This paper develops local versions of Voevodsky's motives over fields, simplifying the global category over flexible fields and introducing local invariants, with computations and conjectures relating local and numerical Chow motives.
Contribution
It introduces local motivic categories parameterized by finitely-generated extensions, and demonstrates their simplicity and relation to topological counterparts over flexible fields.
Findings
01
Computed local motivic cohomology of a point for p=2
02
Studied local Chow motivic category and introduced local Chow groups
03
Conjectured and proved cases where local Chow motives match numerical Chow motives
Abstract
In this article we introduce the local versions of the Voevodsky category of motives with Z/p-coefficients over a field k, parameterized by finitely-generated extensions of k. We introduce the, so-called, flexible fields, passage to which is conservative on motives. We demonstrate that, over flexible fields, the constructed local motivic categories are much simpler than the global one and more reminiscent of a topological counterpart. This provides handy "local" invariants from which one can read motivic information. We compute the local motivic cohomology of a point, for p=2, and study the local Chow motivic category. We introduce local Chow groups and conjecture that, over flexible fields, these should coincide with Chow groups modulo numerical equivalence with Z/p-coefficients, which implies that local Chow motives coincide with numerical Chow motives. We prove this Conjecture in…
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Full text
Isotropic motives
Alexander Vishik
Abstract
In this article we introduce the local versions of the Voevodsky category of motives with Fp-coefficients
over a field k, parameterized by finitely-generated
extensions of k. We introduce the, so-called, flexible fields, passage to which is conservative on motives.
We demonstrate that, over flexible fields, the constructed local motivic categories are much simpler than the global one
and more reminiscent of a topological counterpart. This provides handy ”local” invariants from which one can read
motivic information.
We compute the local motivic cohomology of a point, for p=2, and study the local Chow motivic category. We
introduce local Chow groups and conjecture
that, over flexible fields, these should coincide with Chow groups modulo numerical equivalence with
Fp-coefficients, which implies that local Chow motives coincide with
numerical Chow motives. We prove this Conjecture in various cases.
1 Introduction
The category of algebraic varieties is rich and marvelous, but not additive. In a sense that one can’t add morphisms between varieties.
The program to ”linearize” the algebro-geometric world was first introduced by A.Grothendieck in the 1960-ies, who proposed the
category of Chow motives. It is a close relative of the category of correspondences, where objects are smooth projective varieties
and morphisms are algebraic cycles on the product modulo rational equivalence. The result is a tensor additive category, as we can add
(and subtract) algebraic cycles and multiply them externally. Moreover, one doesn’t have to limit oneself to only rational equivalence
of cycles. Instead, it is possible to consider algebraic, numerical, or homological equivalence, and actually, the theory
of Chow groups here can be substituted by any oriented cohomology theory
(in the sense of [11, Def. 3.1.1] or [9, Def. 1.1.2]).
Chow motives of varieties split into smaller pieces which permit to express in a precise form some of the similarities observed
in the behavior of different varieties. In particular, the Tate-motives appear, responsible for the cellular structure.
The above Grothendieck’s category has innumerate remarkable applications, but it deals with smooth projective varieties only.
At the same time, in topology, motives were known already for a long time in full generality in the form of singular complexes of
topological spaces.
This problem was solved by V.Voevodsky in [19] who constructed the triangulated category of motives
DM(k) over a field k
(around the same time, alternative constructions were proposed by M.Hanamura and M.Levine). This category of Voevodsky contains the
Grothendieck’s category of Chow motives as a full additive subcategory closed under direct summands, and, in particular, permits to
study these ”pure” objects by triangulated methods.
Voevodsky supplied his category with many flexible tools and his motives found numerous bright applications, most notably, to
the proof of Milnor’s and Bloch-Kato Conjectures.
In this article, we study Voevodsky category DM(k;Fp) with finite coefficients over a field of characteristic zero.
We introduce the local versions DM(E/k;Fp) of this category, corresponding to all finitely generated
field extensions E/k together with the natural localization functors φE:DM(k;Fp)→DM(E/k;Fp).
In the case of a trivial extension we get the isotropic motivic categoriesDM(E/E;Fp) and localization
functors can be specialized further to isotropic functors ψE:DM(k;Fp)→DM(E/E;Fp).
Such isotropic versions (in the appropriate situation) appear to be much simpler than the original global category, and permit
to obtain ”local” invariants of motives, residing in a rather simple world.
The construction of isotropic motivic category is based on the notion of an anisotropic variety, that is, a variety which
doesn’t have closed point of degree prime to a given prime p (so, the fact that coefficients are finite is really essential).
The rough idea is to ”kill” the motives of all anisotropic varieties over k. This idea belongs to T.Bachmann, who in [1]
considered the full tensor triangulated subcategory DQMgm of DM(k;F2) generated by motives of smooth projective quadrics
and studied it with the help of functors ΦE:DQMgm→Kb(Tate(F2)) to the category of bi-graded F2-vector spaces.
These functors were defined by the property that they ”kill” the motives of k-Quadrics, which stay anisotropic over E
(and act ”identically” on Tate-motives). In our approach, the same idea comes naturally from the development of some ideas of Voevodsky
and that of [14]. Namely, we consider the natural ⊗-idempotents in Voevodsky category, given by
motives XQ of Čech simplicial schemes corresponding to smooth varieties Q over k. The respective
projectors naturally commute with each other and form a
partially ordered set P, where XQ⩾XP if there exists a correspondence of degree 1 (modulo p) Q⇝P
(Definition 2.1).
This condition is equivalent to the fact that
XQ⊗XP=XQ. That is, a stronger projector ”consumes” a weaker one.
Moreover, there is a natural map XQ→XP (the unique lifting of the projection XQ→T).
For connected varieties, this is, actually, a condition on their
generic points.
The ”smallest” idempotent is the unit object of the tensor
structure, given by the trivial Tate-motive T (it corresponds to P=Spec(k)). Thus, we get a P-parameterized filtration by
idempotents on the unit object. We may consider the upper graded components of this filtration. In other words, we
take a particular idempotent XP and mod out all strictly large ones, that is, we consider the colimit of idempotents
XP⊗XQ, for all XQ≩XP, where XQ is an idempotent complementary to XQ.
The result is a certain idempotent in DM(k;Fp), which actually can be described in terms of the Čech simplicial scheme of a
variety with infinitely many connected components. This idempotent will be zero, unless P is connected up to equivalence
(i.e., can be replaced by a connected variety with the same X), and, in the latter case, it depends only on E=k(P), and even
only on the equivalence class of such finitely generated field extension E/k.
Applying the respective projector to DM(k;Fp) we obtain the motivic categoryDM(E/k;Fp)
of the extension E/k - Definition 2.3.
It is naturally a full tensor localizing subcategory of the Voevodsky category DM(k;Fp) supplied with the
localization functorφE:DM(k;Fp)→DM(E/k;Fp).
In the case of a trivial extension k/k, we get the isotropic motivic categoryDM(k/k;Fp), where the respective projector
is the colimit of projectors XQ⊗, where Q runs over all varieties with XQ=T, or, in other words, over all
anisotropic varieties. Since XQ⊗M(Q)=0, such a projector ”kills” the motives of all anisotropic varieties.
These local motivic categories were discovered in an attempt to find an alternative approach to the functors of Bachmann
(mentioned above) and were briefly introduced in [18, Sect. 4].
Our next point is that to extract the local information in a meaningful form one should first pass to an appropriate field extension
of a ground field. This is illustrated by the example of an algebraically closed ground field k, where, up to equivalence, there is
only one (trivial) class of field extensions, represented by the extension k/k, and the respective localization functor
φ:DM(k;Fp)→DM(k/k;Fp) is an equivalence of categories - see Remark 2.12. Thus, it is conservative,
but not very interesting. At the same time, there is a large class of fields, for which the localization really simplifies things.
These are, the so-called, flexible fields introduced in Section 1.2. Fields, which are purely transcendental extensions
of infinite (transcendence) degree of some other fields. Note, that one can always pass from an arbitrary field k0 to a flexible one
k0(t1,t2,…) without loosing any motivic information. The class of flexible fields is closed under finitely generated extensions.
Thus, if the ground field k is flexible, then all the functors ψE:DM(k;Fp)→DM(E/E;Fp) take values in ”flexible”
isotropic categories. And such categories are really simple. We examine them from two points of view: we look at the
isotropic motivic cohomology of a point HM∗,∗′(k/k;Fp) and at the isotropic Chow motivic categoryChow(k/k;Fp).
