated in a chosen finite set SS of places.

Duursma and Mak (Compositio Mathematica 149 (2013) 1108–1128) developed this into a practical criterion. Given a conductor m=∑p∈Sνpp\mathfrak{m}=\sum_{\mathfrak{p}\in S}\nu_{\mathfrak{p}}\mathfrak{p} (a formal sum of places with positive integer exponents directing allowed ramification) and a set TT of tt rational places required to split completely, they form the ray class field K=kTmK=k^\mathfrak{m}_T — the maximal abelian extension of conductor dividing m\mathfrak{m} in which all places of TT split — and prove (Theorem 1.1) that if the splitting set and conductor exponents satisfy an explicit numerical inequality of Golod–Shafarevich type, then the (T,p)(T,p)-class field tower over KK is infinite and

A(q) ≥ tg−1+12[K:k]∑χdeg⁡fχ,A(q)\ \geq\ \frac{t}{g-1+\tfrac{1}{2[K:k]}\sum_{\chi}\deg\mathfrak{f}_\chi},

where fχ\mathfrak{f}_\chi is the Artin conductor of the character χ\chi of Gal(K/k)\mathrm{Gal}(K/k) (a divisor measuring the ramification of χ\chi), and the sum runs over the characters of that group. Their records A(2)≥0.316999…A(2)\geq 0.316999\ldots and A(3)≥0.492876…A(3)\geq 0.492876\ldots use explicit Artin–Schreier models (equations of the form yp−y=fy^p-y=f for a rational function ff, which define the cyclic degree-pp covers in characteristic pp) of elementary abelian extensions of small-genus function fields over F2\mathbb{F}_2 and F3\mathbb{F}_3: a genus-2 hyperelliptic function field H=F2(x,y)H=\mathbb{F}_2(x,y), y2+(x3+x+1)y=x2+xy^2+(x^3+x+1)y=x^2+x, underlies the A(2)A(2) record, while the A(3)A(3) record is built over the elliptic curve y2=x3−x+1y^2=x^3-x+1 over F3\mathbb{F}_3. The authors state the acknowledged limitations of the method verbatim: 'In general it may be difficult to determine exactly the degrees of the conductors for the characters of the group Gal(K/k)\mathrm{Gal}(K/k)' — forcing either the crude bound deg⁡fχ≤deg⁡m\deg\mathfrak{f}_\chi\leq\deg\mathfrak{m} (their Corollary 1.2) or average-conductor factors (1−p−d)(1-p^{-d}) per degree-dd place, which the authors use as rigorous upper bounds on the average conductor — and the systematic search for better base fields and the optimization of SS, the exponents νp\nu_{\mathfrak{p}}, and TT are left open. Determining A(2)A(2) or A(3)A(3) exactly would additionally require a genuinely new upper-bound technique at or below the Drinfeld–Vlăduţ ceiling for nonsquare qq, none being currently known.

Problem Statement

Improve the best known lower bounds for the Ihara constants A(2)A(2) and A(3)A(3) — or determine either constant exactly. Concretely: give a rigorous proof that A(2)≥c2A(2)\geq c_2 for an explicit constant c2>0.316999…c_2>0.316999\ldots (the 2013 Duursma–Mak record), or that A(3)≥c3A(3)\geq c_3 for an explicit c3>0.492876…c_3>0.492876\ldots, or determine the exact value of A(2)A(2) or A(3)A(3) (either of which would require a matching upper bound at or below the Drinfeld–Vlăduţ ceilings 2−1≈0.414214\sqrt{2}-1\approx 0.414214 and 3−1≈0.732051\sqrt{3}-1\approx 0.732051). This is the derived small-field instance of the general open problem of determining A(q)A(q) for nonsquare qq, posed in the exact form the source paper leaves open. Any method is admissible.

References

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