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Point Blowup Resolution on Arbitrary Regular Surfaces

1 · Prerequisites

2 · Summary

This page proves embedded resolution of a reduced curve on an arbitrary Noetherian regular surface by finitely many point blowups, assuming that each irreducible component has finite normalization, without a plane-curve or smoothness-over-a-field hypothesis. It uses the blowup machinery of blowups-exceptional-divisors-and-strict-transforms, the finiteness theory of normalization-finiteness-for-affine-domains, the vocabulary of flat-smooth-and-etale-morphisms only to keep regularity distinct from smoothness, and the local factoriality of nonaffine-algebraic-groups-barsotti-chevalley-and-abelian-varieties for the unique-factorization property of regular local rings.

The local input is the behaviour of a single point blowup of a regular surface: the blowup stays regular of pure dimension two (Point blowups of regular surfaces stay regular, with rational exceptional curves at two-dimensional local rings), and the fibre over a closed point p is Pκ(p)1 in the two-dimensional case, while no smoothness over a ground field is asserted. The local contact of two curve branches is measured by the intersection multiplicity mp(Y∩Z)=length⁡OX,p(OY∩Z,p) (Intersection multiplicity of closed subschemes at a point); blowing up a point at which one branch is regular decreases every contact multiplicity over that point and makes the new exceptional contacts equal to one (A point blowup drops pairwise intersection multiplicity by at least one).

On the one-dimensional side, the blowup of an integral Noetherian curve at a closed point is finite, with fibre the projectivized associated graded scheme, and it is an isomorphism exactly at regular points (The blowup of a one-dimensional integral Noetherian scheme at a closed point is finite). Consequently a finite normalization factors through every point blowup, and blowing up a non-regular point strictly increases the coherent subalgebra β∗OY1 inside the fixed finite normalization (The finite normalization of a curve factors through the blowup of a closed point, Blowing up a non-regular point strictly increases the finite normalization subalgebra). Noetherian stabilization of increasing sequences of coherent subsheaves (Increasing sequences of coherent subsheaves of a coherent module on a Noetherian scheme stabilize) then forces the regularization process to terminate after finitely many steps, both intrinsically (Regularization of a one-dimensional integral curve with finite normalization by point blowups) and for a curve inside an arbitrary Noetherian ambient scheme (Regularization of an integral curve on an arbitrary Noetherian ambient scheme), where the strict transform of the curve is computed as the intrinsic blowup.

The global theorem combines these tools. Finitely many curve components are first regularized and then separated so that their strict transforms are pairwise disjoint regular curves (Separation of finitely many curve components by point blowups). On a regular surface a reduced curve is already an effective Cartier divisor, and its total transform under point blowups remains one; after separating the original components, repeatedly lowering the maximum contact multiplicity among all components of the total-transform support to one, and resolving the finitely many points at which three or more components meet, the support is a strict normal crossings divisor (Strict normal crossings divisor on a regular surface), which is the embedded resolution theorem of the page (Embedded strict-normal-crossings resolution of a reduced curve on a regular surface). The conclusion is SNC support with regular irreducible components; the support itself can fail to be regular at a crossing. No relative-SNC or smoothness assertion over a non-perfect field, or higher-dimensional resolution claim, is included.

3 · Logical flowchart

4 · Definitions, theorems and proofs

DefinitionDefinition: Literature-sourcedProof: Not applicablejudge pass (gpt-6.1-sol)Open item page →

Intersection multiplicity of closed subschemes at a point

Definition

Let X be a locally Noetherian scheme, let Y,Z⊆X be closed subschemes, and let p∈Y∩Z be a closed point. Assume that Y is integral of dimension one (Integral schemes, Chain dimension and the empty-space convention) and that the generic point of Y is not contained in Z; since Z is closed, this means Y⊈Z, and it excludes every one-dimensional component of Y∩Z. The local intersection multiplicity of Y and Z at p is

mp(Y∩Z):=length⁡OX,p(OY∩Z,p),

where OX,p is the local ring of X at p (A local ring is a nonzero commutative ring with a unique maximal ideal), where IY∩Z=IY+IZ is the sum of the ideal sheaves of Y and Z, and where

OY∩Z,p=OX,p/IY∩Z,p

is the local ring at p of the scheme-theoretic intersection (Scheme-theoretic fibre).

The definition is meaningful. Write η for the generic point of the integral one-dimensional scheme Y. By hypothesis η∉Z, so η∉Y∩Z. An irreducible component of the closed subset Y∩Z is the closure of one of its points, hence a closed subset of Y not containing η. Such a component is a single closed point of Y: if a point y≠η of Y had a closure containing a further point z≠y, then the closures of z, of y and of η would form a strict chain of irreducible closed subsets of length two, contradicting dim⁡Y=1 (Chain dimension and the empty-space convention); therefore Y∩Z is supported in the closed points of Y that lie on Z. In particular OY∩Z,p, being a quotient of the Noetherian local ring OX,p (Locally Noetherian and Noetherian schemes, Noetherian commutative rings and modules), is a zero-dimensional Noetherian local ring, and such a ring has a finite composition series over itself (Composition series and length of a module); so the length is a well-defined natural number (Remarks). The value depends only on the local data at p: pulling back along the canonical localization morphism Spec⁡OX,p→X does not change OX,p, IY,p or IZ,p, so replacing X by an open neighbourhood of p leaves mp(Y∩Z) unchanged. Finally mp(Y∩Z)≥1, because p∈Y∩Z makes OY∩Z,p a nonzero ring.

The invariant is the one used for strict transforms: after blowing up a closed point, one computes mq(Y′∩Z′) in the blown-up ambient scheme at a closed point q lying over p.

Remarks

[R1] A zero-dimensional Noetherian local ring has finite length. Let (A,m) be Noetherian local with dim⁡A=0. Every prime ideal of A is then equal to m, so the nilradical Nil⁡(A), which is the intersection of all prime ideals, equals m; hence m is nilpotent, say mN=0 (The nilradical of a Noetherian ring is nilpotent). This gives a finite filtration A=m0⊇m⊇⋯⊇mN=0 by ideals of A. Each successive quotient mi/mi+1 is a module over the field A/m that is generated by the images of a finite generating set of the ideal mi, so it is a finite-dimensional A/m-vector space and has finite length; the length of A is the sum of these finitely many lengths (Module length is additive in short exact sequences). No choice principle beyond the ambient definition is used.

[R2] On this page, Y may be the strict transform of a curve and Z another curve component or an exceptional divisor; Y∩Z is their zero-dimensional contact locus. When both components are regular curves on a regular surface, mp(Y∩Z)≥2 is exactly the tangency that the resolution process must remove: the point-blowup drop lemma compares mp(Y∩Z) with the multiplicities mq(Y′∩Z′) at points of the blown-up surface lying over p.

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6.1-sol)Open item page →

Increasing sequences of coherent subsheaves of a coherent module on a Noetherian scheme stabilize

Statement

Let X be a Noetherian scheme and let F be a coherent OX-module (Coherent module sheaves). If F1⊆F2⊆F3⊆⋯ is an increasing sequence of coherent OX-submodules of F, then the sequence stabilizes: there is an index n0 with Fn=Fn0 for every n≥n0.

The proof inherits the Axiom of Choice through the affine quasi-coherent interface (Affine quasi-coherent sheaves are modules, The Axiom of Choice); apart from that interface it selects nothing and is otherwise choice-free.

Facts & Assumptions

[F1]

A scheme is Noetherian if and only if it has a finite affine open cover by spectra of Noetherian rings (Locally Noetherian and Noetherian schemes).

[F2]

On a locally Noetherian scheme a quasi-coherent module is coherent if and only if it is of finite type (Coherent sheaves on a locally Noetherian scheme); on an affine scheme Spec⁡A, finite type means that the module is isomorphic to M~ for a finitely generated A-module M (Finite type and finitely presented module sheaves, Coherent module sheaves).

[F3]

For an affine scheme U=Spec⁡A, the functor Γ(U,−) is an equivalence from quasi-coherent OU-modules to A-modules with inverse M↦M~ (Affine quasi-coherent sheaves are modules, Quasi-coherent module on a scheme). An equivalence of abelian categories preserves and reflects monomorphisms, so a quasi-coherent subsheaf G⊆H of a quasi-coherent sheaf on U corresponds to the inclusion of A-modules Γ(U,G)⊆Γ(U,H), and G is recovered from its module of sections; thus two quasi-coherent subsheaves of H with the same module of sections are equal.

[F4]

If M is a finitely generated module over a Noetherian ring A, then M is a Noetherian module, so every ascending sequence of submodules of M stabilizes (Finite modules over Noetherian rings are Noetherian, Finite generation, ACC, and maximal-condition characterizations of Noetherian modules, Noetherian modules: every submodule is finitely generated). This uses no choice principle.

Proof

Given: A Noetherian scheme X, a coherent OX-module F and an increasing sequence F1⊆F2⊆⋯ of coherent OX-submodules of F.

1.1F1given

If X=∅ there is nothing to prove, so assume X≠∅. By [F1] fix a finite affine open cover X=U1∪⋯∪Ur with Ui=Spec⁡Ai and Ai Noetherian; necessarily r≥1. This is a single existential instantiation of the cover granted by the definition of a Noetherian scheme, not a choice from an infinite family.