We show in Theorem 3.7 that, in the case of a flexible field, HM∗,∗′(k/k;F2) is the external algebra ΛF2(r{i}∣i⩾0)
with the generators in one-to-one correspondence with Milnor’s operations and the
action of the latter given by Qi(r{i})=1 and Qi(r{j})=0, for i=j. Thus, the answer is the same for
all flexible fields, and all these cohomology elements are ”rigid”, as we can get 1 from any such non-zero element by applying
appropriate combination of Milnor’s operations. The answer is also remarkable in the sense that Milnor’s operations are encoded into
the structure of isotropic motivic category (in the form of their ”inverses” r{i}’s).
The computation is done with the help of Voevodsky technique used in the proof of Milnor’s conjecture, and our answer explains to some
extent why Milnor’s operations played such an important role in Voevodsky proof - see Theorem 3.5.
Finally, the answer is drastically different
from the ”global” one and the localization functor HM∗,∗′(k,F2)→HM∗,∗′(k/k;F2) is zero outside the bi-degree (0)[0].
We are restricted to the prime p=2, since in our calculations the crucial role is played by
[15, Cor. 3], and there is no analogue of this statement for p>2.
It appears that isotropic Chow motives are closely related to the numerical equivalence of cycles with Fp-coefficients.
We conjecture that, in the case of a flexible field, isotropic Chow groupsChk/k∗ (describing Homs between such motives)
coincide with the Chow groups (with Fp-coefficients) modulo numerical equivalence ChNum∗ - see Conjecture 4.7.
This would imply that the category of isotropic Chow motives is equivalent to the category of
Chow motives modulo numerical equivalence (with finite coefficients).
We prove this Conjecture for divisors, for varieties of dimension ⩽5, and for cycles of dimension ⩽2 -
Theorem 4.11. In particular, this implies that isotropic Chow groups are finite-dimensional in these
situations. This also shows that the projection Ch∗↠Chk/k∗ factors through the 3-rd theory of higher typeCh(3)∗ (where Ch(0)∗=Ch∗ is the original theory of rational type and Ch(1)∗=Chalg∗ is the
algebraic version) - see Definition 4.3 and Proposition 4.25.
The proof of Theorem 4.11 constitutes the bulk of this article. It is by induction on the dimension of a variety X.
Using the moving technique introduced in Section 6, we show that after an appropriate blow-up, any class u numerically equivalent
to zero may be represented by a cycle supported on a smooth connected divisor Z and numerically trivial already on Z. An important step
here is to represent u by the class of a smooth connected subvariety and numerically annihilate certain characteristic classes of it
cf. Corollaries 6.11, 6.12.
Interestingly, the latter is achieved by a combination of appropriate blow-ups and Steenrod operations, depending on a prime involved.
The paper is organized as follows. After briefly discussing flexible fields in Section 1.2, in Section 2
we introduce the local motivic category with Fp-coefficients as well as its Chow-motivic version. In Section 3
we study the isotropic motivic cohomology of a point, while Section 4 is devoted to the study of isotropic
Chow groups and the respective Chow-motivic category. In Section 5 we expand the definition of local motivic category
beyond prime coefficients. Finally, in Section 6 we prove various geometric results used in Section 4.
Acknowledgements: I’m very grateful to J.-L.Colliot-Thélène for useful discussions,
to C.Voisin for helpful comments and drawing my attention to [13, Theorem 5], and to J.I.Kylling, P.A.Østvær, O.Röndigs and
S.Yagunov for fruitful interaction during my visit to the University of Oslo which led to the inclusion of Section 5.
Also, I’m very grateful to T.Bachmann for the valuable remarks on the previous version of the paper.
Finally, I would like to thank the Referee for many useful suggestions which helped to improve the exposition.
1.1 Notations and conventions
Everywhere below k will denote a field of characteristic zero.
Smk - the category of smooth quasi-projective varieties over k.
Ch∗ - the Chow groups CH∗/p with finite coefficients, where p is some prime
(in Section 6, p will be replaced by an arbitrary natural number n).
DM(k;Fp) will denote the triangulated category of Voevodsky motives over a field - [19], [3] and
DMgm(k;Fp) will denote the full triangulated subcategory of geometric motives in it.
L - the Lazard ring, that is, the coefficient ring of the universal formal group law.
1.2 Flexible fields
Traditionally, algebraic geometry was considered over algebraically closed fields. Over such fields, every algebraic variety
(of finite type) has a rational point, which simplifies many things. In the case of a general field the standard approach is
to consider the passage to its algebraic closure. Note, however, that (torsion) information is lost under such a passage.
One of the aims of the current paper is to convince the reader that there are other directions one can pursue.
Namely, I propose to move instead in the direction of the, so-called, flexible fields. Such fields have the advantage that
one doesn’t have to distinguish between the ground field and finitely-generated purely transcendental extensions of it. This helps
with many algebro-geometric constructions.
Definition 1.1
Let us call a field k flexible if it is a purely transcendental extension of countable infinite degree of some other field:
k=k0(t1,t2,…)=k0(P∞).
Note, that any finitely generated extension of a flexible field k is itself flexible. Indeed, such an extension is defined by
finitely many generators and relations, which can ”spoil” only finitely many of the original transcendental generators.
Thus, all the points of the large Nisnevich site of Spec(k) are flexible.
On the other hand, we have:
Remark 1.2
The natural restriction functor DM(k0;Fp)→DM(k;Fp) is conservative. So, we can substitute a field by a flexible one
without loosing any motivic information.
*
△*
The main property of flexible fields we will need is the following obvious observation.
Proposition 1.3
Let k be a flexible field, X - variety of finite type over k, and E/k be a finitely-generated purely transcendental
field extension. Then there exists a commutative diagram
[TABLE]
with horizontal maps isomorphisms (over some subfield k0).
Proof:
Let k=k0(t1,t2,…). Then X is defined over some finitely-generated purely transcendental extension F of k0 such that
k/F is purely transcendental. That is, there is a variety X of finite type over F, such that Xk=X.
Since extensions k/F and E/F are isomorphic, we get what we need.
□
2 Motivic category of a field extension
Everywhere below DM(k;Fp) will denote the triangulated motivic category of Voevodsky over Spec(k)
with Fp-coefficients (see [19], [3]).
We will construct the local versions of this category, corresponding to all finitely-generated field extensions E/k,
or, in other words, to all points of the big Nisnevich site over Spec(k).
The local motivic categories will be obtained as full localizing subcategories of a global one by application
of certain projectors. These projectors will be produced using Čech simplicial schemes.
Let P be a smooth variety over k. The Čech simplicial scheme Cˇech(P) has graded components
(Cˇech(P))n=P×(n+1) with faces and degeneracy maps given by partial projections and partial diagonals.
This object is an analogue of the contractible space EG in topology, and it will be contractible in Morel-Voevodsky homotopic
motivic category as long as P has a rational point, while in general, it ”measures” how far we are from acquiring such a point.
In particular, it is a form of a point, since it certainly contracts over algebraic closure.
Let us denote the motive of Cˇech(P) as XP.
The natural projection Cˇech(P)→Spec(k) provides the morphism
XP→T to a trivial Tate-motive, which is an isomorphism if and only if P has a zero cycle of degree 1 (modulo p, in our case)
(a ”weak form” of a rational point) - [14, Thm 2.3.4].
This gives an exact triangle
[TABLE]
where XP and XP are mutually orthogonal idempotents:
[TABLE]
Thus, the functors of tensor product with these objects:
[TABLE]
are projectors. This defines the semi-orthogonal decomposition of the category DM(k;Fp) as
an extension of XP⊗DM(k;Fp) by XP⊗DM(k;Fp), as there are no Hom’s from the latter subcategory to
the former one (by [14, Thm 2.3.2], which is, basically, [20, Lem. 4.9]).
For different varieties, these projectors naturally commute and we have canonical (co-associative, respectively, associative)
identifications
[TABLE]
(note, that endomorphism rings of XV and XV are either Fp, or zero - [14, Thms 2.3.2, 2.3.3], and such
an endomorphism is fixed by the map XV→T, respectively, T→XV).
Thus, tensor product of any (finite) number of such objects can be always expressed as XR⊗XS, for some R and S.
Each XP corresponds to a sub-sheaf χP of the constant sheaf T=Fp on the big Nisnevich site over Spec(k)
defined as follows. For a smooth connected quasi-projective variety X,
χP(X)=Fp, if P has a zero-cycle of degree 1 over k(X), and it is zero, otherwise.
Equivalently, χP(X)=Fp exactly when XP⊗M(X)=0 ([14, Thms 2.3.6, 2.3.3]).
