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LemmaStatement: AI-adaptedProof: AI-generatedPipeline-generatedprecheck passjudge pass (gpt-6-luna)verified 2026-11-04 (gpt-6.1-sol)
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Polygraph common ideal bases and freeness of every alternating-ideal power

Statement

Assume AC. For n≥1,l≥0 over C, let Wf⊂(A2)n×(A2)l be the graph ai=xf(i),bi=yf(i) of f:[l]→[n], and R(n,l)=C[x,y,a,b]/⋂f I(Wf). For 0≤r≤n,0≤k≤l and integer m, let I(m,r,k) be the ideal of the reduced union of V(xj:jinT)∩Wf over pairs with |T∩[r] minus f([k])∣≥m. Then R(n,l) has a homogeneous C[y1,…,yn]-basis with a subset spanning each I(m,r,k). In particular it is free over C[y]. If A is the space of Sn-alternating polynomials in C[x,y] and J=C[x,y]A, then every Jd, d≥0, is free over C[y]. No Hilbert-scheme Cohen–Macaulayness or n! theorem is a premise.

Facts & Assumptions

[A1]

AC and DC are retained where required by the actual coherent and projective suppliers. No external-theorem waiver is used.

Proof

Given: Exactly the objects and hypotheses in the Statement.

1.1givenA1F1algebra

Let B=C[y1,…,yn], E=A2, and let xj,yj (j∈[n]) and ai,bi (i∈[l]) be coordinates on En×El. Let f:[l]→[n] range over all functions.

2.1givenA1F1step 1.1algebra

Wf=V(ai−xf(i),bi−yf(i):iin[l]), R(n,l)=C[x,y,a,b]/⋂f I(Wf).

3.1givenA1F1step 2.1algebra

For 0≤r≤n, 0≤k≤l and integer m let Y(m,r,k) be the reduced union of V(xj:jinT)∩Wf over pairs (T,f) satisfying ∣T∩[r]∖f([k])∣≥m, and let I(m,r,k) be its ideal in R(n,l). The cases m≤0 give I=0 and m>r give I=R; also I(n,n,k)=R if k>0. Only finitely many nontrivial ideals are involved at each (n,l).

4.1givenA1F1step 3.1algebra

We construct an x-homogeneous B-basis of R(n,l) with a subset spanning every I(m,r,k). The construction is by induction on (n,l), with a secondary induction on x-degree. The x-degree counts x,a and the y-degree counts y,b. Each x-degree component is finite over B: the monic relations ∏j(ai−xj)=∏j(bi−yj)=0 make R finite over C[x,y]. Coordinate rings of all reduced arrangements used below embed in direct sums of their component polynomial rings, so they are torsion-free over B.

5.1givenA1F1step 4.1algebra

Let U1⊂Spec B be the distinct-y locus and U2 the locus with at most one equality among the yj. The complement of U2 has codimension at least two. At a point above U1 only one Wf occurs. At a point above U2∖U1, with the sole equal pair indexed N={p,q}, the local arrangement is a product of a polynomial affine space with R(N,L), where L consists of those i whose assigned y-value equals yp=yq. Indeed assignments outside this pair are fixed and eliminate their ai,bi, while assignments inside it are exactly the two choices p,q. This is an equality of local ideals, since the unwanted component ideals contain an invertible y-difference.

6.1givenA1F1step 5.1algebra

Here are the coefficient-extension principles used throughout. If a globally specified subset T of a torsion-free B-module is a basis after localization at every point of U2, it is a global B-basis. Expand an element at the generic point; its finitely many coefficients are the same in every localization and have no pole at any height-one prime. Polynomial unique factorization implies they lie in B. Torsion-freeness gives the resulting equality globally. Likewise two free submodules of one torsion-free module which coincide on U2 coincide globally. Finally, if T is a B-basis of M and T∩J spans J over C(y), it spans J over B, since the unique basis coefficients outside T∩J must vanish. Local equality of ideals at all points above Ui implies equality after B-localization at Ui, by testing all prime localizations of the latter module. The global elements in the first principle are essential: mere local freeness off codimension two does not imply freeness.

7.1givenA1F1step 6.1algebra

Over U1 the ring is a sum over f of C(y)[x]. In a coordinate-subspace union, standard square-free monomial ideals therefore show that the x-degree Hilbert function of its generic fiber counts pairs (e,f), einNn, with the corresponding monomial xe not killed on at least one component. For Y(m,r,k), this condition is

8.1givenA1F1step 7.1algebra

|[r] minus ({j:ej>0}∪f([k]))∣≥m.

9.1givenA1F1step 8.1algebra

For R(n,l) the generic Hilbert series is nl/(1−t)n. This counting statement follows by embedding into the component rings, localizing to separate their distinct y-values, and using ordinary monomial bases in each surviving coordinate-subspace union. In a fixed x-degree, homogeneous generators modulo (y) lift to generators by graded Nakayama; if their number equals this generic rank, they are a free basis, since a relation would vanish generically in a free source.