2.1F2F3step 1.1

Fix i. The restriction F∣Ui is quasi-coherent, and it is of finite type because F is coherent and the restriction of a coherent module to an open subscheme is coherent; by [F2] put Mi:=Γ(Ui,F), a finitely generated Ai-module. Each Fn∣Ui is likewise a coherent, hence finite type, quasi-coherent subsheaf of F∣Ui, and Ni,n:=Γ(Ui,Fn) is a finitely generated Ai-submodule of Mi.

3.1F3step 2.1

For m≤n the inclusion Fm⊆Fn induces, under the equivalence of [F3], an inclusion of Ai-modules Ni,m⊆Ni,n; in particular Ni,1⊆Ni,2⊆Ni,3⊆⋯ is an ascending sequence of submodules of Mi.

4.1F4step 3.1

By [F4] the module Mi is Noetherian, so the ascending sequence of step 3.1 stabilizes: there is an integer si with Ni,n=Ni,si for every n≥si. This holds for each fixed i with no choice used.

5.1F3step 1.1step 4.1algebra∎

Set s:=max⁡{s1,…,sr}, which exists because r is finite. Let n≥s. For every i we have Ni,n=Ni,s, both being Ni,si, so the quasi-coherent subsheaves Fn∣Ui and Fs∣Ui of F∣Ui have the same module of sections and are therefore equal by [F3]. Equality of subsheaves of a quasi-coherent sheaf can be checked on the members of an open cover, and the Ui cover X; hence Fn=Fs for every n≥s, which is the asserted stabilization with n0=s.

DefinitionDefinition: Literature-sourcedProof: Not applicablejudge pass (gpt-6.1-sol)Open item page →

Strict normal crossings divisor on a regular surface

Definition

Assume the Axiom of Choice for the local factoriality and the equivalence argument below (The Axiom of Choice). Let S be a regular surface: a locally Noetherian scheme of pure dimension two all of whose local rings are regular (A local ring is a nonzero commutative ring with a unique maximal ideal, embedding dimension and regular local ring). Let D⊆S be a reduced curve, that is, a reduced closed subscheme of pure dimension one; equivalently, a reduced effective Cartier divisor on S of pure dimension one (Effective cartier divisor, Cartier divisor).

Then D is a strict normal crossings divisor (an SNC divisor) on S if at every closed point p of S one of the following holds:

(a) no irreducible component of D passes through p;

(b) exactly one irreducible component of D passes through p, and it is regular at p;

(c) exactly two irreducible components Y1,Y2 of D pass through p, both are regular at p, and they meet transversally at p, that is, mp(Y1∩Y2)=1 (Intersection multiplicity of closed subschemes at a point).

Equivalently (Stacks, Lemma 41.21.2, in the locally Noetherian case): D is reduced, every irreducible component of D is a regular scheme, every nonempty scheme-theoretic intersection of two distinct irreducible components of D is a regular scheme of dimension zero, and no three distinct irreducible components of D meet at a point. The equivalent local equation form is: at every point p∈S the stalk ideal ID,p⊆OS,p is principal, with a generator of the form x1⋯xr where r≥0 and x1,…,xr extend to a regular system of parameters of OS,p (for a closed point of the surface, 0≤r≤2; r=0 means the unit ideal).

No smoothness over a ground field is part of the definition; over a non-perfect field the components are regular but need not be smooth. The empty curve D=∅ and a single regular component are SNC divisors by (a) and (b).

Remarks

[R1] The pointwise conditions and the regular-intersection criterion agree. At a closed point p∈D, the local ring of an integral curve component through p has dimension one. Its defining prime in A=OS,p is nonzero, since that component has dimension one and is not an irreducible component of the pure two-dimensional surface. The chain from the zero prime of the regular local domain A through this prime to its maximal ideal has length two. Thus A has dimension two, and is a unique factorization domain (Regular local rings are unique factorization domains). The irreducible components of D through p correspond to the height-one prime ideals p1,…,pr containing the radical ideal ID,p, and ID,p=p1∩⋯∩pr is generated by the product of prime generators x1⋯xr of those primes, a nonzerodivisor; so near p the curve has the local equation x1⋯xr. A component Yi is regular at p exactly when its local equation xi extends to a regular system of parameters of A (regular local quotient by parameter is regular), which for one element of a two-dimensional regular local ring means that xi is not in mp2. Conversely, if A/(xi) is regular of dimension one, its cotangent space has dimension one; if xi lay in mp2, the quotient cotangent space would still be the two-dimensional mp/mp2, a contradiction. For two distinct components Y1,Y2 the scheme-theoretic intersection near p is cut out by (x1,x2); it is a regular scheme of dimension zero precisely when (x1,x2)=mp, that is, when x1,x2 form a regular system of parameters, and this is exactly mp(Y1∩Y2)=1. Three distinct components cannot meet at p when the criterion holds, because ⋂j∈JDj for a three-element set J would have to be regular of codimension three inside the surface S and therefore empty. Conversely, the pointwise conditions give the criterion: components are regular, every local intersection of two distinct components is a reduced point, and no three components meet. This is the surface case of the finite-subset form of Stacks Lemma 41.21.2.

[R2] Why the two descriptions of the ambient object agree. For a reduced closed subscheme D⊆S of pure dimension one, being an effective Cartier divisor is a local condition: at p the ideal ID,p is generated by one nonzerodivisor. If p∉D it is the unit ideal; if p is the generic point of a component, OS,p is a discrete valuation ring and ID,p is principal; if p is a closed point, [R1] exhibits the principal generator x1⋯xr. Thus every reduced curve on a regular surface is a reduced effective Cartier divisor, and conversely a reduced effective Cartier divisor of pure dimension one is a reduced curve.

[R3] Closed points suffice. On a scheme of dimension at most two, every non-closed point of D is the generic point of an irreducible component, where the local ring of D is a field and no two distinct components meet; so regularity of the components and all pairwise contacts are detected at closed points. This is why the definition tests only closed points.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Point blowups of regular surfaces stay regular, with rational exceptional curves at two-dimensional local rings

Statement

Assume the Axiom of Choice (The Axiom of Choice). Let S be a regular surface: a locally Noetherian scheme of pure dimension two all of whose local rings are regular (embedding dimension and regular local ring). Let p∈S be a closed point and let π:S′→S be the blowup of S in p (Blowup of a scheme along an ideal sheaf), with exceptional curve E=π−1(p) (Exceptional subscheme of a blowup). Then S′ is regular of pure dimension two, and E is an effective Cartier divisor on S′. Moreover:

  1. if dim⁡OS,p=2, there is an isomorphism E≅Pκ(p)1 over κ(p);
  2. if dim⁡OS,p=1, the morphism π is an isomorphism and E is the reduced point Spec⁡κ(p);

and in either case π restricts to an isomorphism S′∖E→S∖{p}. In particular the blowup creates no new singular one-dimensional component: the only new one-dimensional component is E, which is a regular curve in case 1.

No smoothness over any ground field is asserted: over a non-perfect residue field extension the blowup can be regular without being smooth over the ground field (Smooth morphism of schemes), and this lemma claims regularity only.

Facts & Assumptions

[F1]

Local algebra of the regular local ring A=OS,p in the case dim⁡A=2: A is a Noetherian regular local ring of dimension two, hence an integral domain and a unique factorization domain; its maximal ideal m=(x,y) is generated by a regular system of parameters. The polynomial ring A[T] is regular and dim⁡A[T]=3, localizations of a regular ring are regular, and for z∈m∖m2 the quotient A/(z) is regular local of dimension one less; in a regular local ring a generating list of the maximal ideal with as many entries as the dimension is a regular system of parameters, whose classes form a basis of the cotangent space (regular local domain induction, Regular local rings are unique factorization domains, localisation and polynomial extension of regular rings, localisations of regular local rings are regular, regular local quotient by parameter is regular, A Noetherian polynomial ring has dimension one larger, regular system of parameters equivalent basis).

[F2]

If A is a regular local ring of dimension two with residue field κ, then any cotangent basis induces a graded κ-algebra isomorphism gr⁡mA≅κ[X,Y] with standard grading (associated graded ring of a regular local ring).

[F3]

A one-dimensional regular local ring is a discrete valuation ring: its maximal ideal is principal, generated by a uniformizer (one dimensional regular local rings are dvrs, embedding dimension and regular local ring).

[F4]

The Axiom of Choice is assumed for the cited local-algebra theorems ([F1], [F2]) as stated there; no further selection is made in this proof (The Axiom of Choice).

Proof

Given: AC, a regular surface S, a closed point p∈S, the blowup π:S′=Bl⁡pS→S and the exceptional curve E=π−1(p).

1.1F1F3given

Take a Noetherian affine neighbourhood U=Spec⁡R of p, with center ideal n, and put A=Rn=OS,p. The blowup restricts to the blowup on U (Blowups restrict to open subschemes of the base). Flat base change along R→A identifies its further pullback with Bl⁡mSpec⁡A, where m=nA (Flat base change for blowups, and failure without flatness). The local ring of any point above p is unchanged by this localization, because every element of R∖n is already a unit there. Thus regularity above p can be checked over A. Its dimension is one or two: p cannot be a zero-dimensional irreducible component of the pure two-dimensional regular scheme, and the dimension is at most two. The two dimensions are treated separately below.

