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Flexes are contacts of order at least three with the tangent line

Statement

Assume the Axiom of Choice, inherited from the cited local-length, smoothness or Bezout suppliers.

Let C be a plane projective curve over the algebraically closed field k and let p∈C be a smooth point with tangent line T=TpC. Then p is a flex of C if and only if T is not a component of C and the nonzero restriction to T of a defining form of C vanishes at p to order at least three. Whenever T is not a component,

Ip(C,T)=ord⁡p(F∣T).

In particular p is an ordinary flex exactly when Ip(C,T)=3, and for a smooth conic or a line there are no flexes.

Facts & Assumptions

Given: AC The Axiom of Choice, a plane projective curve C=V(F) of degree d over the algebraically closed field k and a smooth point p∈C with tangent line T=TpC Plane projective curves and their components, Multiplicity one characterises smooth points with a unique tangent.

[F1]

A flex is a smooth point whose tangent line is not a component and has Ip(C,TpC)≥3, an ordinary flex one with Ip(C,TpC)=3 Flexes and bitangents defined by intersection multiplicity.

[F2]

If the tangent line T is not a component of C, then Ip(C,T)=ord⁡p(F∣T), with order taken in the DVR OT,p, by Intersection with a line is the order of vanishing of the restricted equation. The equivalent valuation along the smooth curve C is ord⁡p(l∣C) for a local equation l of T Intersection with a smooth curve is a vanishing order, Uniformising parameters at smooth points of a plane curve.

[F3]

When T is not contained in C, the restriction F∣T is a nonzero binary form of degree d; the order of vanishing at p is at most d by the root bound for the restriction Flexes and bitangents defined by intersection multiplicity, Plane projective curves and their components.

Proof

1.1F1F2F3given

If T is a component of C, its contact has infinite multiplicity and p is not a flex by [F1]. Otherwise regard T as the smooth curve and restrict the local equation F of C to it. By symmetry of the defining local quotient and [F2], Ip(C,T)=ord⁡p(F∣T); [F3] makes this finite and at most d.

2.1F1step 1.1algebra

In the finite-contact case of step 1.1, by [F1] the point p is a flex exactly when Ip(C,T)≥3, i.e. by step 1.1 exactly when ord⁡p(F∣T)≥3; it is an ordinary flex exactly when both are 3.

2.2step 1.1F1F3given

If C is a smooth conic and its tangent is not a component, then d=2, so ord⁡p(F∣T)≤2<3 and no point is a flex. If C is a line, then TpC=C for every point, the pair (C,TpC) has a common component and Ip is not finite, so no point is a flex in the sense of the definition.

3.1step 1.1step 2.1step 2.2∎

Steps 1.1, 2.1 and 2.2 establish the identification, the characterisation of ordinary flexes by contact order three, and the absence of flexes on smooth conics and lines.

Depends on

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