10.1givenA1F1step 9.1algebra

Take n=2 and l>0. Index basis candidates p[e,f] by e=(e1,e2)inN2 and f:[l]→{1,2}. For e=0 define

11.1givenA1F1step 10.1algebra

p[0,f]=∏j>1,f(j)≠f(1)(bj−b1) · (b1−y2iff(1)=1,else1).

12.1givenA1F1step 11.1algebra

For e=(0,h), h>0, split f−1(1)=S⊔T with S its first min(h,∣f−1(1)∣) indices, and define

13.1givenA1F1step 12.1algebra

p[(0,h),f]=x2h−∣S∣∏iinS(ai−x1−x2)∏jinT(bj−y2).

14.1givenA1F1step 13.1algebra

Let θ exchange x1,x2 and y1,y2, fix a,b, and compose f with the transposition. Set p[(h,0),f]=x1 θp[(0,h−1),θf]. If both ej>0, set p[e,f]=(x1x2)q p[e−(q,q),f], q=min(e1,e2).

15.1givenA1F1step 14.1algebra

These elements form a B-basis. To verify spanning, first reduce modulo y,x1x2. It is enough that the p[(0,h),f] span further modulo x1; multiplication by x1 and the transposition then cover the complementary summand. Vanishing on the Wf gives the relations ai2=aix2, aibi=bi2=x2bi=0, and ajbi=aibj for i<j in this quotient. Thus it is spanned by x2q∏iinSai∏jinTbj, where S,T are disjoint, every index in S precedes every index in T, and q=0 if T is nonempty. If S,T are both nonempty, choose h=∣S∣ and f−1(1)=S∪T; the displayed candidate reduces exactly to the monomial because all extra x2bj terms vanish. If T is empty, use h=q+∣S∣ and induct down from larger q, since expanding ∏(ai−x2) leaves the desired term and terms with larger x2 exponent. If S is empty, the h=0 candidates with f(1)=1 give all square-free b-monomials containing b1; those with f(1)=2 give the remaining square-free b-monomials modulo those already obtained. The constant is included. This proves spanning in every fixed degree; multiplying back by powers of x1x2 and the x1-transposed candidates proves spanning modulo (y). The degree enumerator of all candidates is 2l/(1−t)2, exactly the generic Hilbert series. The coefficient-count principle of the argument beginning at step 1.1 proves freeness and independence.

16.1givenA1F1step 15.1algebra

The candidates in I(m,r,k) are exactly the ones with

17.1givenA1F1step 16.1algebra

|[r] minus ({j:ej>0}∪f([k]))∣<m.

18.1givenA1F1step 17.1algebra

Here are explicit equations sufficient to check membership, including all nontrivial cases:

19.1givenA1F1step 18.1algebra

I(2,2,0)=(x1,x2,a1,…,al), I(1,2,k)=(x1x2,ai−x1−x2,bi−b1:i≤k), I(1,1,k)=(x1,ai−x2,bi−y2:i≤k).

20.1givenA1F1step 19.1algebra

For k=0 the empty sums are omitted. Each right-hand ideal vanishes on its defining arrangement. Substitution of the displayed products puts each selected p in the corresponding right-hand ideal. The one exceptional-looking product is x1(b1−y1) in I(1,2,k), k>0; the relation (a1−x2)(b1−y1)=0 makes it equal to −(a1−x1−x2)(b1−y1). All other factors either include x1x2, include a chosen ai−x1−x2 or bi−b1, or vanish after setting x1=0,ai=x2,bi=y2 for i≤k. This exhausts the three listed cases and the trivial ideals. The generic count from the argument beginning at step 1.1 gives exactly the complementary basis elements, so the selected elements span the entire ideal, not just a subideal. Thus the equations above and the common-basis assertion hold scheme-theoretically.

21.1givenA1F1step 20.1algebra

It follows that every sum/intersection in the lattice generated by these ideals and independent coordinate ideals is radical. Indeed the common basis makes every quotient by such a lattice ideal free over B; over C(y) the arrangement is a union of coordinate subspaces, hence reduced, and a torsion-free algebra embedding in its reduced generic fiber is reduced. After the U2 product reduction, the same radical assertion holds locally on U2 for the lattice generated by I(m,r,k) for arbitrary n. Sums and intersections remain computed by the corresponding subsets of the common basis in the two-coordinate factor and monomials in the other x variables.