2.1F1step 1.1algebra

Suppose dim⁡A=2 and choose regular parameters x,y generating m. The standard charts are A[m/x] and A[m/y] (Affine blowup standard charts and overlaps). By the power-torsion presentation of Affine blowup algebras: normal form, nonzerodivisors, reducedness, domains, the first is the quotient of B′=A[T]/(xT−y) by its x-power torsion. This torsion is zero. Indeed A/(x) is a regular one-dimensional local domain and y is nonzero modulo x by [F1]. If xg=(xT−y)h in A[T], reduction modulo x gives y‾ h‾=0 in the domain (A/(x))[T], so h=xh1; cancelling x in the domain A[T] gives g=(xT−y)h1. Thus multiplication by x is injective on B′, and A[m/x]=B′. It is a domain because it embeds into A[1/x]. The other chart is symmetrically A[U]/(yU−x).

2.2F3step 1.1

In the case dim⁡A=1, the one-dimensional regular local ring A is a discrete valuation ring [F3], so m is principal generated by a uniformizer, the center ideal is invertible on a neighbourhood of p, and the blowup of an invertible ideal is an isomorphism: π is an isomorphism (Blowing up an effective Cartier divisor does nothing). Then E=π−1(p) is the closed point p with its reduced structure Spec⁡κ(p), and it is an effective Cartier divisor.

3.1F1step 2.1casesalgebra

Consider a prime Q of B=A[T]/(xT−y) whose contraction q in A is not m. If x∉q, the localized chart is B⊗AAq=Aq by solving T=y/x. If x∈q, then y∉q; in the localized chart y=xT is a unit, so x is a unit and the chart is Aq[1/x]. In either case BQ is a localization of the regular ring Aq and is regular. This includes contraction q=(0), where the local ring is a field.

3.2F1step 2.1algebra

For a prime Q of B over m, its preimage P in C=A[T] is either mC or (x,y,h(T)), where h lifts a monic irreducible polynomial of κ[T]. The regular local ring CP has dimension two in the first case and three in the second: the prime chains (0)⊊(x)⊊mC and, in the second case, mC⊊P give the lower bounds, while the displayed two or three maximal-ideal generators give the upper bounds on dimension. Consequently x,y, or x,y,h, form a cotangent basis by [F1]. The class of xT−y in PCP/(PCP)2 is the residue of T times the class of x minus the class of y, and is nonzero because the coefficient of y is −1. The parameter-quotient lemma therefore makes BQ=CP/(xT−y) regular. Its dimension is one for P=mC (the generic point of the exceptional curve), and two for P=(x,y,h).

4.1F1step 1.1step 2.2step 3.1step 3.2

Steps 3.1 and 3.2 prove regularity on the x-chart, and the symmetric proof proves it on the y-chart; step 1.1 transfers these local rings to all points above p. Away from p the blowup is an isomorphism (The blowup is an isomorphism off the center), so S′ is regular everywhere. It is pure of dimension two as well. In the dimension-one case this follows from the identity in step 2.2. In the dimension-two case the local charts above p are domains of dimension two: all their prime-local dimensions are at most two, and step 3.2 exhibits dimension-two closed local rings. The exceptional divisor is not an irreducible component, since its chart equation x (or y) is a nonzerodivisor. Thus every component meeting the exceptional divisor is the strict transform of the corresponding component through p and has dimension two; every other component is unchanged. The components of the original regular surface all have dimension two, so the same holds for S′. The dimension-one local ring at the generic point of E does not contradict pure dimension two.

5.1F2step 4.1

The exceptional curve is effective Cartier: the pulled-back center ideal IpOS′ is invertible with nonzerodivisor local generators, and E=V(IpOS′) is the associated effective Cartier divisor (The pulled-back center ideal is the relative twist; the exceptional divisor is Cartier). In the case dim⁡A=2, the normal cone theorem identifies E with Proj⁡Z(gr⁡IpOS) over Z={p} (The exceptional divisor is the projectivized normal cone); on the one-point scheme Z=Spec⁡κ(p) its graded pieces are mn/mn+1, so E≅Proj⁡(gr⁡mA) and [F2] gives E≅Proj⁡κ(p)[X,Y]=Pκ(p)1 over κ(p). In particular E is a regular curve, so the blowup creates no new singular one-dimensional component.

6.1F4step 4.1step 5.1step 2.2∎

Collecting: S′ is regular of pure dimension two and E is effective Cartier by steps 4.1 and 5.1; in the two-dimensional case E≅Pκ(p)1 by step 5.1; in the one-dimensional case π is an isomorphism and E=Spec⁡κ(p) by step 2.2; and π restricts to an isomorphism off E by step 4.1. Only regularity of S and of the local charts was used, never smoothness over a field, so no smoothness claim is made.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

A point blowup drops pairwise intersection multiplicity by at least one

Statement

Assume the Axiom of Choice (The Axiom of Choice). Let X be a locally Noetherian scheme, let Y,Z⊆X be closed subschemes and let p∈Y∩Z be a closed point such that Y is integral of dimension one, the generic point of Y is not contained in Z, and the local ring OY,p is regular. Let π:X′→X be the blowup of X in p (Blowup of a scheme along an ideal sheaf), with exceptional subscheme E=π−1(p) (Exceptional subscheme of a blowup), and let Y′,Z′ be the strict transforms of Y and Z (Strict transform of a closed subscheme). Then:

  1. π restricts to an isomorphism Y′→Y;
  2. Y′ meets E in exactly one point q, which is the unique point of Y′ over p, and mq(Y′∩E)=1 (Intersection multiplicity of closed subschemes at a point);
  3. if q also lies on Z′, then mq(Y′∩Z′)<mp(Y∩Z).

In particular the blowup strictly decreases the intersection multiplicity at every point over p where the strict transforms still meet, and if mp(Y∩Z)=1 then Y′ and Z′ are disjoint over p.

Facts & Assumptions

[F1]

A one-dimensional regular local ring is a discrete valuation ring, its maximal ideal is principal and generated by a uniformizer π, every nonzero ideal is a power of the maximal ideal, and for x=uπn with u a unit one has ℓV(V/(x))=n; in particular the quotient has finite length and its length is the valuation (one dimensional regular local rings are dvrs, Every DVR is a PID, Length and valuation in a DVR, Composition series and length of a module).

[F2]

The local intersection multiplicity is mp(Y∩Z)=length⁡OX,p(OY∩Z,p) whenever the hypotheses of the definition hold (Intersection multiplicity of closed subschemes at a point).

[F3]

The Axiom of Choice is assumed, inherited from the blowup and strict transform constructions and from [F1]; no further selection is made (The Axiom of Choice).

Proof

Given: AC, X,Y,Z,p, the blowup π:X′→X in p, the exceptional subscheme E=π−1(p) and the strict transforms Y′,Z′.

1.1F1F2given

Put A=OX,p with maximal ideal m, let I=IY,p and J=IZ,p be the stalk ideals, so that A/I=OY,p is a one-dimensional regular local ring and hence a discrete valuation ring with valuation v [F1]. Choose x1∈m whose image x‾1∈A/I is a uniformizer; then m=I+(x1), because both sides are ideals contained in m and their images in the discrete valuation ring A/I are equal to its maximal ideal. The image J(A/I) is a nonzero ideal of the valuation ring, so J(A/I)=(x‾1 N) for a unique integer N≥1, and N=min⁡{v(g‾):g∈J}; pick f∈J with v(f‾)=N. By [F2], N=ℓA/I(A/(I+J))=mp(Y∩Z). All claims are local over p and its unique preimage, and blowups commute with the flat base change Spec⁡A→X (Flat base change for blowups, and failure without flatness), and localizing the chart saturation (JB):x1∞ commutes with taking this schematic closure: a fraction lies in the localized saturation exactly when some power of x1 carries it into the localized ideal. Thus we compute in the local model Bl⁡m(Spec⁡A).

2.1F1step 1.1

The center ideal on Y is IpOY, whose stalk at p is m(A/I)=(x‾1); it is not the zero ideal IOY defining Y itself. It is the unit ideal away from p, and its generator at p is a nonzerodivisor. Coherence allows the stalk generator to generate on a neighbourhood of p, so this ideal sheaf is invertible on Y. The strict transform of Y is its blowup in this induced center ideal (Strict transforms of closed subschemes are blowups of the subscheme), and the blowup of an invertible ideal is an isomorphism (Blowing up an effective Cartier divisor does nothing). Hence Y′→Y is an isomorphism and has exactly one point q above p, with local ring A/I.

3.1F1step 1.1step 2.1algebra

The x1-chart of the local blowup is B=A[m/x1]. Mapping y/x1n∈B (with y∈mn) to the unique element a‾∈A/I with y‾=a‾ x‾1 n gives a well-defined A-algebra homomorphism ψ:B→A/I: existence holds because mn⊆I+(x1n), uniqueness because x‾1 is a nonzerodivisor of the domain A/I, and compatibility with the relations of the localisation holds because x1k(x1my−x1ny′)=0 implies x‾1 k+m+n(ψ(y/x1n)−ψ(y′/x1m))=0. The composite of ψ with the chart morphism Spec⁡B→Spec⁡A is the closed immersion Spec⁡(A/I)↪Spec⁡A; since the pullback of m to Spec⁡(A/I) is the invertible ideal (x‾1), the universal property of the blowup gives a unique lift Spec⁡(A/I)→Bl⁡m(Spec⁡A), and this lift is the strict transform Y′ in the chart (Universal property of the blowup, Affine blowup standard charts and overlaps, Affine blowup algebras: normal form, nonzerodivisors, reducedness, domains, Strict transform of a closed subscheme).

