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Quadratic Chabauty Locus

Updated 28 August 2025
  • Quadratic Chabauty Locus is defined as the zero set of a p-adic Coleman function that cuts out S-integral points on hyperbolic curves through explicit quadratic relations.
  • It leverages Kim’s non-abelian Chabauty method by computing a bilinear form using p-adic logarithms and dilogarithms to reveal underlying arithmetic structures.
  • The approach integrates K-theoretic reductions and motivic cohomology, transforming non-abelian cohomological data into explicitly computable analytic equations.

The Quadratic Chabauty locus is a central object in modern non-abelian Diophantine geometry, describing the set of pp-adic points on an algebraic curve cut out by explicit quadratic relations in the context of Kim’s non-abelian Chabauty–Kim method. For the thrice-punctured projective line X=P1{0,1,}X = \mathbb{P}^1 \setminus \{0,1,\infty\}, the locus is realized as the vanishing set of a bilinear (quadratic) Coleman function arising from the depth-2 unipotent pp-adic Hodge morphism, with coefficients determined by pp-adic logarithms and dilogarithms. This construction generalizes to higher-dimensional and modular settings, providing a powerful framework for controlling SS-integral or rational points on hyperbolic curves.

1. Non-Abelian Chabauty–Kim Theory and the Role of the Depth-2 Morphism

Kim’s non-abelian Chabauty program replaces the classical abelian Chabauty–Coleman approach with Galois-theoretically defined towers of Selmer varieties attached to increasingly deep unipotent quotients π1(n)\pi_1^{(n)} of the étale fundamental group. For X=P1{0,1,}X = \mathbb{P}^1 \setminus \{0,1,\infty\} and finite SS, the integer nn defines the depth. The depth-2 global pp-adic Hodge morphism

h2:Sel2(GT,π1(2))Alb2h_2: \text{Sel}_2(G_T, \pi_1^{(2)}) \to \mathrm{Alb}_2

has three coordinates, with the first two arising linearly from the abelianization (i.e., classical Chabauty level) and the third—h1,3h_{1,3}—encoding novel quadratic information. This third coordinate is a bilinear map

(Q)h1,3:(QS)×(QS)Qp,{}_{(Q)} h_{1,3}: (Q^S) \times (Q^S) \to Q_p,

where QSQ^S is a QQ-vector space with one basis element per qSq\in S (the "2|S|" variables stem from two abelian factors in the cohomological description). This quadratic form is at the heart of the explicit quadratic Chabauty locus.

2. Bilinear (Quadratic) Polynomial: Coefficient Structure and Computational Formula

The explicit description of h1,3h_{1,3} is given by a bilinear polynomial: (Q)h1,3(x,y)=1i,jsh1,3(qi,qj)xiyj,{}_{(Q)} h_{1,3}(x, y) = \sum_{1\leq i, j\leq s} h_{1,3}^{(q_i, q_j)} \, x_i y_j, where each h1,3(q,q)h_{1,3}^{(q, q')} is computed via decompositions in Milnor KK-theory, informed by the vanishing of K2(Q)QK_2(\mathbb{Q}) \otimes \mathbb{Q}. Explicitly,

(Q)h1,3(q,q)=ksk(log(q)(uk)log(q)(vk))ldlLi(tl),{}_{(Q)} h_{1,3}^{(q, q')} = \sum_k s_k \big( \log(q)(u_k) \log(q)(v_k) \big) - \sum_l d_l \mathrm{Li}(t_l),

where sks_k, dld_l are rational numbers obtained from reduction algorithms, and uk,vk,tlu_k,v_k,t_l are selected to control size with respect to q,qq,q'. log\log is the pp-adic logarithm, and Li\mathrm{Li} denotes the pp-adic dilogarithm. Under the de Rham realization, ρ2A(xy)\rho_2^A(x \otimes y) encodes both the symmetric product of logarithms and this bilinear form.

3. Quadratic Chabauty Locus as a Zero Set: Cutting out Integral Points

The image of the global Selmer variety under h2h_2 is typically lower-dimensional than the full de Rham fundamental group. This enables the definition of a nonzero Coleman function—explicitly, the pullback via the unipotent Albanese map of the coordinate function provided by h1,3h_{1,3}—whose vanishing locus in the pp-adic analytic space of XX is the quadratic Chabauty locus: $\{\text{%%%%31%%%%-adic points on %%%%32%%%% where the Coleman function vanishes}\}.$ Integral points map, under the unipotent Kummer map, to (t,1t)(t, 1-t), so the locus is defined by

(Q)h1,3(t,1t)=Li(t),{}_{(Q)} h_{1,3}(t, 1-t) = -\mathrm{Li}(t),

and the vanishing condition becomes

2Li(t)log(t)log(1t)=0,2\mathrm{Li}(t) - \log(t)\log(1-t) = 0,

which is a quadratic relation in the abelianized coordinates. Thus, the integral points lie precisely in the zero set of an explicit quadratic polynomial in $2|S|$ variables.