22.1givenA1F1step 21.1algebra

Two additional local facts will be used. Setting any x or a coordinate to zero in a reduced union of Wf is reduced: simultaneous translation of all x,a coordinates by minus that coordinate defines a retraction of the quotient into the original reduced ring. For n=2 the ideal I(1,1,t−1)+(at) is radical as well. Eliminate the fixed pairs ai=x2,bi=y2 for i<t, reducing to (x1,a1). Its radical is the union of the f(1)=1 component with x1=0 and the f(1)=2 component with x1=x2=0. Modulo b1−y1 the ideal is already radical; its colon by b1−y1 is (x1,x2,a1,…,al,b1−y2). The inclusions follow from (b1−y1)(b1−y2)=0, (b1−y1)(a1−x2)=0, and the determinant with rows (ai,bi,1),(a1,b1,1),(x1,y1,1), which reduces to ai(b1−y1). Equality of this colon and its radical's colon, together with equality modulo b1−y1, gives equality with the radical by the modular law. The U2 product reduction gives the same local assertion for all n.

23.1givenA1F1step 22.1algebra

For a point of the polygraph, its admissible functions f form one equivalence class: f(i),g(i) are equivalent when their (x,y) pairs coincide there. The pointwise maximal f in that class maximizes |T∩[r]\f([k])| simultaneously for all m,r,k, where T is the set of zero x-coordinates. Consequently intersections of the Y(m,r,k) are reduced unions with the same f and both cardinality conditions imposed. This proves that their coordinate rings are B-torsion-free. It also proves all set-theoretic cardinality manipulations below without choosing incompatible assignments for two different conditions.

24.1givenA1F1step 23.1algebra

Use the cyclic shift θ(j)=j+1 mod n on x,y and fix a,b. Put Jt=I(1,1,t). If π forgets at,bt and k<t, then

25.1givenA1F1step 24.1algebra

Y(1,1,t)∪(Y(m,r,k)∩Y(1,1,t−1)) =Y(1,1,t)∪(π−1θY(m−1,r−1,k)∩Y(1,1,t−1));

26.1givenA1F1step 25.1algebra

if k≥t replace (m−1,r−1,k) on the right by (m,r−1,k−1). To prove this restrict outside Y(1,1,t). In Y(1,1,t−1), the maximal admissible f then has f(t)=1 and 1 absent from f([t−1]); otherwise a larger index with the same point would remove 1 from every f([t]) and put the point in Y(1,1,t). For k<t the removed index 1 contributes exactly one to the cardinality; for k≥t it is already in f([k]) and contributes zero. Removing that index and the t-th coordinate gives the asserted formulas. Adding back Y(1,1,t) gives the full unions.

27.1givenA1F1step 26.1algebraconstruct

For a finite one-variable algebra S=R[b]/J define, for m≥1, Em(S)={c∈R:cbm−1+∑i=0m−2cibi∈J for some ci∈R}, with the sum empty for m=1, and put E0(S)=0. Thus the coefficient is that of the specified term bm−1; multiplying a lower-degree relation by a power of b supplies its later-stage leading coefficient. We also write em(S)=Em(S). With Fm=R⟨1,…,bm−1⟩⊂S and F0=0, the cyclic map R→Fm/Fm−1 has exactly this kernel, so Fm/Fm−1=R/Em(S). The ideals increase, and a monic relation gives Fd=S and Em(S)=R for all m>d. Their zero sets are the loci where the fiber length is at least m. At a base prime P, a fiber algebra of vector-space dimension q=0 is the zero algebra; Nakayama then gives SP=0, so every Em(S)P=RP for m≥1. For q>0, over a residue field the finite one-variable quotient has basis 1,…,bq−1, where q is its dimension, and Nakayama makes Fq the whole localized algebra but Fq−1 a proper submodule. Hence Eq is proper there and Eq+1 is the unit ideal. Partial elimination commutes with flat scalar extension: intersect the relation module J with the finite-degree polynomial module, use flat exactness, and then take the image of the coefficient map. For a union defined by J1∩J2 the next inclusion follows.

28.1givenA1F1step 27.1algebra

Es(R[b]/J1) Et(R[b]/J2) ⊂ Es+t−1(R[b]/(J1∩J2)),

29.1givenA1F1step 28.1algebra

because multiplying two relations adds their leading degrees and multiplies their leading coefficients.

30.1givenA1F1step 29.1algebra

Suppose R has a common B-basis partitioned into disjoint sets Bj so that Em is spanned by the Bj with j<m, and suppose A is B-torsion-free. It is enough to know this elimination-ideal equality locally over U2. The filtration quotients then show that