4.1F1step 1.1step 3.1algebra

In the chart the exceptional subscheme is V(x1): the pulled back center ideal mO is generated by the nonzerodivisor x1 and E=V(mO) (The pulled-back center ideal is the relative twist; the exceptional divisor is Cartier, Affine blowup algebras: normal form, nonzerodivisors, reducedness, domains). Hence the scheme-theoretic intersection Y′∩E is computed in the chart by A/I⊗BB/(x1)=(A/I)/(x‾1(A/I))=A/(I+(x1))=A/m=κ(p); so Y′∩E is a single reduced point q with residue field κ(p) and mq(Y′∩E)=ℓOX′,q(κ(q))=1, proving claim 2.

4.2F1step 1.1step 2.1step 3.1

The strict transform of Z in the chart is cut out by the saturation J′=(JB):x1∞, the closure of V(JB) on the open chart complement of E (Strict transform of a closed subscheme); it contains f/x1, because x1⋅(f/x1)=f∈JB. Let K=ψ(J′)⊆A/I be the image, an ideal of the discrete valuation ring A/I containing ψ(f/x1)=f‾/x‾1, which has valuation N−1. If q∈Z′, then the closed subscheme Y′∩Z′ of Y′=Spec⁡(A/I) contains the closed point q, so K is a proper ideal contained in the maximal ideal (x‾1) and therefore K=(x‾1 j) for some j≥1; from x‾1 N−1∈K we get j≤N−1, and hence mq(Y′∩Z′)=ℓA/I(A/I/K)=j≤N−1<N=mp(Y∩Z) [F1], proving claim 3.

5.1F3step 2.1step 4.1step 4.2∎

Finally, if mp(Y∩Z)=N=1, then the element f‾/x‾1 of step 4.2 is a unit, so K is the unit ideal whenever q∈Z′, a contradiction; hence q∉Z′, and since q is the only point of Y′ over p by step 2.1, the strict transforms Y′ and Z′ are disjoint over p. This completes claims 1-3 and the additional assertions.

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The blowup of a one-dimensional integral Noetherian scheme at a closed point is finite

Statement

Assume the Axiom of Choice (The Axiom of Choice). Let Y be an integral Noetherian scheme of dimension one (Integral schemes, Chain dimension and the empty-space convention) and let p∈Y be a closed point. Let β:Y1=Bl⁡pY→Y be the blowup of Y in p (Blowup of a scheme along an ideal sheaf). Then β is proper and of finite type, is locally H-projective, and admits the global closed immersion Y1↪Proj⁡YSym⁡(Ip) for the coherent center ideal Ip. The presenting sheaf Ip is coherent and need not be locally free or globally generated. This does not assert a global H-projective immersion into PYN for a single integer N. It restricts to an isomorphism over Y∖{p}; its fibre over p is the projectivized associated graded scheme Proj⁡(gr⁡mpOY,p) (The exceptional divisor is the projectivized normal cone), which is a finite scheme over the residue field κ(p); consequently β is quasi-finite and therefore finite. Moreover β is an isomorphism if and only if OY,p is regular, equivalently if and only if the maximal ideal mp is invertible; in the regular case β∗OY1=OY.

Facts & Assumptions

[F1]

Let A=OY,p with maximal ideal m. Since Y is integral, Y has a nonempty affine open cover by spectra of domains, so A is a domain; since Y is Noetherian, A is a Noetherian local ring; and since p is a closed point of the one-dimensional scheme Y, dim⁡A=1 (Integral schemes, Locally Noetherian and Noetherian schemes, Every quotient and every localisation of a Noetherian ring is Noetherian, Chain dimension and the empty-space convention).

[F2]

Hilbert-Samuel theory: for the Noetherian local ring (A,m) and M=A≠0 with ideal of definition m, the function χ(n)=ℓA(A/mn+1) agrees with a polynomial for large n whose degree is dim⁡Supp⁡(A)=1; the differences φ(n)=ℓA(mn/mn+1)=χ(n)−χ(n−1) are therefore eventually constant (The Hilbert-Samuel function and eventual Hilbert-Samuel polynomial of a finite local module, The degree of the Hilbert-Samuel polynomial equals the dimension of the support).

[F3]

Projective Hilbert theory over a field k: for a closed subscheme E=V+(I)=Proj⁡(k[x0,…,xr]/I)↪Pkr with OE(1) the restriction of the twisting sheaf, the Hilbert polynomial of OE exists, agrees with hOE(n)=dim⁡kH0(E,OE(n)) for all large n, and has degree dim⁡Supp⁡OE=dim⁡E; moreover H0(Pkr,O(n)) is the degree-n part of k[x0,…,xr], and Serre vanishing kills H1(Pkr,IE(n)) for all large n, where IE is the coherent ideal sheaf of E. The homogeneous-ideal/saturation dictionary identifies the chart ideals of I and Isat; the eventual coordinate-ring comparison is derived below (Closed subschemes of projective space and saturated ideals, Projective scheme of a homogeneous quotient and its standard affine charts, Global sections of projective twists, Serre vanishing for coherent sheaves and ample twists, Hilbert function and Euler characteristic on a projective scheme, Euler characteristic is a Hilbert polynomial, Degree of the coherent Hilbert polynomial).

[F4]

Properness and finiteness: a projective morphism is proper and of finite type, and every proper quasi-finite morphism is finite; quasi-finiteness is finite type together with zero-dimensional fibres at every point (Projective morphisms are proper, A proper quasi-finite morphism is finite, Quasi-finite morphisms of schemes).

[F5]

A one-dimensional regular local ring is a discrete valuation ring, and a nonzero Noetherian local domain of dimension one is a discrete valuation ring exactly when its maximal ideal is principal (one dimensional regular local rings are dvrs, Equivalent characterizations of a DVR).

[F6]

The Axiom of Choice is assumed, inherited from the blowup, Hilbert-Samuel and projective-cohomology suppliers cited above (The Axiom of Choice).

Proof

Given: AC, an integral Noetherian one-dimensional scheme Y, a closed point p∈Y and the blowup β:Y1=Bl⁡pY→Y.

1.1F1F4givenalgebra

Put Ip for the coherent ideal of the closed point. Multiplication gives a canonical graded surjection Sym⁡(Ip)↠⨁n≥0Ipn: it sends a degree-n product of local sections to their product in Ipn (Symmetric algebra of a quasi-coherent module). Relative Proj is constructed on affine base opens (Relative Proj of a graded quasi-coherent algebra). On each standard homogeneous open, the quotient map induces a surjection on degree-zero localized coordinate rings, hence a closed immersion. These maps come from the same graded quotient and glue to the global closed immersion Y1↪Proj⁡YSym⁡(Ip), the projective presentation asserted here. Locally the center has finitely many generators, so Blowups of finite type ideals are locally H-projective, and proper gives local embeddings into finite-dimensional projective spaces; it also gives global properness, and finite type follows from those local embeddings. Away from p the blowup is an isomorphism (The blowup is an isomorphism off the center), so every fibre away from p is a single point. By [F1], A=OY,p is a Noetherian local domain of dimension one.

2.1F1step 1.1

The fibre E=β−1(p) is canonically Proj⁡Z(gr⁡mpOY) over Z={p}=Spec⁡κ(p) (The exceptional divisor is the projectivized normal cone); over the one-point base Z this is Proj⁡(S) with S=gr⁡mA=⨁n≥0mn/mn+1, a graded κ(p)-algebra generated in degree one by the finite-dimensional space m/m2. Fixing generators of m/m2 presents S as a quotient of a polynomial ring κ(p)[x0,…,xr], so E=V+(I)=Proj⁡(S) is a closed subscheme of Pκ(p)r with OE(1) the restriction of the twisting sheaf ([F3]).

2.2F1F5step 1.1

Isomorphism criterion. If β is an isomorphism, then the pulled-back center ideal mpOY1 is invertible (The pulled-back center ideal is the relative twist; the exceptional divisor is Cartier), and since an isomorphism identifies ideal sheaves and their invertibility, mp itself is invertible; then m=mpA is generated by a nonzerodivisor, so dim⁡κm/m2=1=dim⁡A and A is regular by the definition of regularity (embedding dimension and regular local ring). Conversely, if A is regular, then A is a discrete valuation ring by [F5] and mp is generated by a uniformizer, which is a nonzerodivisor and generates the maximal ideal at p while mp is the unit ideal away from p; so mp is invertible and the blowup of an invertible ideal is an isomorphism (Blowing up an effective Cartier divisor does nothing), with β∗OY1=OY. This proves the equivalence and the final clause.

3.1F1F2step 2.1algebra

By [F2], χ(n) agrees eventually with a polynomial an+b of degree one. Since χ(n) is nonnegative for every n and a≠0, its leading coefficient a is positive. For all sufficiently large n, the difference χ(n)−χ(n−1) equals a; this difference is ℓA(mn/mn+1)=dim⁡κ(p)Sn, because the quotient is annihilated by m. Thus the graded Hilbert function is eventually a positive constant c=a∈Z>0.