Respectively, XP corresponds to the quotient sheaf
χP=T/χP. We can introduce an order on the set of XQ’s as follows:
Definition 2.1
We say that XQ⩾XP if any of the following equivalent conditions is satisfied:
(1)
The natural map XQ←≅XQ⊗XP is an isomorphism;
(2)
The natural map XQ⊗XP←≅XP is an isomorphism;
(3)
The map XQ→T factors through XP→T;
(4)
P* has a zero-cycle of degree 1 modulo p over the generic point of every component of Q;*
(5)
χQ* is a sub-sheaf of χP.*
Here (1)⇔(2) is automatic from the definition; (2)⇒(5) follows from the description of
χP above; (5)⇒(4) follows from the fact that χQ(Ql)=Fp, for any connected component Ql of Q;
(4)⇒(1) is [14, Thm 2.3.6]; (1)⇒(3) is straightforward; and, finally, (3)⇒(1)
is clear, since XQ⊗XP⊗(XQ→T) is the identity map of XQ⊗XP.
Note, that the relation XQ⩾XP is obviously transitive. In the case of connected varieties, this
relation may be formulated in terms of the respective field extensions (generic points).
Let E/k and F/k be two finitely-generated extensions of a field of characteristic zero.
Let P/k and Q/k be smooth projective varieties whose function fields are identified with E and F.
Definition 2.2
We say that F/k⩾E/k, if there exists a correspondence of degree 1 (with Fp-coefficients)
Q⇝P. We call extensions ”equivalent” F/k∼E/k, if F/k⩾E/k and E/k⩾F/k.
By the composition of correspondences, the property F/k⩾E/k is transitive.
It is also equivalent to the condition XQ⩾XP above.
If k/l is a field extension, then F/k⩾E/k implies that F/l⩾E/l.
Let P be some smooth variety (of finite type) over k.
Let Q be the disjoint union of all connected varieties Q/k, such that
XQ≩XP (so, it is a smooth variety, but with infinitely many components), and let XQ be the motive
of the respective Čech simplicial scheme, which is still an idempotent in DM(k;Fp), and XQ be the
complementary idempotent. Define
[TABLE]
We can view ΥP as a colimit of projectors XQ⊗XP, where Q runs over all smooth projective varieties
of finite type with XQ≩XP.
Note, that if P is not connected up to equivalence, that is, if P can’t be substituted by a connected variety with the
same X, then ΥP=0. Indeed, let P1 be a ”minimal” component, that
is, XP1⩾XPi implies that XP1=XPi. Suppose, there exists another component P2 with
XP2⩾XP1. Let P^1 be the union of all the components equivalent to P1. Then for
Q1=P\P^1 and Q2=P^1 we have:
XQ1≩XP, XQ2≩XP, but XQ1∐Q2=XP.
Now we can define the local motivic category corresponding to a finitely-generated extension E/k (cf. [18, Sect. 4]).
Definition 2.3
Let E/k be a finitely generated extension and
P/k be a smooth connected variety with k(P)=E.
Define the ”motivic category of the extension E/k” as the full localizing subcategory
[TABLE]
of DM(k;Fp), and the ”local geometric category” DMgm(E/k;Fp) as the full thick triangulated subcategory
of DM(E/k;Fp) generated by (local) motives of smooth projective varieties.
This definition doesn’t depend on the choice of a smooth model P, since XP depends on k(P) only.
Moreover, it depends only on the ∼-equivalence class of an extension E/k.
In the case of a trivial extension, we obtain (cf. [18, Sect. 4]):
Definition 2.4
The ”isotropic motivic category” is the full localizing subcategory DM(k/k;Fp) of DM(k;Fp) given by
ΥSpec(k)⊗DM(k;Fp),
while the geometric version DMgm(k/k;Fp) is the full thick triangulated subcategory of it generated by (isotropic) motives
of smooth projective varieties.
Now, we can read the information about motive by looking at local versions of it.
Namely, we get a collection {φE∣E/k−f.g. extension} of localization functors
[TABLE]
parameterized by all points of the big Nisnevich site over Spec(k). These can be further specialized
to isotropic realizations
[TABLE]
The following result shows that there are no unexpected objects
in the isotropic geometric category.
Proposition 2.5
The category DMgm(k/k;Fp) is the idempotent completion of the full subcategory ΥSpec(k)⊗DMgm(k;Fp) of DM(k;Fp).
Proof:
We need to prove that ΥSpec(k)⊗DMgm(k;Fp) is closed under cones. For this, it is sufficient to show
that, for any objects U,V of DMgm(k;Fp) and a map f:XQ⊗U→XQ⊗V
(where Q is the disjoint union of all anisotropic varieties over k), there is a map f:U′→V′ in DMgm(k;Fp),
such that f⊗idXQ≅f. Composing the map f with U→XQ⊗U we obtain
a map g:U→XQ⊗V with the property that g⊗idXQ≅f.
Define (XQ)⩽n as Cone((XQ)⩽n−1→T) and (XQ)>n
as Cone((XQ)⩽n→XQ). Then (XQ)>n is an extension of M(Y)[r],
for some smooth varieties Y and r>n. Since U and V are geometric, for sufficiently large n, there are no Hom’s from U
to (XQ)>n⊗V. Hence, the map g can be lifted to a map
f′:U→(XQ)⩽n⊗V, which, in turn, can be lifted to a geometric map
f:U→(XQ)⩽n⊗V, for some anisotropic variety Q of finite type over k.
Since XQ⊗(XQ)⩽n=XQ, for any n⩾0,
we obtain that f⊗idXQ≅f.
□
We can describe Hom’s from geometric isotropic motives as follows.
For an object X of DM(k;Fp) and some idempotent ξ, we will denote by the same letter the image of X in
ξ⊗DM(k;Fp).
Proposition 2.6
Let U∈Ob(DMgm(k;Fp)) and V∈Ob(DM(k;Fp)). Then
[TABLE]
where the colimit is taken over all the functors
XS⊗:XR⊗DM(k;Fp)→XS⊗DM(k;Fp),
for XR⩾XS=T. In other words, Q runs over all anisotropic varieties over k.
Proof:
We have: HomDM(k/k;Fp)(U,V)=HomDM(k;Fp)(ΥSpec(k)⊗U,ΥSpec(k)⊗V),
and the latter can be identified with HomDM(k;Fp)(U,XQ⊗V), where
Q is the disjoint union of all anisotropic varieties over k. But since U is geometric, any map
U→XQ⊗V factors through U→XQ⊗V, for some anisotropic Q of finite type,
and the map U→XQ⊗V vanishes when extended to a map to XQ⊗V if and only if
there exists an anisotropic Q′ with XQ⩾XQ′, such that the composition U→XQ⊗V→XQ′⊗V
is zero. Thus, our Hom-group can be identified with the
[TABLE]
where the colimit is taken over a directed system (as XQi⩾X∐iQi and if XQi=T,
for each i, then X∐iQi=T, since the coefficients are Fp).
□
Geometric motives vanishing in the local category can be also detected by projectors corresponding to varieties of finite type.
Let P be smooth connected variety with E=k(P).
Proposition 2.7
An object U of DMgm(k;Fp) vanishes in DM(E/k;Fp) if and only if there is a variety Q of finite type over k,
with XQ≩XP and XQ⊗XP⊗U=0.
Proof:
If ΥP⊗U=0, then (XQ⊗U)E=0, where, as above, Q is the disjoint union of all
smooth connected varieties Q over k, with XQ≩XP. That means that the projection (XQ⊗U→U)E
has a section (from the right). But since U is geometric, such a section will factor through some section of
(XQ⊗U→U)E for some variety Q of finite type over k with XQ≩XP. Hence,
(XQ⊗U)E=0 (as UE is a direct summand of XQ⊗UE, and so, XQ⊗UE is a direct summand
of it as well, but the latter object is stable under XQ⊗ while the former one is killed by it).
But, according to [14, Thm. 2.3.5], the functor
XP⊗DM(k;Fp)→DM(E;Fp) is conservative. Hence, XQ⊗XP⊗U=0 in DM(k;Fp).
□
Since XQ⊗M(Q)=0, the projection to the isotropic motivic categoryDM(k/k;Fp) kills the motives of all
anisotropic varieties over k. Hence, the name of this category.
Remark 2.8
The isotropic motivic categoryDM(k/k;Fp) is the Verdier localization of DM(k;Fp) modulo the localizing
subcategory A generated by motives of anisotropic varieties111I’m grateful to T.Bachmann for pointing this out..
Indeed, an object U of DM(k;Fp) vanishes in DM(k/k;Fp) if and only if U=U⊗XQ, where
Q is the disjoint union of all connected anisotropic varieties Q/k. Hence, U belongs to A, since this
subcategory is a tensor ideal. By the universal property of the Verdier localization, ψE:DM(k;Fp)→DM(k/k;Fp)
is equivalent to DM(k;Fp)→DM(k;Fp)/A.