31.1givenA1F1step 30.1algebra

⋃m≥1 Bm {1,b,…,bm−1}

32.1givenA1F1step 27.1step 30.1step 31.1algebra

Write S for the finite algebra called A in step 30.1, let em(S) denote its actual partial elimination ideal, and put Dm=B⟨⋃j<mBj⟩. Let Fm=R⟨1,b,…,bm−1⟩⊂S, with F0=0. For every base prime Q above which the y-tuple lies in U2, equality em(S)=Dm after localization at every prime of RQ implies equality as ideals of RQ: a nonzero quotient of the two ideals would have nonempty support and a prime localization detecting it. Therefore (Fm/Fm−1)Q≅(R/Dm)Q has basis bm−1⋃j≥mBj. Since b satisfies a monic relation, Fd=S for some finite d; these finitely many successive quotient bases lift to a basis of SQ. The union of their lifts is precisely the set in step 31.1. These are globally specified elements, not locally chosen frames. They are a basis at the generic point, and for every s∈S its finite generic expansion in them has coefficients regular at every height-one prime of B, because every such prime is in U2. Unique factorization gives coefficients in B; torsion-freeness of S makes this expansion an equality in S. Thus the displayed set is a global basis. To prove ideal compatibility, let I⊂R be spanned by a subset A⊂B and assume that the pullback to R of em(S/IS) equals I+em(S) locally over U1. Work at such a localization. The quotient-filtration identity gives Fm/(Fm−1+IS∩Fm)≅R/em(S/IS). On the other hand the modular law and the definition of em(S) give Fm/(Fm−1+bm−1I)≅R/(em(S)+I). Both isomorphisms are induced by the same cyclic generator bm−1, so their equal kernels imply Fm−1+IS∩Fm=Fm−1+bm−1I. Subtracting the indicated element of bm−1I⊂IS shows that multiplication by bm−1 gives the actual isomorphism I/(I∩em(S))≅(IS∩Fm)/(IS∩Fm−1). The subset bm−1⋃j≥m(A∩Bj) is its basis. Induction through the finite filtration therefore shows that A′=(A{1,b,b2,…})∩B′ spans IS generically. Every element of A′ already lies in IS, and B′ is now a global basis of S; expansion in that basis shows that every coefficient outside A′ vanishes. Hence A′ spans IS over B. This argument proves ideal compatibility without assuming in advance that S/IS is torsion-free or reduced.

33.1givenA1F1step 32.1algebra

For an increasingly ordered auxiliary label set L, the notation R(n,L) uses those labels and In,L(m,r,k′) counts its first k′ labels; after deleting a label the remaining labels are always ordered increasingly. For 1≤k≤l and 0≤r≤n let Z'(r,k) be the reduced union of V(ak)∩Wf over f with f(k)∈[r]\f([k−1]). It is finite over Z(n,L), L=[l]∖{k}, generated by the one remaining coordinate bk; ∏j(bk−yj)=0. Its partial elimination ideals satisfy

34.1givenA1F1step 33.1algebra

Em(Z′(r,k)) ⊂ In,L(m,r,k−1)

35.1givenA1F1step 34.1algebra

everywhere, with equality locally on U2. The inclusion follows from fiber counts on U1: above an assignment f the allowed points are precisely the indices j∈[r]\f([k−1]) with xj=0. Their count≥m defines the arrangement on the right, densely on each component, so leading coefficients vanish there.

36.1givenA1F1step 35.1algebra

For the reverse inclusion on U1, the defining ideal of the arrangement contains ∏jinT(xj,bk−yj), T=[r]∖f([k−1]). For 1≤m≤∣T∣+1, its leading coefficients include every square-free monomial of degree |T|+1−m in those xj, exactly the ideal of the locus with at least m zero coordinates. For m>∣T∣, the monic relation ∏jinT(bk−yj) makes Em the unit ideal, as required for the empty locus; this also covers T empty. At a U2 point split the indices into the unique pair N and its complement. The components with f(k) outside N give this same coordinate calculation; those with f(k) in N give the two-coordinate special arrangement. In that two-coordinate arrangement, E1 is the image ideal I(1,r,k−1); all Em for m>2 are the unit ideal; for r=1 or k>1, already Em=1 for m>1. The only remaining case is m=r=2,k=1, where I(2,2,0)=(x1,x2,ai:iinL). These generators are the b1-leading coefficients of

37.1givenA1F1step 36.1algebra

(b1−y2)x1, (b1−y1)x2, (b1−y1)ai+(bi−y2)x1.

38.1givenA1F1step 37.1algebra

They vanish on Z'(2,1), the last by the three-row determinant relation already used in the argument beginning at step 10.1. This proves the two-coordinate equality. In the product reduction, the product inclusion for elimination ideals gives the sum over s+t=m+1 of the tensor products of the outside-coordinate ideal for s and the pair ideal for t. The sum is radical by the common two-coordinate basis, and its zero set is the locus where the two counts add to at least m. It is therefore exactly I(m,r,k−1) locally. This verifies the required U2 scheme equality.