4.1F3step 2.1step 3.1algebra

Write P=κ(p)[x0,…,xr], S=P/I, and b=P+. The ideal sheaf IE is coherent: on each standard affine chart it is a finite ideal in a Noetherian ring (Coherent module sheaves). By [F3], Serre vanishing applied to this ideal sheaf makes the global sections of 0→IE(n)→OPr(n)→OE(n)→0 exact on the right for n≫0. The sections of the middle sheaf are Pn, and its kernel is (Isat)n: a homogeneous polynomial represents a section of the ideal sheaf exactly when its fractions on every standard chart lie in the chart ideals, the saturation criterion of Closed subschemes of projective space and saturated ideals. Thus H0(E,OE(n))=Pn/(Isat)n for large n. The polynomial ring P is Noetherian (If R is Noetherian then R[x1,…,xn] is Noetherian for every n∈N), so the graded module Isat/I has finitely many homogeneous generators. Each is annihilated by some power of b by the definition of saturation; one common power bN annihilates them all. If their degrees are at most D, then in degree n≥D+N every coefficient multiplying such a generator has degree at least N and lies in bN. Hence (Isat/I)n=0 for all such n. It follows that H0(E,OE(n))=Sn eventually. By step 3.1 its dimension is the positive constant c, so the Hilbert polynomial of OE is the nonzero constant c. Its degree equals dim⁡E by [F3], giving dim⁡E=0.

5.1F4step 1.1step 4.1

The space E is a closed subscheme of the Noetherian space Pκ(p)r, hence is Noetherian of dimension zero by step 4.1, so it has finitely many points and all its local rings are zero-dimensional; as a closed subscheme of projective space E is proper and of finite type over κ(p), so E is quasi-finite over κ(p) and therefore finite over κ(p) by [F4]. Combined with step 1.1, where the fibre over every q≠p is a single point, every fibre of β is finite with zero-dimensional local rings, so β is quasi-finite; as β is also proper by step 1.1, [F4] makes β finite. This proves the first part of the statement and the finiteness of the fibre over p.

6.1F6step 2.1step 5.1step 2.2∎

All assertions are proved: β has the displayed closed immersion into Proj⁡YSym⁡(Ip), is locally H-projective, proper, finite type, finite, quasi-finite with fibre Proj⁡(gr⁡mpOY,p) over p, an isomorphism over Y∖{p}, and an isomorphism exactly when OY,p is regular, and the fiber over p is finite by step 5.1.

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The finite normalization of a curve factors through the blowup of a closed point

Statement

Assume the Axiom of Choice (The Axiom of Choice). Let Y be an integral Noetherian scheme of dimension one and let ν:Yν→Y be a finite normalization: a finite birational morphism from a normal one-dimensional scheme (for a reduced curve of finite type over a field this exists and is finite by the normalization theory of curves Normalization of a reduced curve is finite). Let p∈Y be a closed point and let β:Y1=Bl⁡pY→Y be the blowup of Y in p (Blowup of a scheme along an ideal sheaf). Then β is finite, and ν factors uniquely through β: there is a unique Y-morphism ν1:Yν→Y1 with β∘ν1=ν. Consequently Yν is also the normalization of Y1, and the finite pushforward β∗OY1 is naturally a coherent OY-subalgebra of ν∗OYν. If OY,p is regular then β is an isomorphism and ν1 is the original normalization map under the identification Y1=Y.

Facts & Assumptions

[F1]

A normal one-dimensional local ring that is a domain is a discrete valuation ring: a one-dimensional Noetherian local integrally closed domain is a discrete valuation ring, and the local rings of a normal scheme are normal domains (Equivalent characterizations of a DVR, serre normality criterion two directions, normal noetherian ring).

[F2]

Finiteness: the blowup β is finite and restricts to an isomorphism over Y∖{p} (The blowup of a one-dimensional integral Noetherian scheme at a closed point is finite); a finite morphism is affine, and its pushforward of the structure sheaf is coherent over the Noetherian base (Finite morphisms of schemes, Coherent module sheaves, Coherent sheaves on a locally Noetherian scheme).

[F3]

Universal property: for a closed subscheme Z=V(I)⊆X, every X-scheme f:W→X whose inverse image of Z is an effective Cartier divisor admits a unique X-morphism W→Bl⁡IX (Universal property of the blowup); an invertible ideal sheaf with nonzerodivisor generators cuts out an effective Cartier divisor (Effective cartier divisor).

[F4]

The blowup of an integral scheme in a nonzero ideal is integral (Blowing up a nonzero ideal on an integral scheme is birational).

[F5]

The Axiom of Choice is assumed, inherited from the cited blowup, finiteness and integral-closure suppliers; the only selection is that of the given normalization ν (The Axiom of Choice).

Proof

Given: AC, an integral Noetherian one-dimensional scheme Y, a finite normalization ν:Yν→Y, a closed point p∈Y and the blowup β:Y1=Bl⁡pY→Y.

1.1F1F2

The blowup β is finite and is an isomorphism over Y∖{p} by [F2]; in particular β is affine and β∗OY1 is a coherent OY-module. The scheme Yν is normal of dimension one, so each of its local rings is a discrete valuation ring or a field by [F1].

2.1F1F2step 1.1algebra

The normalization is integral with the same function field as Y. At a point q above p, the map OY,p→OYν,q embeds both rings into that function field. The maximal ideal mp contains a nonzero element, whose image remains nonzero; its extended ideal is proper because the map of local rings is local. The point q is closed, since the fibre of the finite morphism ν is zero-dimensional, and its normal local ring is therefore a DVR by step 1.1. Every nonzero ideal in a DVR is generated by a nonzerodivisor, so mpOYν,q is principal and invertible. At points not over p the pullback center ideal is the unit ideal. This coherent ideal is thus locally invertible everywhere: local stalk generators extend to neighbourhoods, and the equality with the principal ideal holds after shrinking because its cokernel is coherent. Its inverse-image subscheme is an effective Cartier divisor.

3.1F3F4step 1.1step 2.1

By the universal property [F3] applied to the center {p}⊆Y and the morphism ν:Yν→Y (whose inverse image of p is effective Cartier by step 2.1), there is a unique Y-morphism ν1:Yν→Y1 with β∘ν1=ν. This morphism is dominant: ν is surjective and β is an isomorphism over Y∖{p}, so ν1(Yν)⊇β−1(Y∖{p}), a nonempty open subset of the irreducible scheme Y1 by [F4] and therefore dense.

4.1F2step 3.1

The morphism ν1 is finite: over an affine open U=Spec⁡R⊆Y, write Y1∣U=Spec⁡B and Yν∣U=Spec⁡C with R→B and R→C module-finite by [F2]; the factorization gives a ring map B→C, and since C is a finitely generated R-module with R⊆B acting through B→C, the ring C is a finitely generated B-module; hence ν1 is affine with module-finite coordinate algebras, i.e. finite (Finite morphisms of schemes).

4.2F2step 3.1

Finally, if OY,p is regular, then β is an isomorphism by [F2], and under the identification Y1=Y the unique factorization ν1 of ν through the identity is ν itself, by uniqueness in step 3.1; the two displayed clauses about the regular case follow.

5.1F4step 1.1step 3.1step 4.1

The morphism ν1 is birational: ν is an isomorphism over a dense open V⊆Y (birationality), and β is an isomorphism over Y∖{p} by [F2]; hence ν1 is an isomorphism over the dense open β−1(V∖{p}) of Y1 (here V∖{p} is nonempty open in the one-dimensional irreducible scheme Y, hence dense). Since Y1 is integral by [F4] and Yν is normal, ν1 is a finite birational morphism from a normal scheme onto the integral scheme Y1. The affine coordinate ring C of the source is the integral closure of the coordinate ring B of Y1 in their common function field: C is integral over B by finiteness, while every element integral over B is also integral over C and therefore belongs to the integrally closed ring C. Thus ν1 is the normalization of Y1.

6.1F2F4step 4.1step 5.1

On an affine chart V=Spec⁡B of the integral scheme Y1, the inverse image under the finite birational normalization map is Spec⁡C. The map B→C is injective: localizing it at the generic point is the identified inclusion of the common function field, so any element in its kernel is zero in Frac⁡(B) and hence zero in the domain B. Thus OY1↪ν1,∗OYν. Applying the left exact pushforward along β gives β∗OY1↪ν∗OYν. Coherence follows from finiteness over the Noetherian base, establishing the claimed coherent subalgebra.

7.1F5step 1.1step 4.1step 5.1step 6.1step 4.2∎

Steps 1.1-6.1 and 4.2 prove: β is finite; ν factors uniquely as β∘ν1 with ν1:Yν→Y1; Yν is a normalization of Y1; and β∗OY1 is a coherent OY-subalgebra of ν∗OYν, with the regular case giving β=id⁡Y and ν1=ν under Y1=Y.

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Blowing up a non-regular point strictly increases the finite normalization subalgebra

Statement

Assume the Axiom of Choice (The Axiom of Choice). Let Y be an integral Noetherian scheme of dimension one with finite normalization ν:Yν→Y, let p∈Y be a closed point that is not a regular point of Y, let β:Y1=Bl⁡pY→Y be the blowup of Y in p, and let ν1:Yν→Y1 be the factorization of ν through β (The finite normalization of a curve factors through the blowup of a closed point). Then the natural inclusion of coherent OY-subalgebras OY⊆β∗OY1 inside ν∗OYν is strict: β∗OY1 strictly contains OY, and the quotient β∗OY1/OY is a nonzero coherent sheaf of finite length supported exactly at p.

More generally, if Yi→Yi−1 is a blowup at a closed non-regular point and fi:Yi→Y denotes the composite, then fi,∗OYi strictly contains fi−1,∗OYi−1 inside ν∗OYν for every i≥1.