*
△*
We have functoriality for the ”denominator” of the extension E/k.
Suppose, we have a tower of fields L⊂F⊂E, and P/L, Q/L are smooth projective varieties with L(P)=E and
XQ≩XP. Then Q remains anisotropic over L(P), and so, over F(P) (since F⊂L(P)).
Hence, XQ∣F≩XP∣F.
Thus, we get a natural functor
[TABLE]
The following result shows that, in the case of a flexible ground field, we can pass from (geometric) local realizations{φE∣E/k−f.g. extension} to isotropic realizations{ψE∣E/k−f.g. extension}
without loosing any information.
Proposition 2.9
Let E/k be a finitely-generated extension of a flexible field. Then the functor
[TABLE]
is conservative on the image of φE.
Proof:
Let us start with purely transcendental extensions.
Lemma 2.9.1
Let E/L/k be a tower of finitely generated extensions where L/k is a purely transcendental extension of a flexible field.
Then the functor
[TABLE]
is conservative on the image of φE.
Proof:
Let L=k(An), and E=k(R) for some smooth variety R/k.
Let U∈Ob(XR⊗DMgm(k;Fp)) be an object vanishing in DMgm(E/L;Fp). Then,
according to the Proposition 2.7, there exists a
variety Q/L of finite type such that XQ≩XRL and UL⊗XQ=0 in DM(L;Fp).
The condition XQ≩XRL means that we have an L-correspondence
α:Q⇝RL of degree one, and there is no such correspondence in the opposite direction.
Since k=k0(P∞) is flexible,
varieties R and Q are, actually, defined over F and M=F(An), respectively, where extensions k/F/k0 are
purely transcendental and F/k0 is moreover finitely generated. By the same reason, we can assume that
the geometric object U is defined over F, while
the correspondence α is defined over M.
So, there exist varieties R/F, Q/M, an object U of XR⊗DMgm(F;Fp) and a degree one M-correspondence
α:Q⇝RM such that R∣k=R, Q∣L=Q, U∣k=U and α∣L=α.
Note, that we still have: XQ≩XRM (since α is defined over M and by functoriality),
and UM⊗XQ=0 (since the restriction DM(M;Fp)→DM(L;Fp) is conservative).
But the extension
M/F can be embedded into k/F making k/M purely transcendental. Let Q′ be a variety over k obtained from
Q using this embedding. Then XQ′≩XR (since k/M is purely transcendental) and
U⊗XQ′=0 in DM(k;Fp). Hence,
U=0 in DM(E/k;Fp).
□
Using Lemma 2.9.1 our problem is reduced to
the case of a finite extension. In this situation, the statement is true for an arbitrary field.
Lemma 2.9.2
Let E/L be a finite extension of fields. Then the functor
[TABLE]
is conservative.
Proof:
Let E=L(P) for some smooth connected 0-dimensional variety P.
Let U∈Ob(XP⊗DM(L;Fp)) be an object
vanishing in DM(E/E;Fp). Then, for the disjoint union Q of all anisotropic varieties over E,
we have: UE⊗XQ=0 in DM(E;Fp). Consider a smooth L-variety Q
given by the composition
Q→Spec(E)→Spec(L). We have a natural map Q→QE.
This means that XQ⩾XQE,
and so, UE⊗XQE=0 as well. Clearly, XQ⩾XP.
Suppose, these are equal. Then there exists a commutative
diagram
[TABLE]
where F is an extension of E of degree prime to p. But since [E:L] is finite, the composition
Spec(F)→Q→Spec(E) has the same (prime to p) degree.
This contradicts to the fact that Q is anisotropic.
Hence, XQ≩XP, and so,
XQ⩾XQ, where Q is a disjoint union of all L-varieties Q
with XQ≩XP. Thus, (U⊗XQ)E=0 as well.
By [14, Thm 2.3.5], the functor
XP⊗DM(L;Fp)→DM(E;Fp) is conservative,
so, (U⊗XQ)⊗XP=0 in DM(L;Fp). This means that U=0 in DM(E/L;Fp).
□
Another type of functoriality we have is the following one. Let k(A)/k be a purely transcendental extension of k. Then we have a
natural functor
[TABLE]
One just needs to observe that the inequality XQ≩XP is preserved under the passage from k to k(A).
It is natural to ask, in which situations will our localization functors be conservative?
Question 2.10
a* a*
(a)
What is the kernel of the collection of functors {φE∣E/k−f.g. extension}?
(b)
What is the kernel of the collection of functors {ψE∣E/k−f.g. extension}?
Since the passage from k0 to k=k0(t1,t2,…) is conservative, and any finitely generated extension E of k has the form
E=E0(tN,…), for some finitely-generated extension E0 of k0, and by Proposition 2.9,
the triviality of
{φE0∣E0/k0−f.g. extension} on X0
implies the triviality of
{ψE0∣E0/k0−f.g. extension} on X0,
implying the triviality of
{ψE∣E/k−f.g. extension} on X0∣k,
which, in turn, is equivalent to the triviality of
{φE∣E/k−f.g. extension} on X0∣k.
Thus, for a given geometric object X0/k0,
[TABLE]
where (a) means that X0 is in the kernel of the family {φE0∣E0/k0−f.g. extension},
(a)flex means that X0∣k (the restriction to the flexible closure) is in the kernel of the family
{φE∣E/k−f.g. extension}, etc..
Remark 2.11
Restricting the functors ψE to the tensor triangulated subcategory DQMgm generated by motives of smooth projective quadrics,
and specializing it further, one gets the functors of T.Bachmann ΦE:DQMgm→Kb(Tate(F2)) to the category of
bi-graded F2-vector spaces - see [1].
This can be deduced from the fact that the functor ψE maps the subcategory DQMgm to the subcategory of
geometric Tate-motives in DM(E/E;Fp) (by [18, Prop. 4.9]).
The functors ΦE, constructed originally by completely different methods,
were shown by T.Bachmann to be conservative [1, Thm. 31]. In particular, the collection
{ψE∣E/k−f.g. extension} is conservative on DQMgm. Our approach also permits to see conservativity on this and
other similar subcategories. Namely, it follows from [18, Prop. 4.9] that, for any object A of DQMgm, there exists
a finite filtration by idempotents on the unit object T, such that associated graded idempotents map A to geometric Tate-motives.
And this collection of associated graded idempotents (having a form XQ⊗XP, for some smooth varieties P and Q, with
P-connected) acts conservatively (as the unit object is an extension of them). It remains to
observe that, for geometric Tate-motives, the triviality of XQ⊗XP⊗A is equivalent to the triviality
of ΥP⊗A∈Ob(DM(E/E;Fp)), for E=k(P).
*
△*
Remark 2.12
If the ground field k0 is algebraically closed, then there exists only one ∼-equivalence class of
finitely-generated extensions of k0 (the trivial one). Thus, there is only one ”local” point and only one localization functor
φ:DM(k0;Fp)⟶DM(k0/k0;Fp) which is an equivalence of categories
(as there are no anisotropic varieties over k0).
Thus, in this case, the family {φE0∣E0/k0−f.g. extension} is conservative, but it does not provide
any interesting information.
*
△*
The collection {φE∣E/k−f.g. extension} is not conservative, in general.
Example 2.13
(1) Let k be a flexible field and C be an elliptic curve over k without complex multiplication. Consider p=2.
Then M(C)=T⊕M(C)⊕T(1)[2]. Consider the Chow groups ChNum(p) modulo numerical equivalence with
F2-coefficients - see Subsection 4.2. Then
[TABLE]
Indeed, for an arbitrary p, such a group is generated by [pt×C], [C×pt] and the class of the diagonal [Δ]
(in the absence of complex multiplication).
But with F2-coefficients, [Δ]∼Num(p)[pt×C]+[C×pt].
Thus, M(C)=0 in ChowNum(E;F2), for any extension E/k. Hence, by Theorem 4.11(1),
it is zero in Chow(E/E;F2) which is a subcategory of DM(E/E;F2). So, all isotropic realizations ψE(M(C))
are trivial.
At the same time, M(C) is non-trivial, since the (complex) topological realisation of it is non-trivial (has non-zero HTop1).
Alternatively, one can see that the restriction to the algebraic closure M(C)∣k is non-trivial.
Note, that the choice of a prime was essential here.
(2) Refining the previous example, we can show that even the combination
[TABLE]
is not conservative on DMgm(k;F2).
In the above situation, consider some non-trivial quadratic extension F=k(a) and P=Spec(F)→πSpec(k).
Let α={a}∈K1M(k)/2 and
Mα be the ”completely” reduced Rost-motive - see the proof of Theorem 3.5. This motive fits into the
exact triangle Mα→Xα[1]→Xα→Mα[1], where
Xα=XP.