39.1givenA1F1step 23.1step 27.1step 32.1step 38.1algebra

Assume inductively that R=R(n,L) has its common basis, put S=O(Z′(r,k)), and set I=I(m′,r′,k′)⊂R. The arrangement embedding makes S torsion-free over B, and steps 34.1--38.1 give the partial elimination equality over U2, so the first part of step 32.1 produces a global basis of S. For its compatibility with IS, put Y′=Spec⁡(S/IS) and first establish the quotient partial-elimination equality without supposing IS radical. At a point of U1 the base has its unique component Wf; the distinct possible values bk=yj separate the special-arrangement branches, indexed by j∈[r]∖f([k−1]) with xj=0. If the base point also belongs to Y(m′,r′,k′), all these fiber points remain in the reduced preimage Yred′. Consequently its fiber has at least m points at every point of Y(m′,r′,k′)∩Y(m,r,k−1)∩U1. These intersections are scheme-theoretically reduced: on the unique component their defining ideals are sums of square-free coordinate-monomial ideals, and such a sum is again a square-free monomial ideal. The fiber-length criterion in step 27.1 therefore implies em(Yred′)⊂I+I(m,r,k−1) locally over U1. If J⊂R[bk] defines S, then J+IR[bk]⊂J+IR[bk], so the leading-coefficient definition gives em(Y′)⊂em(Yred′). Conversely I⊂em(Y′) for every m>0, since multiplying a constant relation by bkm−1 supplies its leading coefficient, and em(S)⊂em(Y′) because J⊂J+IR[bk]. Using em(S)=I(m,r,k−1) over U1 proves the exact scheme identity em(Y′)=I+em(S) there. The second part of step 32.1 now proves that the lifted subset with base coefficient in I spans IS. Thus S/IS is free over B. Its generic fiber is reduced: after inverting all y-differences, the branches are disjoint, and on the branch bk=yj the quotient adds xj=0 to a square-free coordinate-monomial ideal. A square-free monomial ideal remains radical after adding a coordinate variable. Finally S/IS injects into its generic fiber because it is free over the domain B; a nilpotent must have zero image and hence be zero. This proves that IS is globally radical and supplies its common basis, in that order.

40.1givenA1F1step 39.1algebra

For 1≤r≤n, put S=O(Z′(r,k)), S′′=O(Z′(r−1,k)), and K=ker⁡(S→S′′). For a base basis vector p define m(p) by p∈I(m(p)+1,r,k−1) and p∉I(m(p),r,k−1), and define m′(p) in the same way with r−1. The defining counts give the ideal inclusions I(a,r−1,k−1)⊂I(a+1,r,k−1)⊂I(a+1,r−1,k−1) and therefore m′(p)≤m(p)≤m′(p)+1. The compatible bases supplied by step 39.1 are B1={pbkj:0≤j<m(p)} for S and B1′={pbkj:0≤j<m′(p)} for S′′; regard the latter displayed polynomials also as their specified lifts in S. For each p with m(p)=m′(p)+1, the unique excess vector is p0=pbkm(p)−1. Express its image in S′′ uniquely as a B-linear combination p1 of B1′, and define qp=p0−p1∈K. Replacing every excess vector p0 by qp is a triangular change of basis, with diagonal entries one and correction terms only in the unchanged subset B1′. Hence {qp}∪B1′ is a basis of S. The quotient map sends qp to zero and sends B1′ isomorphically to its basis in S′′, so {qp} is a basis of K. To check simultaneous compatibility, fix I=I(m′,r′,k′) in the base. The basis of IS is A1={pbkj∈B1:p∈I} and that of IS′′ is the analogous subset A1′⊂B1′. If p∈I, then the image of p0 belongs to IS′′; uniqueness of its basis expansion forces p1 to use only A1′. Thus qp∈IS∩K. Rewriting the basis A1 by this same triangular replacement shows that IS has basis A1′∪{qp:p∈I}. Intersecting with the coordinate submodule K=B⟨qp⟩ gives exactly IS∩K=B⟨qp:p∈I⟩. The construction is simultaneous for all the base ideals and preserves homogeneity, since every unique expansion in a homogeneous quotient basis has the same total degree. No freeness of a general kernel of free modules is used.

41.1givenA1F1step 6.1step 40.1algebra

Write B=C[y1,…,yn] and K=C(y1,…,yn). Let R be a B-algebra, J,I1,…,Iq ideals, and suppose every R/Ii is B-torsion-free. Assume J has a B-basis D with subsets spanning every Ii∩J, and R/J has a B-basis C with subsets spanning every Ii+J/J. Suppose that for every intersection I of some of the Ii, I+J is radical locally over U2. Here, as in step 6.1, local reducedness means reducedness at every prime of R above the indicated coefficient point; consequently (I+J)BQ is radical for each coefficient prime Q∈U2, since a ring is reduced if all its prime localizations are reduced. This includes Q=(0), and U2 contains every height-one prime of B. Then R has a common B-basis for J and all Ii. The same assertion holds in each fixed homogeneous x-degree when B has x-degree zero and the given ideals and bases are homogeneous.

