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A point blowup lowers pairwise contact order by one and separates transverse branches

Statement

Assume the Axiom of Choice, inherited from the blowup construction (The Axiom of Choice). Let S be a regular surface over a field k (Contact order of two regular components at a point), let p be a closed point, and let Y,Z⊆S be distinct curves that are regular at p and pass through p, with contact order n=np(Y,Z)≥1 (Contact order of two regular components at a point). Let π ⁣:S′→S be the blowup of p, with exceptional curve E, and let Y′,Z′ be the strict transforms of Y,Z. Then:

  1. if n=1, then Y′ and Z′ meet E at distinct points, so they are disjoint in a neighbourhood of E;
  2. if n>1, then Y′ and Z′ meet at the point of E corresponding to their common tangent direction, the contact order of Y′ and Z′ there is n−1, and every intersection of a strict transform with E has order one.

Facts & Assumptions

Given: A regular surface S over k, a closed point p with local ring A=OS,p, a regular system of parameters x,y∈A, local equations y of Y and z of Z at p, the blowup π ⁣:S′→S of p with exceptional curve E and strict transforms Y′,Z′, and the contact order n=np(Y,Z) of Contact order of two regular components at a point.

[F1]

Contact order of two regular components at a point: n=length⁡A/(y)((A/(y))/(z)) and OY,p=A/(y) is a one-dimensional reduced Noetherian local ring; every component of Y and of Z through p is regular at p.

[F2]

Affine blowup standard charts and overlaps, Affine blowup algebras: normal form, nonzerodivisors, reducedness, domains, Flat base change for blowups, and failure without flatness, The exceptional divisor is the projectivized normal cone and associated graded ring of a regular local ring: Localizing the base at p gives the charts A[(x,y)/x] and A[(x,y)/y], with inverse ratio overlap. The exceptional curve is Proj⁡gr⁡mA, hence Pκ(p)1 after choosing parameters, since dim⁡A=2 at the contact point. The quotient presentations follow from the regular-sequence torsion calculation below.

[F3]

Affine blowup algebras: normal form, nonzerodivisors, reducedness, domains: The chart ring is the affine blowup algebra A[I/x] with IA[I/x]=xA[I/x] and x a nonzerodivisor, so on the first chart the inverse image ideal of the centre is (x).

[F4]

Total transform equals strict transform plus multiplicity times the exceptional divisor: For a reduced curve C⊆S through p whose local equation has multiplicity m at p, one has π∗C=C′+mE and C′ meets E in the 0-cycle of degree m cut out by the degree-m leading form of a local equation of C at p.

[F5]

Contact order of two regular components at a point and regular local quotient by parameter is regular: In a two-dimensional regular local ring, a regular curve germ has a prime equation with nonzero cotangent class, as shown in the definition's local-equation argument. Conversely, quotienting by an equation with nonzero cotangent class gives a regular one-dimensional local ring. Thus regularity of such a curve germ is equivalent to its equation having order one.

[F6]

Effective cartier divisor and Cartier divisor: The exceptional curve E is an effective Cartier divisor on S′, so the total transform π∗C and the expression C′+mE of [F4] are well defined as divisors.

[F7]

regular local quotient by parameter is regular, one dimensional regular local rings are dvrs and regular local rings are domains and cohen macaulay: A quotient of a regular local ring by an element with nonzero cotangent class is regular of dimension one less; in dimension one it is a discrete valuation domain.

[F8]

dimension at most embedding dimension: The dimension of a nonzero Noetherian local ring is at most its embedding dimension.

Proof

1.1F1F5F7

The regular curve germ Y has prime ideal P with A/P regular of dimension one. Its cotangent space has dimension one, so the kernel of m/m2→m/(P+m2) is nonzero. Choose y∈P with nonzero cotangent class and extend it to a parameter system x,y. The ring A/(y) is a one-dimensional regular local domain, hence a DVR. The prime P/(y) must be zero, since its quotient has dimension one, whereas the only nonzero prime in a DVR is maximal and has zero-dimensional quotient. Thus P=(y). The same argument gives a principal equation z of Z. In the DVR A/(y), xˉ is a uniformizer and the contact order is n=ord⁡xˉzˉ.