4. Cohomological and K-theoretic Underpinnings

The construction of the coefficients of the quadratic form leverages Milnor KK-theory and Tate's theorem (K2(Q)Q=0K_2(\mathbb{Q}) \otimes \mathbb{Q} = 0). Every tensor qqq \otimes q' is reduced to sums of tensors of units and tl(1tl)t_l \otimes (1-t_l). These reductions feed into the computation of the pp-adic logarithms and dilogarithms entering the explicit formula.

The bilinear form exhibits a "twisted antisymmetry" property: (Q)h1,3(u,v)+(Q)h1,3(v,u)=(logu)(logv).{}_{(Q)} h_{1,3}(u, v) + {}_{(Q)} h_{1,3}(v, u) = (\log u) (\log v). This reflects the decomposition of the quadratic piece into an antisymmetric dilogarithmic term and a symmetric logarithmic self-product, further tying the polynomial to KK-theoretic structures.

5. Function-theoretic and Motivic Interpretation

In the motivic Chabauty–Kim framework, the Selmer variety parametrizes non-abelian cohomology classes associated to mixed Tate motives over Z[S1]\mathbb{Z}[S^{-1}]. The unipotent pp-adic Hodge morphism maps these classes into the de Rham fundamental group, with the vanishing of the regular function (Coleman function) exactly characterizing the image. The depth-2 novelty is precisely the quadratic coordinate h1,3h_{1,3}, which introduces new motivic and functional constraints beyond those seen in abelian Chabauty.

6. Explicit Geometric and Computational Realizations

In practice, as demonstrated in the case of X=P1{0,1,}X = \mathbb{P}^1 \setminus \{0,1,\infty\}, the quadratic Chabauty locus is realized as the zero set of a single explicit quadratic polynomial involving pp-adic logarithms and dilogarithms, computable through the reduction algorithm described in the main theorem. The function is purely pp-adic analytic and serves directly as a cutting tool for SS-integral points. In explicit computational examples—including rings of the form Z[1/2]\mathbb{Z}[1/2] or the ring of integers of real quadratic fields—a single Coleman function suffices to cut out all integral points.

7. Conceptual and Diophantine Implications

The explicit quadratic nature of the Chabauty locus provides a functional machinery for detecting non-density of the image of the global Selmer variety in the de Rham fundamental group, and hence for establishing finiteness statements for SS-integral or rational points (akin to Siegel's theorem). In the broader Chabauty–Kim program, this clarifies how non-abelian cohomological invariants descend to explicit analytic equations, fulfilling conjectural expectations that such analytic loci coincide with sets of integral points. The approach also demonstrates that in certain settings, the quadratic locus gives a complete, uniform description across several base rings.

Table: Key Structural Ingredients of the Quadratic Chabauty Locus

Object/Concept Description Formula/Role
h1,3h_{1,3} Quadratic coordinate in pp-adic Hodge morphism h1,3(x,y)=i,jci,jxiyjh_{1,3}(x, y) = \sum_{i,j} c_{i,j}x_iy_j
Coefficients ci,jc_{i,j} In terms of log/dilog via K-theory reduction ci,j=sklog(uk)log(vk)dlLi(tl)c_{i,j} = \sum s_k \log(u_k)\log(v_k) - \sum d_l \mathrm{Li}(t_l)
Quadratic Chabauty locus Zero set of Coleman function in pp-adic coordinates 2Li(t)log(t)log(1t)=02\mathrm{Li}(t) - \log(t)\log(1-t) = 0

Summary

The quadratic Chabauty locus in Kim’s explicit Chabauty–Kim theory for the thrice-punctured line is characterized as the explicit vanishing locus of a pp-adic analytic bilinear polynomial—the third coordinate of the unipotent pp-adic Hodge morphism at depth two. Its coefficients are given algorithmically by pp-adic logarithms and dilogarithms arising from KK-theoretic reductions. The locus “cuts out” exactly the SS-integral points, transforming motivic and cohomological information into computable analytic equations that govern finiteness of integral solutions for X=P1{0,1,}X = \mathbb{P}^1 \setminus \{0,1,\infty\}, and providing a model for higher-dimensional generalizations in the Chabauty–Kim program (Dan-Cohen et al., 2012).

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