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The Artin-Mumford invariant

1.1 Classical birational invariants and functoriality

1.1.1 The Artin-Mumford invariant

Our last examples of classical birational invariants will need functoriality properties slightly different from what we used in Lemmas 1.1 and 1.3, namely functoriality under correspon-dences. Let X 7→ I(X) be an invariant of smooth projective varieties. Assume that any correspondence Γ X ×Y with dim Γ = dimX = dimY induces Γ : I(Y) I(X) and that this action is compatible with composition of correspondences. In particular a morphismϕ:X →Y between smooth projective varieties of the same dimensions induces ϕ : I(Y) I(X) and ϕ : I(X) I(Y). Assume also that the projection formula ϕ◦ϕ = (degϕ)Id: I(Y) →I(Y) holds. Assume the characteristic is 0 or resolution of singularities holds in the following sense: for any rational mapϕ:X 99KY, withY projec-tive, there exists a smooth varietyτ:Xe →X, obtained fromX by a sequence of blow-ups along smooth centers, such thatϕ◦τ gives a morphismXe →Y.

Lemma 1.9. Let X 7→ I(X) be an invariant of smooth projective varieties satisfying the functoriality properties above. Then I(X) is invariant under birational maps of smooth projective varieties if and only if it is invariant under blow-up.

Proof. Letϕ:X 99KY be a birational map. The graph Γϕ ⊂X×Y induces a morphism Γϕ:I(Y)→I(X). If

ϕ˜:Xe →Y, τ :Xe →X

is a resolution of indeterminacies of ϕ (or singularities of Γϕ), with τ a composition of blow-ups, one has

Γϕ=τ◦ϕ (1.3)

because Γϕ = (τ, IdY)(Γϕ˜) or equivalently Γϕ =tΓτΓϕ˜. Invariance of I under blow-ups guarantees thatτ:I(X)e →I(X) is an isomorphism. Butϕ is injective onI(Y) because ϕ◦ϕ=IdonI(Y). Hence by (1.3), Γϕis injective. In order to prove surjectivity, we now use resolution of singularities forϕ1. We thus have a diagram

ϕ˜1:Ye →X, τ:Ye →Y whereτ is a composition of blow-ups.

As before we have Γϕ= ˜ϕ1◦τ′∗, where nowτ′∗is an isomorphism by assumption while ϕ˜1is surjective by the projection formula ˜ϕ1( ˜ϕ1)=IdI(X). Thus Γϕis surjective.

Remark 1.10. The proposition above becomes a triviality if we use the weak factorization instead of resolutions of singularities.

Let us now introduce the Artin-Mumford invariant which was used in [3]. It will be generalized in the next section but the simplest version of it is the following: X is defined over the complex numbers and

I(X) = TorsHB3(X,Z), (1.4)

whereHBi(X, A) denotes Betti cohomology groupHi(Xan, A).

Proposition 1.11. The Artin-Mumford invariant is a stable birational invariant of smooth projective varieties.

Proof. As all the Betti cohomology groups with integral coefficients have functoriality under correspondences, the same holds for their torsion subgroups. Similarly for the projection formula. By Lemma 1.9, in order to show birational invariance of TorsHB3(X,Z), it thus suffices to show its invariance under blow-up. We now use the blow-up formula

HBi(X,e Z) =HBi(X,Z)⊕HBi2(Z,Z)⊕HBi4(Z,Z)⊕. . . ,

where τ : Xe X is the blow-up ofX along the smooth locus Z with exceptional divisor τE :E→Zand the first map isτwhile the other maps arej(es)◦τE, withe= [E]|E HB2(E,Z). The end of the proof follows from the observation that the blow-up formula remains true if we replace integral cohomology by its torsion and that TorsHB1(W,Z) = 0 for any topological spaceW. This last fact follows indeed from the cohomology long exact sequence associated with the short exact sequence of constant sheaves

0Zm ZZ/mZ0 onW. The blow-up formula then gives

TorsHB3(X,e Z) = TorsHB3(X,Z).

In order to get stable birational invariance, it remains to see invariance underX 7→X×Pr. This follows from K¨unneth formula which givesHB3(X×Pr,Z) = HB3(X,Z)⊕HB1(X,Z), hence

TorsHB3(X×Pr,Z) = TorsHB3(X,Z)TorsHB1(X,Z) = TorsHB3(X,Z).