Facts & Assumptions

[F1]

The blowup β is finite, ν factors uniquely through it, and β∗OY1 is a coherent OY-subalgebra of ν∗OYν; β is an isomorphism over Y∖{p} (The finite normalization of a curve factors through the blowup of a closed point, The blowup of a one-dimensional integral Noetherian scheme at a closed point is finite).

[F2]

β is an isomorphism if and only if OY,p is regular; equivalently, if and only if the maximal ideal mp is invertible (The blowup of a one-dimensional integral Noetherian scheme at a closed point is finite, Blowing up an effective Cartier divisor does nothing, one dimensional regular local rings are dvrs).

[F3]

On a locally Noetherian scheme the cokernel of a morphism of coherent modules is coherent, and a coherent module whose support is a single closed point y has a stalk of finite length at y: the stalk is a finitely generated module over the Noetherian local ring OY,y annihilated by an my-primary ideal, and a zero-dimensional Noetherian ring is Artinian of finite length (Coherent module sheaves, Coherent sheaves on a locally Noetherian scheme, Locally Noetherian and Noetherian schemes, A Noetherian ring is Artinian exactly when every prime ideal is maximal, A commutative ring is Artinian exactly when it has finite length as a module over itself, Composition series and length of a module).

[F4]

A finite morphism is affine; for an affine morphism and a short exact sequence of quasi-coherent modules over the source, the pushforward sequence is again short exact, because on affine charts the pushforward is given by the same ring extension and localization is exact (Finite morphisms of schemes, Localisation of modules is exact).

[F5]

The Axiom of Choice is assumed, inherited from the cited blowup, normalization and length suppliers (The Axiom of Choice).

Proof

Given: AC, an integral Noetherian one-dimensional scheme Y with finite normalization ν:Yν→Y, a closed non-regular point p∈Y, and the blowup β:Y1=Bl⁡pY→Y with factorization ν1:Yν→Y1.

1.1F1F2algebra

By [F1] the inclusion OY⊆β∗OY1⊆ν∗OYν holds as OY-algebras, and β∗OY1 is coherent. If the first inclusion were an equality, then the finite morphism β would satisfy β∗OY1=OY; on an affine chart U=Spec⁡R⊆Y with β−1(U)=Spec⁡B this says that the image of the structure map R→B generates B as an R-module, so B=R and β∣β−1(U) is an isomorphism; hence β would be an isomorphism. But p is not a regular point, so β is not an isomorphism by [F2]. Therefore OY⊊β∗OY1: the inclusion is strict.

2.1F1F3step 1.1

The quotient Q=β∗OY1/OY is coherent by [F3] and is nonzero by step 1.1. Away from p the morphism β is an isomorphism, so (β∗OY1)q=OY,q for every q≠p, and the stalk Qq=0 there; hence the support of Q is contained in the closed point p, and therefore equals {p}. By [F3] the stalk Qp has finite length over OY,p.

3.1step 1.1step 2.1

This proves the first assertion. For the general step, argue by induction on i. At each stage Yi−1 is an integral Noetherian one-dimensional scheme with a fixed finite normalization νi−1:Yν→Yi−1: for i−1=0 this is ν; inductively, Yi is the blowup of the integral scheme Yi−1 in a nonzero ideal, hence is integral (Blowing up a nonzero ideal on an integral scheme is birational) and Noetherian, and The finite normalization of a curve factors through the blowup of a closed point shows that Yν is a normalization of Yi as well. Let βi:Yi=Bl⁡pi−1Yi−1→Yi−1 be the blowup at a closed non-regular point pi−1, so that by the already proved first assertion applied to Yi−1 and pi−1 the sequence of OYi−1-modules 0→OYi−1→(βi)∗OYi→Qi→0 is exact with Qi≠0.

4.1F1F4step 3.1algebra

Push the short exact sequence of step 3.1 forward along the finite affine morphism fi−1. By [F4] this gives 0→fi−1,∗OYi−1→fi,∗OYi→fi−1,∗Qi→0. This last sheaf is nonzero: choose an affine open V=Spec⁡R of Y containing the image of the center. Its inverse image is affine, say Spec⁡B, and Qi restricts there to a nonzero finite B-module M, because its nonzero center stalk lies on that open. The pushforward restricts to the same nonzero module M viewed as an R-module. Restriction of scalars is faithful, so fi−1,∗Qi≠0. Consequently the pushed-forward inclusion is strict. Both terms embed as coherent subalgebras in ν∗OYν by the normalization factorization at each stage. No assertion that Qi is a sheaf on the reduced residue-field point is needed: its stalk may have nontrivial nilpotent maximal-ideal action.

5.1F5step 1.1step 2.1step 4.1∎

Collecting: the inclusion OY⊊β∗OY1 is strict with quotient a nonzero coherent sheaf of finite length supported exactly at p, and every further point blowup at a closed non-regular center strictly increases the pushed-forward structure sheaf inside the fixed finite normalization ν∗OYν.

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Regularization of a one-dimensional integral curve with finite normalization by point blowups

Statement

Assume the Axiom of Choice (The Axiom of Choice). Let Y be an integral Noetherian scheme of dimension one whose normalization ν:Yν→Y is finite. Then there exists a finite sequence Yn⟶Yn−1⟶⋯⟶Y1⟶Y of blowups in closed points such that Yn is regular. Moreover the sequence may be chosen with every center a non-regular closed point of the preceding curve; then no blowup is an isomorphism, and the increasing sequence of coherent OY-subalgebras OY⊆f1,∗OY1⊆f2,∗OY2⊆⋯⊆ν∗OYν (with fi:Yi→Y the composite) strictly increases at every step, so that termination is exactly Noetherian stabilization of this sequence.

No claim is made about normalizations that are not finite, and no higher-dimensional resolution of singularities is asserted. If Y is already regular the sequence may be taken empty (n=0).

Facts & Assumptions

[F1]

Step data for a point blowup of Yi−1: the blowup βi:Yi=Bl⁡pi−1Yi−1→Yi−1 in a closed point is finite, is an isomorphism if and only if OYi−1,pi−1 is regular, and the finite normalization of Yi−1 factors uniquely through it, so that Yν is a normalization of Yi and (βi)∗OYi lies between OYi−1 and νi−1,∗OYν (The blowup of a one-dimensional integral Noetherian scheme at a closed point is finite, The finite normalization of a curve factors through the blowup of a closed point).

[F2]

If the center is non-regular, the inclusion OYi−1⊊(βi)∗OYi is strict with nonzero quotient of finite length supported at the center (Blowing up a non-regular point strictly increases the finite normalization subalgebra).

[F3]

Integrality and Noetherianity are preserved: the blowup of an integral scheme in a nonzero ideal of finite type is integral (Blowing up a nonzero ideal on an integral scheme is birational), and the source of a finite morphism onto a Noetherian scheme is Noetherian, its affine charts being finitely generated algebras over Noetherian rings (Finite morphisms of schemes, Every algebra of finite type over a Noetherian ring is a Noetherian ring). The finite birational map has injective integral maps on affine coordinate domains, so dimension is preserved on an affine cover (Injective integral extensions preserve Krull dimension, Dimension can be computed on an open cover).

[F4]

Stabilization: on the Noetherian scheme Y, every increasing sequence of coherent subsheaves of the coherent module ν∗OYν stabilizes (Increasing sequences of coherent subsheaves of a coherent module on a Noetherian scheme stabilize, Coherent module sheaves).

[F5]

A one-dimensional integral Noetherian scheme is regular if and only if all of its closed points are regular: a local ring at a non-closed point of a one-dimensional integral scheme is a field, hence regular (Integral schemes, Chain dimension and the empty-space convention, embedding dimension and regular local ring).

[F6]

The Axiom of Choice is assumed for the choice of one non-regular closed point at each stage and for the cited suppliers (The Axiom of Choice).

Proof

Given: AC, an integral Noetherian one-dimensional scheme Y with finite normalization ν:Yν→Y.

1.1F1F5given

(Base of the recursion) Put Y0=Y and f0=id⁡Y; then Y0 is integral, Noetherian and one-dimensional, ν:Yν→Y0 is a finite normalization and f0 is finite. We construct, as long as the current curve is not regular, a point blowup at a non-regular closed point and keep the data of [F1].

2.1F1F2F3F5step 1.1

(Existence of a suitable center) Suppose Yi−1 is not regular. By [F5] some closed point pi−1∈Yi−1 is not regular; choose it and let βi:Yi=Bl⁡pi−1Yi−1→Yi−1 be the blowup, with fi=fi−1∘βi. By [F1] the morphism βi is finite, is not an isomorphism (the center is non-regular), and Yν is a normalization of Yi; by [F3] the scheme Yi is integral, Noetherian and one-dimensional, and fi is finite. By [F2] the inclusion fi−1,∗OYi−1⊊fi,∗OYi is strict, both terms being coherent OY-subalgebras of ν∗OYν.

3.1F2F4step 2.1

(Termination) Suppose, for contradiction, that Yi−1 is non-regular for every i≥1. Then step 2.1 can be iterated for all i, and it produces the infinite strictly increasing sequence OY⊊f1,∗OY1⊊f2,∗OY2⊊⋯⊆ν∗OYν of coherent OY-submodules of the coherent module ν∗OYν over the Noetherian scheme Y. This contradicts stabilization [F4]. Hence there is an integer n≥0 with Yn regular.