Let us show that U=M(C)⊗Xα=0. Indeed,
such a triviality is equivalent to the fact that the projection XP×M(C)→M(C) has a section.
And since M(C) is a pure motive (= Chow motive), any such section is liftable to a section of
P×M(C)→M(C).
This would mean
that the projector ρ defining M(C) is in the image of the natural map π∗:Ch1(C×C×P)→Ch1(C×C).
Note however, that Ch1(C×C∣k)=[Δ]⋅F2⊕[pt×C]⋅F2⊕[C×pt]⋅F2 (since
k-points of the Jacobian form a 2-divisible group), and so the map
resk∘π∗:Ch1(C×C×P)→Ch1(C×C∣k) is zero (since the action of the Galois group on
Ch1(C×C∣k) is trivial, which implies that resk∘π∗=2⋅resk/F).
On the other hand, ρ∣k=0, since it is non-zero even in the topological realization. Hence, ρ is not in the
image of resk∘π∗ and M(C)⊗Xα=0. Notice, that ψE(U)=0, since
ψE(M(C))=0, while resk(U)=0, since resk(Xα)=0. Thus, we have produced a non-trivial
example on which the needed combination of functors vanishes, but so far, not a geometric one.
Consider V=M(C)⊗Mα. Then we have a distinguished triangle
V→U[1]→U→V[1]. In particular, V is geometric and all the above functors vanish on it. It remains to show
that V=0. Note that, since U=0, the homology HomDM(E;F2)(T(∗)[∗′],U) considered for all finitely generated
extensions E/k, is non-trivial. At the same time, this homology is zero for ∗′<∗ (below the main diagonal).
This implies that V=0. Indeed, if it would be zero, then the homology of U would be [1]-periodic, which is not the case.
*
△*
2.1 Local Chow motivic category
Let X be a scheme of finite type over k. We can define its isotropic Chow groups as
[TABLE]
where Mc(X) is the motive with compact support of X - see [19].
For smooth varieties, we have from duality:
[TABLE]
The theory Chk/k has natural pull-backs and push-forward maps coming from the respective maps between motives of varieties,
which satisfy all the axioms of [9, Def. 1.1.2] (since these follow from the properties of motives). Finally, we have
the excision axiom (EXCI), claiming that for a scheme X with the closed subscheme Z and open complement U, there is an
exact sequence:
[TABLE]
This follows from the Gysin exact triangle [19, (4.1.5)]:
[TABLE]
and the fact that the map Ch∗↠Chk/k∗ is surjective, which follows from Proposition 2.16
below. Thus, Chk/k∗ is an oriented cohomology theory (with excision) on Smk in the sense of [17, Def. 2.1].
Definition 2.14
Let Q be a scheme (of finite type) over k and n∈N. We say that Q is ”n-anisotropic”, if the degrees of
all closed points of Q are divisible by n.
Schemes which don’t have this property will be called not n-anisotropic, while we will reserve the term isotropic for
a scheme having a zero-cycle of degree 1 (mod n). Below almost everywhere we will be dealing with n=p-prime, and so isotropic
will be the complement to anisotropic. Unless specified, the term anisotropic will mean p-anisotropic, for some prime
p.
Definition 2.15
Let X be a scheme over k, and x∈Chr(X). We call x ”anisotropic”, if there exists a proper morphism
f:Y→X from a p-anisotropic scheme Y and a class y∈Chr(Y) such that x=f∗(y).
For fields of characteristic zero and X projective, x is anisotropic if and only if it is a push-forward of the generic cycle
from some smooth projective anisotropic variety over k.
Isotropic Chow groups can be alternatively described as follows.
Proposition 2.16
[TABLE]
Proof:
By Proposition 2.6, HomDM(k/k;Fp)(T(r)[2r],Mc(X)) is the colimit of the groups
[TABLE]
where Q runs over all anisotropic varieties over k.
Recall, that we have an exact triangle
[TABLE]
By [14, Thm 2.3.2] (which is, basically, [20, Lem 4.9]),
HomDM(k;Fp)(XQ(∗)[∗′],Mc(X)⊗XQ)=0, and so, our group is the colimit of groups
HomDM(k;Fp)(T(r)[2r],Mc(X)⊗XQ), where Q can be assumed to be projective.
Since XQ is an extension of M(Q×i)[i], for i⩾0, and HomDM(k;Fp)(T(r)[2r],Mc(Y)[i])=0, for any i>0
and any scheme Y of finite type, we can identify:
[TABLE]
Thus,
HomDM(k/k;Fp)(T(r)[2r],Mc(X))=Chr(X)/I, where I is the subgroup generated by the images of (πQ)∗, for all
anisotropic varieties Q/k. In other words, we mod-out all anisotropic classes.
□
The isotropic motivic categoryDMgm(k/k;Fp) has a pure part.
Definition 2.17
*Define the ”isotropic Chow motivic category” Chow(k/k;Fp) as the full additive subcategory of DMgm(k/k;Fp)
the image of Chow(k;Fp) under the natural projection*
[TABLE]
Thus, the objects of Chow(k/k,Fp)
can be identified with direct summands of motives of smooth projective varieties over k, while the morphisms are described as follows.
Proposition 2.18
Let X and Y be smooth projective k-varieties. Then
[TABLE]
Proof:
If B is an object of DMgm(k;Fp) with the dual B∨, and A,C are objects of DM(k;Fp), then we have a functorial
identification
[TABLE]
Hence, for the projector ρQ=XQ⊗ we also have a functorial identification
[TABLE]
Taking into account that M(X)∨=M(X)(−d)[−2d], where d=dim(X), we obtain that
[TABLE]
□
We can describe Chow motives disappearing in the isotropic category.
Remark 2.19
An object U of Chow(k,Fp) vanishes in Chow(k/k,Fp) if and only if it is a direct summand in the motive of a (smooth
projective) anisotropic variety222I’m grateful to T.Bachmann for emphasizing this..
Indeed, a direct summand U of M(P) vanishes in Chow(k/k,Fp) if and only if the identity map idU:U→U does.
By Propositions 2.16 and 2.18, this means that the map ΔU:T→U⊗U∨ factors through
(the motive of) a smooth projective anisotropic variety Q. Consequently, U is a direct summand of M(Q)⊗U, which, in turn, is a direct summand of M(Q×P), and the latter variety is still anisotropic.
*
△*
The functor Chow(k,F/p)→Chow(k/k,F/p) is surjective
on morphisms.
In other words, all ”local” morphisms between (isotropic) Chow motives are defined ”globally”.
We will have a closer look at the category Chow(k/k,Fp) in Section 4.
3 Local motivic cohomology of a point
In this Section we will compute the motivic cohomology of a point in the isotropic motivic category, for p=2.
This will be achieved by substituting all anisotropic k-varieties in the colimit of Proposition 2.6
by norm-varieties for non-zero pure symbols from K∗M(k)/2 (anisotropic Pfister quadrics, in our case).
This makes the problem amenable to calculation due to Voevodsky technique. Moreover, the resulting answer, drastically different from
the ”global” one, in turn, sheds some light on this technique.
The starting point is the following statement,
which is a slight modification of the result of J.-L.Colliot-Thélène and M.Levine [4, Theorem 3].
We provide a somewhat different proof.
Statement 3.1
Let B be an anisotropic (mod n) projective variety. Then, over some finitely generated purely transcendental extension,
it can be embedded into an anisotropic hypersurface of degree n.
Proof:
Embed B into a projective space. Passing to a Veronese embedding, we can assume that all the relations in the projective coordinate
ring of B are generated by quadratic ones, or in other words, that B is defined by quadrics.
Then it will be also defined by hypersurfaces of degree n (in our Pm), for any n⩾2.
Let Pr=Proj∣D∣ be the projective
system of hypersurfaces of degree n containing B. I claim that the generic element of this linear system is an anisotropic hypersurface.
Consider Y⊂(Pm\B)×Pr defined by Y={(x,H)∣x∈H}. Then Y is a projective bundle
Proj(Pm\B)(V) over (Pm\B), where V is a co-dimension one subbundle in the trivial bundle ∣D∣.
Let Yη be the generic fiber of the projection
Y→Pr. This is exactly (Qη\B), where Qη is the generic hypersurface of degree n passing through B.
Note, that the degree (mod n) is well-defined on the zero-cycles on Yη, since B is anisotropic.