42.1givenA1F1step 6.1step 41.1algebraconstruct

Choose one lift c∈R of every vector of C. These lifts together with D are already a B-basis of R: projecting a putative relation to R/J kills its lift coefficients, and subtracting the lifted expansion of an arbitrary element leaves an element of J. For a lift c, let α={i:c‾∈Ii+J/J} and put I=⋂i∈αIi, with the empty intersection interpreted as R. The elementary identity I+J=⋂i∈αIi+J holds because the zero set of an intersection of ideals is the union of their zero sets. It puts c in I+J. At every Q∈U2, the local radical hypothesis therefore gives c∈IBQ+JBQ. Hence there is a correction uQ∈JBQ with c+uQ∈IBQ. The class of uQ in (J/(I∩J))BQ is unique: any two corrections differ by IBQ∩JBQ=(I∩J)BQ, since localization is exact. Intersections of the subset-spanned modules Ii∩J are spanned by the intersections of their subsets of D, so J/(I∩J) is free with basis the complementary subset Dc⊆D. Expand the unique correction class in that basis. The solution at every Q maps to the unique solution at Q=(0), so its finitely many nonzero coefficients are the same rational functions ad∈K, independent of Q, and belong to BQ for every Q∈U2. In particular they belong to every height-one localization of B. A reduced denominator with an irreducible factor would give a pole at that factor's height-one prime, so unique factorization implies ad∈B. Thus u=∑d∈Dcadd is a finite global sum in J and c∗=c+u is a globally defined element of R. Its generic class belongs to IK. For i∈α, torsion-freeness of R/Ii injects it into its generic localization; hence c∗∈Ii globally. The set B=D∪{c∗:c∈C} remains a B-basis because each c∗≡c(modJ). Fix i. At Q=(0) the local radical hypothesis gives (Ii+J)K=(Ii+J)K. The corrected lifts associated to the subset C∩(Ii+J/J) consequently span the image (Ii+J)K/JK, and the given subset D∩Ii spans (Ii∩J)K. The exact sequence 0→(Ii∩J)K→(Ii)K→(Ii+J)K/JK→0 shows that B∩Ii spans (Ii)K. Every element of Ii has its unique finite expansion in the global basis B; after passing to K, its coefficients outside this subset vanish, so they already vanish in B. Therefore B∩Ii spans Ii over B, simultaneously for every i. If a fixed x-degree is being constructed, choose homogeneous lifts and take the homogeneous component of every local correction in that degree. Since B has x-degree zero, the uniqueness and coefficient-extension argument use only basis vectors of that degree, and the corrected lifts remain homogeneous. This proves the claimed gluing assertion and its degreewise version.

43.1givenA1F1step 42.1algebra

First, R(n,l)/Jl is R([n]∖{1},[l])⊗C[y1], since on its components x1=0 and none of the f(i) equals 1. A common ideal basis for R(n−1,l), shifted by θ, is therefore a common basis here. The restriction of Y(m,r,k) for r>0 is Y(m−1,r−1,k) in the remaining indices, directly from the cardinality definition; r=0 gives only trivial ideals.

44.1givenA1F1step 6.1step 22.1step 39.1step 43.1algebraconstruct

For the second induction stage put Js=I(1,1,s), R=R(n,l)/Jt−1 and J=Jt/Jt−1, with 1≤t≤l. Assume the stipulated homogeneous common bases for R(n,l)/Jt and R(n,l−1). The colon identity Jt−1:(at)=Jt follows componentwise in the reduced arrangement: on a component of Y(1,1,t−1) one has x1=0 and 1∉f([t−1]), and at=xf(t) vanishes identically precisely when f(t)=1. Taking the colon removes just these components and leaves Y(1,1,t). Thus multiplication by at identifies (at)⊂R with R(n,l)/Jt, so (at) has a homogeneous free B-basis B1. We also have a homogeneous free basis B2 of R/(at): transpose the first and t-th auxiliary pairs, so at=0 becomes a1=0, and project away the first pair. The resulting arrangement is the reduced preimage of Yn,L(1,1,t−1) inside the special arrangement Z′(n,1), with L=[l]∖{1} increasingly ordered. Indeed the old first t−1 auxiliary indices become exactly the first t−1 labels of L, and their avoidance of the distinguished main index 1 is unchanged. The radical-extension and quotient-basis conclusions of step 39.1 therefore give B2. Choose global homogeneous lifts of B2 to R. By step 22.1, Jt−1+(at) is radical locally above U2; equivalently (at) and (at) have equal localizations there. Hence B1 together with those lifts is a basis of R after every B-localization in U2, by the exact sequence through (at). All the vectors are global elements and R is B-torsion-free, since it is a reduced arrangement ring. The coefficient-extension argument of step 6.1 now makes this a global homogeneous free B-basis of R. This establishes freeness of R before any assertion about the freeness of J.

