Affine centers and normalization of torsion points #
Construct coordinate-ring evaluations and their maximal ideals, and compare affine torsion points with normalization places.
An affine rational point of the plane curve f = 0.
Equations
Instances For
Evaluation at an affine rational point, descended to the coordinate ring.
Equations
- BGS.CorvajaZannier.planeCurvePointEval f z = Ideal.Quotient.lift (Ideal.span {f}) (MvPolynomial.eval₂Hom (RingHom.id K) ![(↑z).1, (↑z).2]) ⋯
Instances For
The maximal ideal of the affine coordinate ring attached to a rational point.
Equations
- BGS.CorvajaZannier.affinePlaneCurvePointMaximalIdeal f z = { asIdeal := RingHom.ker (BGS.CorvajaZannier.planeCurvePointEval f z), isMaximal := ⋯ }
Instances For
Distinct rational affine points define distinct maximal ideals.
A torsion point in the finite-field intersection, as a finite subtype.
Equations
- BGS.CorvajaZannier.TorusCurveTorsionPoint f firstOrder secondOrder = ↥(BGS.External.torusCurveTorsionIntersection K f firstOrder secondOrder)
Instances For
Forget the unit witnesses and regard a torsion point as an affine point of the plane curve.
Equations
Instances For
A finite-field torsion point determines a maximal ideal of the affine coordinate ring.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The first torsion function belongs to the maximal ideal of its point.
The second torsion function belongs to the maximal ideal of its point.
The affine normalization of the plane-curve coordinate ring inside its fraction field.
Equations
Instances For
Choose one normalization branch above an affine maximal ideal. Lying over guarantees that such a branch exists; no smoothness is assumed.
Equations
- BGS.CorvajaZannier.planeCurveNormalizationBranch f m = { asIdeal := Classical.choose ⋯, isMaximal := ⋯ }
Instances For
Chosen normalization branches above distinct affine maximal ideals remain distinct, because their contractions are distinct.
The chosen branch of the normalization above a torsion point.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The first torsion function vanishes on the chosen normalization branch.
The second torsion function vanishes on the chosen normalization branch.
An integral-closure model of the plane-curve function field has that function field as its fraction field.
Membership in a height-one prime gives at least one unit of additive finite-place order.
Generic local bridge for any Dedekind integral-closure model B of the
curve's function field. A maximal ideal of B lying over the torsion point
is a finite place, and both torsion functions have order at least one there.
The branch is an explicit parameter, so a later global normalization or projective model can supply its own chosen lift.