4.1F6step 2.1step 3.1∎

(Conclusion) The finite sequence Yn→Yn−1→⋯→Y1→Y consists of blowups in closed points, each center non-regular in the preceding curve, and ends at the regular curve Yn; no morphism in it is an isomorphism by [F1], and the associated sequence of coherent subalgebras strictly increases at every step by [F2]. Conversely, stabilization of this sequence is precisely what forces the termination: a stabilized non-regular stage would admit one further strict increase, contradicting stabilization. This proves all assertions, including the empty sequence when Y is already regular. No assertion is made for non-finite normalizations or in dimension greater than one.

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Regularization of an integral curve on an arbitrary Noetherian ambient scheme

Statement

Assume the Axiom of Choice (The Axiom of Choice). Let X be a Noetherian scheme and let Y⊆X be an integral closed subscheme of dimension one whose normalization is finite. Then there exists a finite sequence Xn⟶Xn−1⟶⋯⟶X1⟶X of blowups in closed points such that the strict transform of Y in Xn is a regular curve. If the closed points blown up in X are chosen to be the images of the corresponding centers of the intrinsic sequence for Y, the strict transform of Y in Xi is canonically the i-th intrinsic blowup of Y.

Facts & Assumptions

[F1]

The intrinsic regularization theorem: since Y is integral, Noetherian, one-dimensional and has finite normalization, there are a finite sequence Yn→Yn−1→⋯→Y1→Y of blowups at non-regular closed points and a factorization of the normalization through every stage, and Yn is regular (Regularization of a one-dimensional integral curve with finite normalization by point blowups).

[F2]

Strict transform under a blowup: if Z⊆X is a closed subscheme and π:Bl⁡IX→X is a blowup, the strict transform of Z is canonically the blowup of Z in the inverse image ideal of I; on charts it is cut out by the saturation of the pullback ideal. The construction may be iterated on the strict transform along a further blowup (Strict transforms of closed subschemes are blowups of the subscheme, Strict transform of a closed subscheme).

[F3]

The blowup of a Noetherian scheme in a closed point is Noetherian: choose a finite affine open cover of the base by spectra of Noetherian rings (Locally Noetherian and Noetherian schemes). The center ideal has finitely many generators on each chart, giving a finite standard affine chart cover of its blowup. Those chart rings are finitely generated algebras over Noetherian rings, hence Noetherian. The resulting finite affine cover makes the whole blowup Noetherian (Affine blowup standard charts and overlaps, Every algebra of finite type over a Noetherian ring is a Noetherian ring, Blowup of a scheme along an ideal sheaf).

[F4]

A closed point of a closed subscheme is a closed point of the ambient scheme, and the strict transform of an integral curve at each stage is an integral closed subscheme of the ambient scheme, of dimension one (Integral schemes, Strict transform of a closed subscheme).

[F5]

The Axiom of Choice is assumed, inherited from the intrinsic sequence and the blowup suppliers (The Axiom of Choice).

Proof

Given: AC, a Noetherian scheme X, an integral closed one-dimensional subscheme Y⊆X with finite normalization, and the intrinsic blowup sequence of [F1].

1.1F1

Apply [F1] to Y: this gives a finite sequence of closed points y0∈Y0=Y, y1∈Y1,…,yn−1∈Yn−1 with Yi=Bl⁡yi−1Yi−1, each yi−1 non-regular in Yi−1, and Yn regular. Since Yi−1 is integral of dimension one, each yi−1 is a closed point of Yi−1 (Integral schemes).

2.1F3F4step 1.1

Define the ambient sequence by X0=X and, inductively, Xi=Bl⁡zi−1Xi−1, where zi−1 is the image of yi−1 under the closed immersion Yi−1↪Xi−1 whose construction is the induction claim proved below. Each zi−1 is a closed point of Xi−1 by [F4], and each Xi is Noetherian by [F3].

3.1F2step 1.1step 2.1

Claim: for every i the strict transform of Y in Xi is canonically isomorphic over Y to Yi; in particular Yi embeds in Xi as a closed subscheme, so the induction of step 2.1 is legitimate. For i=0 this is the identity Y0=Y. Assume it for i−1. The blowup Xi→Xi−1 is the blowup at the point zi−1∈Yi−1⊆Xi−1; by [F2] the strict transform of Yi−1 in Xi is the blowup of Yi−1 in the inverse image ideal of zi−1, which is the maximal ideal of the point yi−1, and this blowup is Bl⁡yi−1Yi−1=Yi. Since strict transforms may be iterated (the strict transform of Y in Xi equals the strict transform of the strict transform Yi−1 of Y in Xi−1, by the saturation description of [F2]), the strict transform of Y in Xi is Yi.

4.1F5step 1.1step 3.1∎

Taking i=n, the strict transform of Y in Xn is canonically Yn, which is regular by step 1.1; hence the finite sequence of blowups in closed points constructed in step 2.1 has the required property, and by construction its centers are the images of the intrinsic centers, so the canonical identification of strict transforms with the intrinsic blowups holds at every stage. This proves both assertions.

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Separation of finitely many curve components by point blowups

Statement

Assume the Axiom of Choice (The Axiom of Choice). Let X be a Noetherian scheme and let Y1,…,Yr⊆X be pairwise distinct integral closed subschemes of dimension one, each with finite normalization. Then there exists a finite sequence of blowups of X at closed points such that the strict transforms Yi′ in the final blowup are pairwise disjoint regular curves (Strict transform of a closed subscheme).

Facts & Assumptions

[F1]

Regularization in the ambient scheme: for an integral one-dimensional closed subscheme Y⊆X with finite normalization there is a finite sequence of blowups of X at closed points whose final strict transform of Y is a regular curve; the sequence may be taken to consist of blowups at the images of intrinsic centers (Regularization of an integral curve on an arbitrary Noetherian ambient scheme).

[F2]

Preservation of regularity: if Y is an integral curve and π:X′→X is the blowup at a closed point p with OY,p regular, then π restricts to an isomorphism from the strict transform of Y to Y; if p is not a point of Y, the strict transform is the pullback isomorphic to Y. In particular point blowups preserve regularity and integrality of an already-regular curve (A point blowup drops pairwise intersection multiplicity by at least one, Strict transforms of closed subschemes are blowups of the subscheme).

[F3]

Multiplicity drop and separation: let Y,Z be distinct integral curves in the ambient scheme, p∈Y∩Z a closed point with OY,p regular, and let π:X′→X be the blowup at p with strict transforms Y′,Z′. Then the unique point q of Y′ over p satisfies mq(Y′∩E)=1, every point of Y′∩Z′ over p has multiplicity strictly smaller than mp(Y∩Z), and if mp(Y∩Z)=1 then Y′ and Z′ are disjoint over p (A point blowup drops pairwise intersection multiplicity by at least one, Intersection multiplicity of closed subschemes at a point).

[F4]

Two distinct integral closed subschemes of dimension one in a Noetherian scheme meet in a finite set of closed points: a one-dimensional irreducible component of the intersection would be a closed irreducible curve contained in both, hence equal to each of them, contrary to distinctness; a Noetherian space of dimension zero is finite (Integral schemes, Locally Noetherian and Noetherian schemes, Chain dimension and the empty-space convention).

[F5]

The Axiom of Choice is assumed, used to choose finitely many non-regular or maximum-multiplicity centers at each of the finitely many stages (The Axiom of Choice).

Proof

Given: AC, a Noetherian scheme X and pairwise distinct integral one-dimensional closed subschemes Y1,…,Yr⊆X, each with finite normalization.

1.1F1F2given

Apply [F1] successively to the strict transforms of Y1,…,Yr. These applications remain legitimate: a blowup centered away from another component leaves it unchanged; at a center on that component, its strict transform is its intrinsic point blowup (Strict transforms of closed subschemes are blowups of the subscheme), which is finite and retains the same finite normalization (The blowup of a one-dimensional integral Noetherian scheme at a closed point is finite, The finite normalization of a curve factors through the blowup of a closed point). Thus every not-yet-regularized component still satisfies the finite-normalization hypothesis of [F1]. During each later sequence, every already regular component stays regular by [F2]. Since there are finitely many components and each intrinsic regularization is finite, after finitely many ambient point blowups all strict transforms are regular integral curves. Rename these curves and the current ambient scheme Y1,…,Yr and X.

2.1F3F4step 1.1

(The multiplicity maximum) By [F4] each intersection Yi∩Yj with i≠j is a finite set of closed points, so the set of numbers mp(Yi∩Yj), over all pairs and all intersection points, is finite. If it is empty, the Yi are already pairwise disjoint and we are done. Otherwise let n≥1 be its maximum.

3.1F2F3step 2.1

(Phase n≥2: lowering the maximum) Suppose n≥2 and let p1,…,ps be the finitely many points at which the maximum n is attained. Blow up these points one after another (each is a closed point of the current ambient scheme, and the strict transforms are updated). For each pair (i,j) meeting at a blown-up point pt, [F3] shows that every multiplicity of Yi′∩Yj′ over pt is strictly smaller than n; new intersections arise only with the exceptional curves of the blowups and have multiplicity 1; and the local data at points that are not blown up are unchanged. Hence after these finitely many blowups either no pairwise intersection remains, in which case the curves are already disjoint and the process stops, or the maximum of the remaining pairwise multiplicities is strictly smaller than n. All strict transforms remain regular integral curves by [F2], and their pairwise intersections remain finite. Repeating this phase at most n−1 times, always lowering the current maximum, the process either stops with pairwise disjoint curves or reaches the case in which the maximum is 1. Every phase consists of finitely many blowups, so the total number of blowups is finite.