45.1givenA1F1step 24.1step 40.1step 44.1algebraconstruct

Let L=[l]∖{t} in increasing order, Z′=Z′(n,t) and Z′′=Z′(n−1,t), and write K=I(Z′′)/I(Z′)⊂O(Z′). Separate the components of Z′ as Z′=Z′′∪Z1, where Z1 is the union with f(t)=n, n∉f([t−1]) and xn=0. There is no common component. The cyclic main-index shift θ gives Z0=θZ1, and Y(1,1,t−1)=Y(1,1,t)∪Z0, again with no common component: its new components have f(t)=1, 1∉f([t−1]) and x1=0. Denote the shifted ring O(θZ′) by S^ and the shifted ideal by K^=θK. Restriction to Z0 embeds both J and K^ into R0=O(Z0). For example a function of J vanishing also on Z0 vanishes on the reduced union Y(1,1,t)∪Z0 and is zero in R; the proof for K^ uses the other reduced union. This is injectivity of restriction, not freeness of an arbitrary kernel.

46.1givenA1F1step 45.1algebra

The needed equality is the equality of scheme-theoretic intersections, locally above U2, θZ′′∩Z0=Y(1,1,t)∩Z0, or equivalently I(θZ′′)+I(Z0)=Jt+I(Z0) in the localized ambient arrangement ring. Neither intersection is assumed reduced.

47.1givenA1F1step 5.1step 45.1step 46.1algebra

The equation is empty away from a two-y collision involving main index 1: a point of Z0 has an admissible assignment sending t to 1, while membership in either other arrangement requires an assignment sending t away from 1. When y1 differs from every other yj these cannot describe the same point. At the unique collision N={1,q}, discard the auxiliary pairs whose y-values are outside N; they have fixed assignments and give only an affine factor. If the t-th pair is outside this factor the intersection is again empty. Otherwise relabel N as {1,2}, keep the remaining auxiliary labels in increasing order, and let the old label t become s. In this two-coordinate ring the three arrangements have exactly the following ideals.

48.1givenA1F1step 19.1step 22.1step 47.1algebraconstruct

Put I0=(x1,as−x1,bs−y1, ai−x2,bi−y2 (i<s)), I∗=(x2,as−x2,bs−y2, ai−x1,bi−y1 (i<s)), J∗=(x1,as−x2,bs−y2, ai−x2,bi−y2 (i<s)). These are respectively the reduced ideals of Z0, θZ′′ and Y(1,1,s) in the local two-coordinate factor. For the first, eliminate the displayed fixed auxiliary pairs. Its quotient before imposing x1=0 is precisely the smaller polygraph ring with the first s labels omitted, because substitution and forgetting those pairs are inverse on all remaining generators. Imposing x1=0 gives its reduced quotient by the coordinate-translation retraction of step 22.1. This proves radicality and the asserted ideal, including the collision points. The second follows by exchanging the two main labels; the third is exactly the supplied two-coordinate equation I(1,1,s) from step 19.1. Thus no reduced ideal has been guessed from its points alone.

49.1givenA1F1step 46.1step 48.1algebra

Direct addition gives I0+I∗=I0+J∗=(x1,x2,y1−y2, ai,bi−y1 (i≤s)). For instance the two prescriptions for bs force y1=y2, the prescriptions for as together with x1 force x2=0, and the remaining fixed pairs then give exactly the displayed generators. These computations are in the actual quotient ring, so give equality even when the sums have nilpotents. Restoring the affine factors proves step 46.1 scheme-theoretically at every localization above U2.

50.1givenA1F1step 4.1step 6.1step 40.1step 44.1step 45.1step 49.1algebraconstruct

We now justify the two global freeness assertions needed to extend this equality. Step 40.1 makes K free with its common basis, so its semilinear shift K^ is free over B; the shift merely permutes the coefficient variables. To see J is free, fix an x-degree d. The modules Rd and (R/J)d are free by step 44.1 and the inductive hypothesis, and finite over B by step 4.1. The surjection Rd→(R/J)d splits since its target is free, so Jd is a finite projective B-module. It also retains its nonnegative y-grading. Choose a homogeneous complex-vector-space basis of Jd/(y)Jd and lift it homogeneously to Jd. These lifts generate by graded Nakayama: in each y-degree one subtracts the same-degree residue lifts and expresses the remainder using positive-degree y coefficients and lower degrees. There are finitely many lifts since Jd is finite. Their number equals the projective rank at (y) and therefore the generic rank, because the rank of a finite projective module is locally constant on the connected domain B. The resulting surjection from a finite free module of that rank has kernel of rank zero. That kernel is a submodule of a free module and is torsion-free, hence is zero. Thus the lifts are a homogeneous free basis of Jd; their union over all d is a free B-basis of J. This argument does not require the whole J to be finite over B. Restriction identifies J and K^ with free submodules of the same torsion-free module R0. Their images are the ideals (Jt+I(Z0))/I(Z0) and (I(θZ′′)+I(Z0))/I(Z0), which agree on U2 by step 49.1. Expanding each global basis vector of either image in the other's generic basis, its finitely many rational coefficients are regular at every height-one prime of B, since all those primes lie in U2. Unique factorization makes every coefficient polynomial. Torsion-freeness then makes the equality global in both directions. We have obtained the canonical degree-preserving isomorphism K^≅J by restriction through the common image in R0.