2.1F1F5step 1.1

Write ℓY and ℓZ for the leading forms of y and z in the symmetric algebra of m/m2, so ℓY=y and ℓZ=αx+βy with (α,β)≠(0,0) by the regularity of Z at p in [F5]. Since zˉ=z(x,0)=αx+O(x2) in the DVR A/(y) with uniformizer x, the order is n=1 exactly when α≠0: the tangent directions of Y and Z at p, cut out by ℓY and ℓZ, agree exactly when ℓZ is a nonzero multiple of y, that is exactly when α=0 and β≠0; hence n=1 if and only if the tangent directions differ, and in that case β may be zero or not, while for n>1 the two curves have the common tangent direction cut out by y.

3.1F2F3F4step 2.1F6

The first chart is A[T]/(xT−y): if xg=(xT−y)h, reduction modulo x and regularity of y modulo x give h=xh1, then cancellation gives g=(xT−y)h1. Thus no x-power torsion remains in the incidence quotient. Work in the first chart Spec⁡A[T]/(xT−y), T=y/x, so y=xT and E=V(x); by [F2] and [F3] this chart contains the point of E corresponding to the tangent direction cut out by y, namely T=0, and the other chart covers the remaining points, so the two charts together see all of E. By [F4] applied to Y and Z, whose local equations have multiplicity one at p, one has π∗Y=Y′+E and π∗Z=Z′+E as identities of effective Cartier divisors, well defined by [F6]; and Y′ meets E in the reduced point cut out by ℓY, Z′ in the reduced point cut out by ℓZ; explicitly in this chart the total transform of Z is V(z) with z=xh, h=z/x∈A[y/x], and Z′=V(h).

4.1F4step 2.1step 3.1

If n=1, then α≠0 by step 2.1, so h(0,0)=α≠0: the strict transform Z′ does not pass through the point Y′∩E={T=0}, and its intersection with E is cut out by ℓZ at the point of E corresponding to the tangent direction of Z, which differs from that of Y by step 2.1. On the open complement of Z′∩Y′ (a closed subset missing E) the curves Y′ and Z′ are disjoint: they meet E at distinct points and are therefore disjoint near E.

4.2F2F4F5F7F8step 1.1step 2.1step 3.1

If n>1, then α=0 and β≠0, so ℓZ=βy: both Y′ and Z′ meet E at the single point q corresponding to the common tangent direction cut out by y, namely T=0; and h(x,0)=zˉ/x=xn−1u(x) for a unit u of the DVR A/(y), because ord⁡xzˉ=n by step 1.1. The ambient local ring at q is regular: the domain chart B=A[T]/(xT−y) has B/xB=κ(p)[T], and OS′,q=B(x,T) has maximal ideal generated by x,T. The strict prime chain (0)⊊(x)⊊(x,T) gives dimension at least two, while [F8] bounds it above by its embedding dimension at most two. Hence it is regular, with x,T a cotangent basis. Since h mod x=βT is a nonzero linear form, Z′ is regular at q by [F5], and Y′=V(T) is regular there; in the DVR OY′,q≅(A/(y)) with uniformizer x, the ideal of Z′ is generated by h(x,0)=xn−1u(x), so the contact order of Y′ and Z′ at q is n−1. Finally each of Y′,Z′ meets E in a 0-cycle of degree one by [F4], so every intersection of a strict transform with E has order one.

5.1step 4.1step 4.2∎

Steps 4.1 and 4.2 prove the two assertions: for transverse branches (n=1) the strict transforms meet E at distinct points and are disjoint near E, while for n>1 they meet at the common tangent direction with contact order n−1, every intersection with E having order one.

Remarks

  • The computation uses only the first chart because the point of E cut out by y is T=0 there; when the common tangent direction is the other coordinate direction the same argument runs in the second chart with x and y interchanged.
  • The statement is the local input for resolving plane curve singularities by repeated point blowups, where it shows that the contact order of two branches drops by exactly one at each step at which they still share a tangent direction.

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