Remark 1.12. The same proof shows as well that TorsHB2(X,Z) is also a birational in-variant. However, this invariant is trivial for rationally connected varieties, because they are simply connected by Theorem 1.2.

The Artin-Mumford invariant of X has an important interpretation as the topological part of the Brauer group ofX, which detects Brauer-Severi varieties onX. These varieties are fibered over X into projective spaces, but are not projective bundles P(E) for some vector bundle E on X. Given such a fibration π : Z X with fibers Zx isomorphic to Pr,Z =P(E) for some vector bundle of rankr+ 1 if and only if there exists a line bundle L on Z which restricts to O(1) on each fiber. The topological part of the obstruction to the existence of L is the obstruction to the existence of α HB2(Z,Z) which restricts to c1(OZx(1))∈HB2(Zx,Z). The relevant piece of the Leray spectral sequence ofπ gives the exact sequence

H2(Z,Z)→H0(X, R2πZ)d2 H3(X, R0πZ) =H3(X,Z),

where the second map is 0 with Q-coefficients by the degeneration at E2 of the Leray spectral sequence (or because there is a line bundle onZ whose restriction to the fibers is OZx(−r−1), namely the canonical bundleKZ). The imaged2(h) is thus a torsion class in H3(X,Z), called the Brauer class. The same argument shows that the order of the Brauer class dividesr+ 1.

The Artin-Mumford invariant was used by Artin and Mumford to exhibit unirational threefolds which are not stably rational. Let Sf P3 be a quartic surface defined by a degree 4 homogeneous polynomialf. LetXfP3be the double cover ofP3 ramified along Sf. It is defined as Spec (OP3 ⊕ OP3(2)) , where the algebra structure A ⊗ A → A on A=OP3⊕ OP3(2)) is natural on the summandsOP3⊗ OP3 andOP3⊗ OP3(2) and sends OP3(2)⊗ OP3(2) toOP3 via the composition

OP3(2)⊗ OP3(2)→ OP3(4)→ Of P3.

The local equation forXf ⊂Spec(l0OP3(2l)) is thus u2 =f, from which we conclude thatXf has ordinary quadratic singularities ifSf does. WhenSf is smooth,Xf has trivial Artin-Mumford invariant. This follows from Lefschetz theorem on hyperplane sections asXf

can be seen as a hypersurface (not ample but positive) in theP1-bundle Proj (Sym (OP3 OP3(2))) overP3. Assume now thatSf has ordinary quadratic singularities and letXef be the desingularization ofXf by blow-up of the nodes. Note that Xef is unirational. This is

true for all quartic double solids but becomes particularly easy onceSf has a node. Indeed, choose a nodeO∈Sf. The lines inP3 passing throughO intersect Sf in the pointO with multiplicity 2 and two other points. The inverse image of such a line ∆ inXf has a singular point at O (that we see now as a point ofXf), and its proper tranform C in Xef is the double cover of ∆=P1 ramified over the two remaining intersection points of ∆ andSf. It follows thatC is rational and we thus constructed a conic bundle structurea:Xef P2 onXef. On the other hand, if we choose a generic planeP in P3, its inverse image Σf,P in Xf is a del Pezzo surface, hence is rational, and viaa, it is a double cover ofP =P2. The double cover Xef ×P Σf,P of Xf is then rational, being rational over the function field of Σf,P since it is a conic bundle over Σf,P which has a section. We thus constructed a degree 2 unirational parametrization ofXf:

Xef×P Σf,P birat

= P399KXf.

Artin and Mumford constructf in such a way that Xf is nodal and Xef has a nontrivial Artin-Mumford invariant. Their construction is as follows: ProjectSf from one of its nodes O. Then this projection makes the blow-upSef ofSfatOa double cover ofP2ramified along a sextic curve. This sextic curveDis not arbitrary: it has to be tangent to a conic C⊂P2 at any of their intersection points. This conic indeed corresponds to the exceptional curve ofSef. Another way to see it is to write the equationf as X02q+X0t+s, whereq, t, sare homogeneous of respective degrees 2,3,4 in three variables X1, X2, X3. The ramification curve of the 2 : 1 map Sef P2 is defined by the discriminant of f seen as a quadratic polynomial inX0, that is,

g=t24qs. (1.5)

The conic C is defined by q = 0 and (1.5) shows that g|C is a square, and g is otherwise arbitrary. Artin and Mumford choosegto be a product of two degree 3 polynomials, each of which satisfies the tangency condition alongC. Note thatSf has then 9 extra nodes coming from the intersection of the two cubics.