By the projective bundle theorem, CH∗(Y) is a free module over CH∗(Pm\B) with the basis 1,ρ,…,ρr−1,
where ρ=c1(O(1)). On the other hand, we have a surjective ring homomorphism CH∗(Y)↠CH∗(Yη)
which is zero on ρ (as this class is supported on a hypersurface in Pr). Thus, we obtain the surjective map
CH∗(Pm\B)↠CH∗(Yη) which sends the class c∈CH∗(Pm\B) to the
restriction of π∗(c) to Yη, where π is our projective bundle fibration. In particular, c∈CH1(Pm\B)
is mapped to a zero cycle on Yη whose degree is equal to the intersection number of c and any hypersurface from our linear
system (which, again, makes sense, since B is anisotropic). Hence, it is a zero cycle of degree [math] (mod n). Thus, the degrees of all
zero-cycles on Yη are divisible by n, and so, the same is true about Qη=Yη∪B.
□
Corollary 3.2
Let k be a flexible field, U∈Ob(DMgm(k;Fp)) and V∈Ob(DM(k;Fp)). Then
[TABLE]
where the colimit is taken over all the functors ⊗XQ, where Q runs over all anisotropic hypersurfaces of degree p
over k. This system is directed.
Proof:
Let B be any anisotropic variety over k.
By the Statement 3.1, there exists a purely transcendental field extension E/k and anisotropic hypersurface Q over E
such that XB∣E⩾XQ. Let k=k0(P∞). Then there exists a diagram of purely transcendental extensions of fields
[TABLE]
with the extensions of the bottom row finitely generated, such that
the variety B is defined over l, while the variety Q and the correspondence B⇝Q (of degree 1)
are defined over L. But we can embed L into k over l so that k/L will be purely transcendental.
Thus, we obtain an anisotropic hypersurface Q′ over k together with
a correspondence B⇝Q′ of degree 1.
Anisotropic hypersurfaces of degree p thus form a
final subsystem in the system of all anisotropic varieties
which is directed, hence this subsystem is directed
as well.
□
Corollary 3.3
Let k be a flexible field and p=2. Let U∈Ob(DMgm(k;Fp)) and V∈Ob(DM(k;Fp)). Then
[TABLE]
where the colimit is taken over all the functors ⊗XQα, where α runs over all non-zero pure symbols from
K∗M(k)/2 and Qα is the respective Pfister quadric. This is a directed system.
Proof:
By [15, Cor. 3] (see also [8]), every anisotropic quadric Q (over any field k) can be embedded into an anisotropic
Pfister quadric Qα
over an appropriate purely transcendental extension of finite transcendence degree. If now k is flexible, then arguing as in the proof
of Corollary 3.2, we can embed Q into some anisotropic Pfister quadric Qα′ over k. Thus, the set of anisotropic Pfister
quadrics form a
final subsystem in the system of all anisotropic varieties over a flexible field, which, again, must be directed.
□
From the fact that the system in Corollary 3.3 is directed, as a by-product, we obtain the following result
(which, of course, is a simple consequence of Statement 3.1 and [15, Cor. 3], and can be even seen from the
latter result alone):
Proposition 3.4
Let k be a flexible field, and {αl}l∈L be a finite collection of non-zero pure symbols
from K∗M(k)/2. Then there exists a non-zero pure symbol α∈K∗M(k)/2 divisible by every αl.
Using Corollary 3.3,
we can compute the cohomology of a point in isotropic motivic category for p=2.
For a non-zero pure symbolα∈KrM(k)/2, let us denote as DM(α~/k;F2)
the full triangulated subcategory
Xα⊗DM(k;F2), where Xα=XQα and Qα is the respective Pfister quadric.
Hom’s between Tate-objects in this category can be computed as follows.
Define an F2-vector space Q−1(n)=⊕IrI⋅F2, where I runs over all subsets of n={0,1,…,n},
with the structure of a module over
Milnor’s operations Qi defined by: Qi(rI)=rI\i, if i∈I, and zero otherwise, and with the bi-degree of
r∅ being (0)[0].
Let r{n+1} be a polynomial generator with Qn+1(r{n+1})=r∅ and
Qi(r{n+1})=0, for i=n+1.
Let Rα be a module over K∗M(k)/2 isomorphic to the principal ideal α⋅K∗M(k)/2
with the generator in bi-degree (0)[0]. In other words, Rα=K∗M(k)/Ker(⋅α).
In particular, it has a natural ring structure. The multiplicative structure on Q−1(n)[r{n+1}]⊗F2Rα is provided by
rI=∏i∈Ir{i} and the identity:
r{i}2=r{i+1}⋅ρ, for 0⩽i⩽n, and ρ={−1}.
In other words, this is the ring Rα[r{i}∣0⩽i⩽n+1]/(r{i}2−r{i+1}⋅ρ∣0⩽i⩽n).
For a motivic category D with Tate-objects, let us denote as EndD(V) the ring ⊕a,bHomD(V,V(a)[b]).
Theorem 3.5
Let α∈KmM(k)/2 be a non-zero pure symbol. Then
[TABLE]
Proof:
By definition,
EndDM(α~/k;F2)(T)=EndDM(k;F2)(Xα).
From this point, all the Hom’s will be in the category DM(k;F2), unless specified otherwise, so I will omit it from notations.
Let Mα be the respective Rost motive ([12]).
We have natural maps
T(d)[2d]→Mα→T, where d=2m−1−1, whose composition is zero. Cutting out the respective Tate-motives from Mα
and tensoring the result by Xα and Xα, respectively, we obtain:
[TABLE]
Here we are using the fact that Mα⊗Xα=0 and that Mα⊗Xα=0,
which are equivalent to the exactness
of the left triangle - [22, Thm 4.4]. Let us denote the above half of the octahedron as ♢.
Note, that since there are no Hom’s from Xα to Xα(∗)[∗′], we can naturally identify groups
Hom(Xα,Xα(∗)[∗′])=Hom(T,Xα(∗)[∗′]).
For each 0⩽i<m−1, let β∈Ki+1M(k)/2 be any pure symbol dividing α. We obtain a similar map
ηβ(−di)[−2di]:Xβ→Xβ(−di)[−2di−1], where di=2i−1.
Tensoring it with Xα, we obtain the map r{i}:Xα→Xα(−di)[−2di−1].
Or, in other words, an element r{i}∈HomDM(α~/k;F2)(T,T(−di)[−2di−1]).
Below we will see that this map doesn’t depend on the choice of the divisor β.
For any smooth projective R, we have the natural (homological) action of the Steenrod algebra on
Hom(T,XR(∗)[∗′]) and the natural (cohomological) action of it on Hom(XR,T(∗)[∗′]),
which commute with the maps XR→XS (for XR⩾XS).
In particular, we have the action of the Milnor’s operations Qi.
If R is a νi-variety, then by the arguments of V.Voevodsky [22, Cor 3.8],
the differential Qi is exact on Hom(XR,T(∗)[∗′]). By the same arguments, it is exact on
Hom(T,XR(∗)[∗′]). In particular, in our case,
Qi is exact on Hom(T,Xα(∗)[∗′]) and Hom(Xα,T(∗)[∗′]), for any i⩽m−1.
Consider N=⊕Hom(Xα[−1],Xα(∗)[∗′]). It has the natural right action of
A=End(Xα)
as well as the left action of A=End(Xα). In particular, there is a right action by η and a
left one by μ. I claim that these are mutually inverse. Indeed, to see that for any f:Xα→Xα(a)[b],
one has μ∙f∙η=f, it is sufficient to look at the ”vertical axis” of
♢⊗(Xα→fXα(a)[b]), which is (after rotating by 90∘):
[TABLE]
Thus, N is μ−η-periodic, as the action by μ and
η are mutually inverse isomorphisms on N.
At the same time,
Hom(Xα,Xα(a)[b])=Hom(T,Xα(a)[b]) is zero for b>a, while Hom(Xα,T(a)[b])=0,
for b⩽a+1 by the Beilinson-Lichtenbaum ”conjecture” (note, that Xα disappears in the etale topology).
Considering Hom’s from Xα[−1] to the (a)[b]-shifted exact triangle
Xα→T→Xα→Xα[1],
we obtain that
A is exactly the ⩽0 diagonal part of N, while
HM∗,∗′(Xα[−1];F2) is exactly the >0 diagonal part of it.
Thus, N combines the homology and cohomology groups of Xα.
Since there are no Hom’s from T to Xα(a)[a+1], the map Hom(T,T(a)[a])↠Hom(T,Xα(a)[a])
is surjective, and so, the [math]-th diagonal of A (or, which is the same, the [math]-th diagonal of N) as a K∗M(k)/2-module
is generated by 1 - the unit of this ring. Let Rα be this [math]-th diagonal.