3.2F2F3step 2.1

(Phase n=1: separating the components) Assume the maximum of all pairwise multiplicities is 1 and let p1,…,ps be the finitely many points lying in at least two of the curves. Blow up these points one after another. For each pair (i,j) meeting at a point pt with mpt(Yi∩Yj)=1, the final clause of [F3] shows that Yi′ and Yj′ are disjoint over pt; after the finitely many blowups of this phase, every pair of strict transforms meets over none of the points pt. Since intersections can only occur at the pt (the strict transforms agree with the original curves away from the blown-up points), the final strict transforms Yi′ are pairwise disjoint, and they remain regular curves by [F2].

4.1F5step 1.1step 3.1step 3.2∎

Combining steps 1.1, 3.1 and 3.2: first make all components regular, then lower the maximum pairwise multiplicity by finitely many point blowups until either no intersection remains or the maximum is 1; in the latter case separate the remaining multiplicity-1 contacts by finitely many further point blowups. The composite is a finite sequence of blowups of X at closed points whose final strict transforms are pairwise disjoint regular curves, which is the assertion.

TheoremStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Embedded strict-normal-crossings resolution of a reduced curve on a regular surface

Statement

Assume the Axiom of Choice (The Axiom of Choice). Let S be a regular surface: a Noetherian scheme of pure dimension two all of whose local rings are regular. Let Z⊆S be a reduced curve, i.e. a reduced closed subscheme of pure dimension one, and assume that every irreducible component of Z has finite normalization (this is automatic when Z is of finite type over a field, in particular for a reduced plane curve over a field, by the normalization-finiteness theorem for integral finite-type curves). Then there exists a finite sequence Sn⟶Sn−1⟶⋯⟶S1⟶S of blowups of S at closed points such that:

  1. every Si is a regular surface;
  2. the inverse image (total transform) Zn of Z in Sn is an effective Cartier divisor on Sn (Effective cartier divisor, Cartier divisor);
  3. the support of Zn is a strict normal crossings divisor on Sn in the sense of Strict normal crossings divisor on a regular surface: every irreducible component (strict transforms of components of Z together with the exceptional curves) is a regular curve, and at every closed point of the support either one component passes or exactly two components pass and meet transversally.

Exceptional curves are regular and meet the strict transforms only transversally, so no new singular one-dimensional components are created. The conclusion is SNC support with regular irreducible components; the support itself need not be regular at a crossing. No smoothness of the components over a non-perfect ground field, relative SNC structure over a base field, or resolution in dimension greater than two is asserted.

Facts & Assumptions

[F1]

A reduced curve on a regular surface is an effective Cartier divisor: at a point p the local ring OS,p is a regular local ring, hence a unique factorization domain, and the radical ideal of Z at p is the intersection of the finitely many distinct height-one primes through p, generated by the product of their prime generators; a local equation of a nonempty curve is thus a nonzerodivisor, and the empty case is the unit ideal (Regular local rings are unique factorization domains, Effective cartier divisor, Cartier divisor, Strict normal crossings divisor on a regular surface).

[F2]

Since S is Noetherian, Z has finitely many irreducible components Z1,…,Zr, each an integral closed subscheme of dimension one with finite normalization; the underlying space of Z is Noetherian (Locally Noetherian and Noetherian schemes, Integral schemes, Chain dimension and the empty-space convention).

[F3]

Point blowups of a regular surface stay regular surfaces, at centers of local dimension two their exceptional curves are regular curves (at local dimension one the blowup is the identity), and the blowup restricts to an isomorphism away from the center (Point blowups of regular surfaces stay regular, with rational exceptional curves at two-dimensional local rings).

[F4]

Multiplicity drop and separation: if Y is an integral curve and OY,p is regular at a closed point p lying on a second closed subscheme Z with ηY∉Z, then the strict transform Y′ meets the exceptional curve E of the blowup at p in exactly one point q with mq(Y′∩E)=1, every point of Y′∩Z′ over p has multiplicity strictly smaller than mp(Y∩Z), and if mp(Y∩Z)=1 then Y′ and Z′ are disjoint over p (A point blowup drops pairwise intersection multiplicity by at least one, Intersection multiplicity of closed subschemes at a point).

[F5]

Separation of components: for finitely many pairwise distinct integral one-dimensional closed subschemes with finite normalization there is a finite sequence of blowups at closed points whose strict transforms are pairwise disjoint regular curves (Separation of finitely many curve components by point blowups).

[F6]

The Axiom of Choice is assumed for the finitely many center choices at each stage and for the cited suppliers (The Axiom of Choice).

Proof

Given: AC, a Noetherian regular surface S of pure dimension two, and a reduced curve Z⊆S whose irreducible components have finite normalization.

1.1F1F2

By [F1] the curve Z is an effective Cartier divisor on S, with invertible ideal sheaf OS(−Z). By [F2] it has finitely many irreducible components Z1,…,Zr, each integral of dimension one with finite normalization; if r=0 there is nothing to prove, so assume r≥1.

2.1F3F4F5step 1.1

Apply [F5] to the original components: finitely many point blowups make their strict transforms pairwise disjoint regular curves. The centers supplied by that proof lie either at a singular point of one current integral curve or at an intersection of two distinct current curves. Each has ambient local dimension two. Indeed at a dimension-one point of a regular surface the ambient ring is a DVR; the defining prime of an integral curve through a closed point of that curve cannot be its maximal ideal, since the curve has local dimension one there, so the curve's local ring would equal the DVR and be regular. Nor can two distinct one-dimensional curves pass through such a point: their prime ideals would both be zero in this local domain, forcing the same irreducible component locally and hence globally. Thus every center in this sequence has dimension two. By [F3] every new exceptional divisor is a regular P1 over the center residue field. Later blowups preserve regularity of each already regular exceptional curve, because the induced point ideal on that curve is Cartier and [F4] identifies its strict transform with the curve. Consequently, at the end of this sequence all components of the total-transform support are regular, but their contacts need not yet have multiplicity one.

3.1F1F3step 2.1algebra

At every stage the inverse image of Z is effective Cartier. Locally its ideal is generated by the pullback of a nonzero local equation on a regular irreducible component of the surface. Each blowup chart embeds into the function field of that component (Affine blowup algebras: normal form, nonzerodivisors, reducedness, domains), so this pullback stays nonzero and is a nonzerodivisor in the regular local domain. Its ideal is thus the invertible ideal of an effective Cartier divisor (Total transform of a Cartier divisor). Its support consists of the strict transforms of the original components and precisely the exceptional curves whose centers lie on the preceding total-transform support; the sequence of step 2.1 has this property. These components are all regular by step 2.1. The same Cartier and regularity conclusions remain true during the further point blowups below.

4.1F2F3F4step 2.1step 3.1algebra

Let C1,…,Cs be the finitely many regular components of the current support. Every intersection of two distinct components is a finite set of closed points: it is a zero-dimensional closed subscheme of either Noetherian integral curve. The finite set of contact multiplicities therefore has a maximum M, unless the components are already disjoint. If M>1, blow up each of the finitely many points where this maximum occurs. These centers have local ambient dimension two by the intersection argument in step 2.1. For each pair through a center, [F4] strictly decreases its contact multiplicity at any remaining intersection above that center. Every strict transform stays regular, and its intersection with the new exceptional curve has multiplicity one by [F4]. Pairs away from the center are unchanged; pairs previously disjoint remain disjoint. Hence after this finite set of blowups every pairwise contact, including contacts with all new exceptional curves, has multiplicity less than M. Repeat; the positive integer maximum strictly decreases each time, so after finitely many blowups all pairwise contact multiplicities are one, or there are no contacts.

5.1F3F4step 4.1

Suppose there is a closed point p at which three or more components C1,…,Cs (s≥3) of the current support meet. By step 4.1 all pairwise multiplicities mp(Ci∩Cj) equal 1, and all components are regular curves, so [F4] applies to each pair: blowing up p makes the strict transforms Ci′ pairwise disjoint over p and makes each Ci′ meet the new exceptional curve E at its own point qi with mqi(Ci′∩E)=1. Consequently every point of the new support lying over p carries at most two components (one strict transform together with E, or E alone), all components remain regular curves by [F3] and [F4], all pairwise multiplicities remain at most one by step 4.1, and no new point at which three components meet is created. Blowing up all points at which at least three components meet therefore strictly decreases their finite number, and iterating this finitely many times reaches a configuration in which at every closed point at most two components meet, and the pairwise contacts that exist have multiplicity one.

6.1F6step 2.1step 3.1step 5.1∎

In the terminal configuration the total transform Zn of Z is an effective Cartier divisor by step 3.1; its support has only regular irreducible components by steps 2.1 and 3.1; and at every closed point either no component passes, exactly one regular component passes, or exactly two regular components pass and meet transversally in the sense mp=1 of Strict normal crossings divisor on a regular surface. No three components meet, by step 5.1. Hence the support is a strict normal crossings divisor in the sense of the definition, which is assertion 3; assertions 1 and 2 are steps 2.1 and 3.1. Every center used was a closed point of a regular surface, so by [F3] no smoothness over a ground field was used or asserted: the ambient surfaces and individual components are regular, the support is SNC, and no higher-dimensional statement is made.

5 · Examples, counterexamples and false statements

None yet.

Sources