Theorem 1.13. [3] If the ramification curve D is the union of two smooth cubics E, F meeting transversally and tangent toCat each of their intersection points, the desingularized quartic double solidXef has TorsHB3(Xef,Z)̸= 0.

Rather than giving the complete proof of this statement, we describe Beauville’s con-struction [10] of the Brauer-Severi variety Z Xef providing a Brauer class which is a 2-torsion class inHB3(Xef,Z) as described previously. The Artin-Mumford condition implies that the polynomialf is the discriminant of a (4,4)-symmetric matrix M whose entries are linear forms in four variables (the quartic surfaceSf is then called a quartic symmetroid).

This defines a family of quadric surfacesQoverP3if we seeM as an equation of type (2,1) onP31×P32, and the associated double cover ofP32parameterizes the choice of a ruling in the corresponding quadric QtP31. The family of lines in a given ruling on a given fiber is a curve ∆=P1 but the natural embedding of ∆ in G(2,4) gives ∆ as a conic. This way we get a family of rational curves overXef, smooth away from the surface Sf parameterizing singular quadrics. We refer to [10] and also to [37] for the local analysis which shows how to actually construct aP1-fibration on the whole ofXef.

The last, less classical, birational invariant that we will mention is defined as follows.

For a smooth complex varietyX, one has the cycle class map cl:Z2(X)→HB4(X,Z)

and we will denote byHB4(X,Z)alg⊂HB4(X,Z) the image ofcl. The groupHB4(X,Z)alg is contained in the group Hdg4(X,Z) of integral Hodge classes of degree 4 onX.

Lemma 1.14. The groupsTors (HB4(X,Z)/HB4(X,Z)alg)andHdg4(X,Z)/HB4(X,Z)alg are birational invariants of the smooth projective varietyX.

Proof. The two groups satisfy the functoriality conditions needed to apply Lemma 1.9, hence in order to show birational invariance, it suffices to show their invariance under blow-up.

However, for the blow-upXe→X ofZ⊂X, one has

HB4(X,e Z) =HB4(X,Z)⊕HB2(Z,Z)⊕HB0(Z,Z),

where the last term appears only if codimZ 3. In this decomposition, all the maps are natural and induced by algebraic correspondences. In particular this is a decomposition into a direct sum of Hodge structures. This decomposition thus induces

HB4(X,e Z)alg=HB4(X,Z)alg⊕HB2(Z,Z)alg⊕HB0(Z,Z)alg, and

Hdg4(X,e Z) = Hdg4(X,Z)Hdg2(Z,Z)Hdg0(Z,Z).

Using the facts thatHB2(Z,Z)/HB2(Z,Z)alghas no torsion and Hdg2(Z,Z) =HB2(Z,Z)alg, which both follow from the integral Hodge conjecture in degree 2 (or Lefschetz theorem on (1,1)-classes), we conclude that

Tors (HB4(X,e Z)/HB4(X,e Z)alg) = Tors (HB4(X,Z)/HB4(X,Z)alg), Hdg4(X,e Z)/HB4(X,e Z)alg= Hdg4(X,Z)/HB4(X,Z)alg, which proves the desired result.

The invariance of these groups underX 7→X×Pr is proved similarly.

Note that if the rational Hodge conjecture holds for degree 4 Hodge classes onX, these two groups are naturally isomorphic:

Lemma 1.15. For any smooth projective varietyX,

Tors (HB4(X,Z)/HB4(X,Z)alg)) = Tors (Hdg4(X,Z)/HB4(X,Z)alg).

AssumeXsatisfies the rational Hodge conjecture in degree4, the groupTors (HB4(X,Z)/HB4(X,Z)alg)) identifies with the group Hdg4(X,Z)/HB4(X,Z)alg which measures the defect of the Hodge

conjecture for integral Hodge classes of degree4 onX.

Proof. Indeed, a torsion element inHB4(X,Z)/HB4(X,Z)alg is given by a classαonX such that N α is algebraic on X. Then α is an integral Hodge class on X, which proves the first statement. Finally, the rational Hodge conjecture in degree 4 for X is equivalent to the fact that the group Hdg4(X,Z)/HB4(X,Z)alg is of torsion, which proves the second statement.