51.1givenA1F1step 21.1step 23.1step 25.1step 26.1step 39.1step 40.1step 41.1step 42.1step 50.1algebraconstruct

This isomorphism transfers the entire common-basis structure, not just module freeness. In S^ each extended ideal θIn,L(m′,r′,k′)S^ is radical by step 39.1. A function of K^ already vanishes on θZ′′, so its membership in that radical ideal is equivalent to vanishing on Z0∩π−1θYn,L(m′,r′,k′). For a function of J, the same criterion is membership in the reduced preimage ideal on Y(1,1,t−1), since it already vanishes on Y(1,1,t); the two coordinate projections agree on Z0. Thus the isomorphism carries the appropriate intersections with the extended ideals exactly, and the compatible basis furnished by step 40.1 gives corresponding subset bases in J. For a requested I(m,r,k) with r>0, put (m′,k′)=(m−1,k) for k<t, and (m′,k′)=(m,k−1) for k≥t, retaining r′=r−1. These are the first-k′ counts in the increasingly ordered set L: deleting t removes no counted label when k<t and removes exactly one when k≥t. The main-index shift sends the remaining indices 1,…,r−1 to 2,…,r. The cardinality identities of steps 25.1–26.1 therefore identify the union with Y(1,1,t) of the two reduced preimages. Taking its reduced ideal yields precisely J∩I(m,r,k)R on the original side. This proves the subset-basis compatibility for all these intersections; the r=0 cases are trivial. Finally apply the gluing lemma to Lm,r,k=I(m,r,k)R and J. Each R/Lm,r,k is a reduced arrangement ring and is B-torsion-free by step 23.1. The given quotient common basis is exactly a basis for the reduced images of these ideals in R/J. For any intersection L of a subcollection, the required local radicality of L+J follows from the supplied U2 sum/intersection-lattice calculation of step 21.1, with all radicals identified locally there. The free compatible basis of J was just constructed. Hence the gluing lemma supplies the homogeneous common ideal basis of R(n,l)/Jt−1.

52.1givenA1F1step 51.1algebra

Third, suppose R(n,l)/J0 has a common basis. Here J0=(x1) by the coordinate-translation retraction, and x1 is a nonzerodivisor because it vanishes identically on no Wf. For r>0, removing the components on which x1 vanishes gives

53.1givenA1F1step 52.1algebra

I(m,r,k)∩(x1)=x1 θI(m,r−1,k).

54.1givenA1F1step 53.1algebra

If a common basis in degree d is given, multiplying its shift θ by x1 gives a basis in degree d+1 for J0, compatible with these intersections. Apply the degreewise gluing lemma with the supplied quotient basis. In degree zero there is no J0 term, so start from the quotient basis and induct on d. This produces a common homogeneous basis for R(n,l).

55.1givenA1F1step 54.1algebra

For l=0, R(n,0)=C[x,y] and all relevant ideals are generated by square-free x-monomials, so the ordinary x-monomials are a common B-basis. For n=1, R(1,l)=C[x1,y1] and the only nontrivial condition is x1=0, already covered by that basis. Inducting on n+l, use the first stage from R(n−1,l), the second stage for t=l,l−1,…,1 using R(n,l−1), and the third stage. This proves the simultaneous ideal-basis theorem and hence freeness of every R(n,l) over C[y].

56.1givenA1F1step 55.1algebra∎

Let A be the alternating polynomials in C[x,y] under Sn and J=C[x,y]A. Every Jd is free over C[y]. Set l=nd and let (Sn)d permute d consecutive blocks of n coordinate pairs among (a,b), fixing (x,y). The sign-isotypic direct summand of R(n,nd) restricts isomorphically to Jd on the component f0(kn+i)=i. Surjectivity follows by alternating separately in each block: restrictions are exactly products of d alternating polynomials times arbitrary C[x,y] coefficients. For injectivity, a sign-alternating function vanishes on any component with a repeated assignment in a block, and every remaining component is moved to f0 by the block permutation group; hence its restriction to f0 determines it on the whole reduced union. Each fixed x-degree is a finite, nonnegatively y-graded free B-module; its sign summand is graded-projective, hence graded-free by the homogeneous basis-lifting argument already given. Their direct sum is free. This proves alternating-ideal power freeness without invoking the n! theorem.

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