From μ−η-periodicity, the diagonal number (−2m−1) (where η resides),
as a K∗M(k)/2-module, is generated by η. Since the differential Qm−1 is exact on A, we obtain that 1 is covered
by the image of Qm−1 (since A is concentrated in non-positive diagonals). But the only non-zero element of the needed
bi-degree is η. Thus, Qm−1(η)=1. Applying the same arguments to the symbol β (considered above), we obtain that
Qi(ηβ)=1, and so, Qi(r{i})=1.
For any I⊂(m−2), denote rI:=∏i∈Ir{i} and QI=∘i∈IQi.
Denote as Dj the j-th diagonal of N. For 0⩽i⩽m−2, let Ii={i,i+1,…,m−2}.
Since HM∗,∗′(Xα[−1];F2) is trivial below the 1-st diagonal,
and Ql’s are exact, the composition QIi:D2i→D2m−1 is injective.
But from μ−η-periodicity, D2m−1 as a K∗M(k)/2-module is generated by μ.
In particular, the D2i is trivial below μ∙1∙rIi. By the μ−η-periodicity,
D2i−2m−1 is trivial below rIi. In particular, Qi(η)=0, for any 0⩽i⩽m−2 (since this element is below rIi),
and since η generates D−2m−1, all the differentials Qi, for i⩽m−2 are trivial on this diagonal.
Applying the same arguments to the divisor β of degree (i+1), we obtain that Ql(ηβ)=0, and hence,
Ql(r{i})=0, for l<i (the fact that Ql(r{i})=0, for l>i, is obvious, since A is concentrated in non-positive
diagonals).
Combining it with the (external) co-multiplication identity for Milnor’s operations:
[TABLE]
where 2I=∑i∈I2i, we obtain that QI(rI)=1, for any I⊂(m−2).
Let us show that D−2I is a free module over D0=Rα generated by rI. Let s be the smallest element of I
(which we assume to be m−1, if I is empty).
Decreasing induction on s. The (base) s=m−1 follows from μ−η-periodicity.
The (step): let 2J=2I+2s. Since I\s and J consist of elements
larger than s, by inductive assumption, D−(2I+2s)=rJ⋅D0 and D−(2I−2s)=rI\s⋅D0 (where we
denote r{m−1}:=η).
In particular, Qs is trivial on D−(2I+2s), and from the exact sequence
D−(2I+2s)⟶QsD−2I⟶QsD−(2I−2s), taking into account that Qs(rI)=rI\s,
we see that Qs:D−2I⟶≅D−(2I−2s) is an isomorphism inverse to the multiplication by rs. Thus,
D−2I=rI⋅D0.
From μ−η-periodicity we obtain that A is a free module over Rα generated by ηk⋅rI, for
k⩾0 and I⊂(m−2), while HM∗,∗′(Xα[−1];F2) is a free module over Rα
generated by μl∙rI, for l>0 and I⊂(m−2).
Consider γ=μ∙1∙r(m−2) - the generator of D1 - the 1-st diagonal in N, or, which is the same,
the 1-st diagonal in the motivic cohomology of Xα[−1].
By the Beilinson-Lichtenbaum Conjecture,
multiplication by τ identifies D1 with the kernel Ker(K∗M(k)/2→K∗M(k(Qα))/2) - see [20, Lem 6.4].
The generator γ is identified with some element of degree m, which must coincide with the symbol α
(since α vanishes over k(Qα) and there exists exactly one non-zero element of the respective degree in D1).
Hence, as a K∗M(k)/2-module, Rα can be identified
with the principal ideal of K∗M(k)/2 generated by α. So, as a ring,
Rα=(K∗M(k)/2)/(Ker(⋅α)).
This gives the description of A (as well as N) as a module over K∗M(k)/2 and over Steenrod algebra.
Finally, the equation r{i}2=r{i+1}⋅ρ follows from the co-multiplication identity for Milnor’s operations
(1).
□
As a by-product, we obtain the description of motivic cohomology of Xα (known already from the original version of [10]
and [23, Thm 5.8]) but now enhanced with the structure of a module over motivic homology of Xα.
Corollary 3.6
Let α∈KmM(k)/2 be a non-zero pure symbol.
As a module over A=EndDM(k;F2)(Xα),
[TABLE]
It is a free Rα-module with the basis r{m−1}−l⋅rI, for l>0 and I⊂(m−2).
Now we can compute the ”local” motivic cohomology HM∗,∗′(k/k;F2)=EndDM(k/k;F2)(T).
Theorem 3.7
Let k be a flexible field. Then
[TABLE]
Proof:
As we know, our colimit (from Corollary 3.3) is taken over a directed system.
Let α∈KmM(k)/2 and β=α⋅{b}∈Km+1M(k)/2 be non-zero pure symbols. Consider the restriction
[TABLE]
Then res=Xβ⊗ is a ring homomorphism respecting Steenrod algebra action, and, in the notations
of Theorem 3.5,
for I⊂{0,…,m−2}, we have: res(rI)=rI and res(r{m−1}⋅rI)=rI∪{m−1}.
Indeed, res sends r∅ to r∅, while
rI and rI (respectively, r{m−1}⋅rI and rI∪{m−1}) are the only elements (in the source and the target)
which are mapped to r∅ via QI (respectively, QI∪{m−1}). Also, res:Rα→Rβ is
the natural projection, corresponding to the map α⋅K∗M(k)/2⟶⋅{b}β⋅K∗M(k)/2.
where N=∪αKer(⋅α), where α runs over all non-zero pure symbols in K∗M(k)/2.
It remains to observe that N contains K1M(k)/2. Indeed, let {a}∈K1M(k)/2 be any element such that {a}=0={−a}.
Then, from {a,−a}=0, both {a} and {−a} belong to N. This implies that {−1}∈N. Since, over a flexible field, an
element a as above always exists, we obtain that N contains K1M(k)/2, and so, coincides with the augmentation ideal K>0M(k)/2.
Hence, (K∗M(k)/2)/N=F2.
Finally, from the equation r{i}2=r{i+1}⋅ρ it follows that r{i}2=0.
So, we obtain the external algebra in r{i}’s over F2.
□
What is remarkable here, the Milnor’s operations are intertwined into the very fabric of the local motivic category. Also, all the non-zero
elements of HM∗,∗′(k/k;F2) are ”rigid”, in the sense that the identity map of the unit object of the local category can be
obtained from any such element using Milnor’s operations, and so these classes disappear only together with the category itself.
We can now compare ”local” and ”global” motivic cohomology of a point:
[TABLE]
Note, that in contrast to ”global” motivic cohomology of a point residing in the I-st quadrant, the ”local” version resides in the
III-rd one.
In particular, the global-to-local map
[TABLE]
is zero in all bi-degrees aside from (0)[0].
Our ring generators r{i} are related by the action of the Steenrod algebra. Namely, since (modulo ρ={−1}),
Qi+1=[Qi,Sq2i+1] - [21], and ρ disappears locally, anyway, we obtain from bi-degree considerations that
Sq2i+1(r{i+1})=r{i}.
In particular,
Sq1Sq2…Sq2i−1Sq2ir{i}=r∅=1.
Remark 3.8
Despite some similarities between the (complex) topological realization functor and isotropic functors, there is a difference in the way
they handle τ. Namely, τTop=1, while ψE(τ)=0 (in the case of a flexible field).
*
△*
The only obstacle which prevents us from performing the same calculations for odd primes is the lack of the analogue of
[15, Cor. 3] in this situation.
In particular, it would be sufficient to have a positive answer to the following:
Question 3.9
Let Q be an anisotropic hypersurface of degree p over k.
Is it true that, over some finitely-generated purely transcendental extension E/k, the kernel
[TABLE]
contains a non-zero pure symbol?
4 Isotropic category of Chow motives
In this Section we will study in details local Chow motives.
As we will see, over a flexible field, these resemble in many respects their topological counterparts, and
are closely related to the numerical equivalence of cycles with finite coefficients.
In particular, the Hom’s between such local
pure motives are expected to be not larger than Hom’s between their topological realizations, and so
finite-dimensional. We will prove it in various situations.
Let us start by introducing some ”gradual” approach to the numerical equivalence of cycles, which will permit to measure
our progress towards the goal.
4.1 Theories of higher types and numerical equivalence
Let A be a commutative ring and L⟶φA be some formal group law with A-coefficients.
Denote as A(0)∗:=Ω∗⊗LA the respective free theory in the sense of Levine-Morel [9, Rem. 2.4.14].
By [17, Prop. 4.7] this is a theory of rational type. We call this type [math].
We are going to introduce the theory A(n)∗ of type n as some quotient of A(0)∗.
This is based on the following construction (cf. [6, Exa. 4.6]):
Example 4.1
Let A∗ be some oriented cohomology theory (with localization) in the sense of [17, Def. 2.1], and Γ={Qλ,aλ}λ∈Λ be a collection of smooth
projective k-varieties with some classes aλ∈A∗(Qλ). That is, we have a collection of A∗-correspondences
ρλ:Qλ⇝Spec(k).
Construct the new theory AΓ∗ as follows:
[TABLE]
where ρλ×id is the correspondence Qλ×X⇝X.
In other words, we mod out all the elements of the form β∗(α∗(aλ)⋅u),
where u is an arbitrary element of A∗(Qλ×X) and α and β are natural projections:
[TABLE]
One can check that the resulting theory AΓ∗ will be an oriented cohomology theory in the sense of [17, Def. 2.1]
*
△*
Definition 4.2
Let Q⟶πSpec(k) be a smooth projective variety and a∈A∗(Q). We say that a∼Num0, if
π∗(a⋅b)=0, for any b∈A∗(Q).
Now we can introduce the theories of higher types.
Definition 4.3
Consider the collection Γn={Qλ,aλ}λ∈Λ, where Qλ runs through all smooth
projective k-varieties of dimension 2n−1 and aλ∈A∗(Qλ) runs over all elements ∼Num0. Define
[TABLE]
If a∈A∗(Q) is ∼Num0, then a×[(P1)]∈A∗(Q×(P1)×2) is also ∼Num0.
So, the images of correspondences from Γn are covered by those from Γn+1. Hence, we get a chain of surjections
[TABLE]
with the colimit ANum∗. Here ANum∗ is obtained from A∗ by moding-out all classes ∼Num0 on all varieties.
Remark 4.4
For n=1, the theory A(1)∗ is, by definition, the algebraic version Aalg∗.
In particular, CH(1)∗=CHalg∗.*
△*
The meaning of the theory ANum∗ is described by the following universal property.
Proposition 4.5
For any oriented generically constant cohomology theory (with localization) A∗ (in the sense of [17, Def. 2.1] and [9, Def.4.4.1])
with the formal group law L⟶φA,
there exists a unique morphism of theories A∗↠ANum∗
which is moreover surjective.
Proof:
By [17, Prop. 4.8], the canonical morphism of theories G:A(0)∗↠A∗ is surjective
(this morphism is induced by the canonical morphism Ω∗→A∗ of [9, Thm 1.2.6]).
And by the same universality of algebraic cobordism such morphism is unique. In particular, there is a unique morphism
of theories A(0)∗↠ANum∗.
Note, that G∣Spec(k):A→=A is an isomorphism. Hence, if x∈A(0)∗(X) belongs to the kernel of G,
then x∼Num0. Thus, the unique morphism of theories A(0)∗↠ANum∗ factors through A∗→ANum∗.
□
Thus, ANum∗ plays the role opposite to that of A(0)∗, and can be denoted as A(∞)∗, while any
generically constant theory A∗ with the formal group law φ is canonically squeezed between A(0)∗ and A(∞)∗:
[TABLE]
and the latter provides an alternative way of describing such theories A∗.
4.2 Numerical equivalence modulo p and isotropy
Everywhere below X is a smooth projective variety over a field k of characteristic zero.
In the case of a theory Ch∗=CH∗/p, we will denote the numerical equivalence ∼Num as ∼Num(p)
to stress that we consider finite coefficients. Thus, ChNum∗(X)=Ch∗(X)/N, where
N is the ideal of elements ∼Num(p)0. In our situation, x∈Ch(X) is ∼Num(p)0 if, for any y∈Ch(X), the
deg(x⋅y)=0∈Fp.
By the very definition, we have a non-degenerate pairing
[TABLE]
defined by (x,y)↦deg(x⋅y).
Moreover, since deg(x⋅y) may be defined on the level of the (complex) topological realization,
the kernel of the topological realization functor is contained in N, and so, ChNum(X)
is a sub-quotient of the topological cohomology HTop(X;Fp) of X. In particular,
ChNum(X) is finite-dimensional Fp-vector space. Note, however, that this sub-quotient depends on the
ground field k, since for different fields, the images of the topological realization functor will be different.
The theory ChNum∗ inherits the action of the reduced power operations from Ch∗,
as follows from the Proposition 4.6 below.
Recall, that we have reduced power operations Pi:Ch∗→Ch∗+i(p−1) (see [2] and [21])
commuting with pull-back morphisms, and the respective homological operations Pi:Ch∗→Ch∗−i(p−1) commuting
with push-forwards. These are connected as follows:
[TABLE]
where dl satisfies Cartan’s formula and, for a line bundle L, d1(L)=xp, where x=c1(L).
Proposition 4.6
Let u∈Ch∗(X). Then u∼Num(p)0⇒Pi(u)∼Num(p)0.
Proof: Induction on i. Since P0=id, we have the (base) i=0.
(step) We need to show that deg(Pi(u)⋅v)=0, for any class v of complementary dimension.
By Cartan’s formula, Pi(u)⋅v=Pi(u⋅v)−∑j=0i−1Pj(u)⋅Pi−j(v).
By the inductive assumption, we have that deg(Pj(u)⋅Pi−j(v))=0, for any j<i.
And the degree of the first summand can be rewritten as
[TABLE]
The second summand is zero by the inductive assumption, while the degree of
Pi(u⋅v) is the same as that of Pi(π∗(u⋅v)), where π:X→Spec(k) is the natural projection.
The latter degree is equal to zero for any i>0. The induction step is proven.
□
If x is an anisotropic cycle, then x∼Num(p)0. Indeed, x=f∗(x′), for some projective map f:Z→X from
anisotropic variety Z, and some x′∈Ch∗(Z). But then deg(x⋅y)=deg(f∗(x′)⋅y)=deg(x′⋅f∗(y))=0,
since all zero cycles on Z have zero degree (modulo p). Thus we get the surjective map:
[TABLE]
I conjecture that, over flexible fields, these two cohomology theories, in reality, coincide.
Conjecture 4.7
Let k be a flexible field. Then
Chk/k∗=ChNum∗.
Remark 4.8
The condition on the flexibility of k is essential here. For example, if k is algebraically closed, then
from Remark 2.12 we know that Chk/k∗=Ch∗, while ChNum∗ is some sub-quotient of it.
*
△*
Remark 4.9
This Conjecture, in particular, implies that the local Chow motivic category
Chow(k/k;Fp) is equivalent to the numerical Chow motivic category ChowNum(k;Fp).
Since the degree pairing is defined over the algebraic closure and even in the topological realization, we obtain that the numerical
Chow groups over E are sub-quotients of the respective groups over E, which, in turn, are sub-quotients of topological cohomology:
[TABLE]
Thus, our Conjecture implies, that any object of Chow(k;Fp) which vanishes over k, or even in the topological realization,
should vanish in every isotropic category Chow(E/E;Fp).
In contrast, ”non-pure” motives behave differently. For example, the idempotent, corresponding to the projector
πE:DM(k;Fp)→DM(E/k;Fp) is mapped via ψE to the unit object of the category DM(E/E;Fp).
On the other hand, its restriction to k is trivial, since XQ∣k=0, for any non-empty Q
(note that E=E, since k is flexible, so the respective directed system contains non-empty Q’s).
Consequently, all the subcategories DM(E/k;Fp), for all
finitely-generated E/k, are killed by the restriction to the algebraic closure functor DM(k;Fp)→DM(k;Fp).
There are geometric examples as well: the motive Mα of Section 3 vanishes over k, but
is non-zero in the isotropic motivic category.
*
△*
Remark 4.10
Although, the numerical Chow motivic category ChowNum(k;Fp) is a sub-quotient of a topological category
(that is, of the category of graded Fp-vector spaces), it is more interesting. In particular, it is not generated by a single object (Tate-motive). This is reflected by the absence of the Kunneth formula. Namely, for smooth projective X and Y, the product map
[TABLE]
is not an isomorphism (⇔ not surjective), in general.
*
△*
Our aim is to prove the following result.
Theorem 4.11
The Conjecture 4.7 is true in the following cases:
(1)
dim(X)⩽5;
(2)
Ch1;
(3)
Chm, for m⩽2.
Item (2) will be proven in Proposition 4.15, item (3) follows from Corollary 4.16 and Propositions 4.20 and
4.23, and for the item (1) we need to add Proposition 4.24.
Corollary 4.12
In the situation of Theorem 4.11, the local Chow groups Chk/k∗(X) are finite-dimensional Fp-vector spaces.
This contrasts with the global situation, where Chow groups of varieties are often huge.
We have the following Chow-motivic questions of increasing strength related to Question 2.10.
Question 4.13
(1)
Is it true that any U∈Ob(Chow(k;Fp)) which vanishes in the (complex) topological realization is zero?
(2)
Is it true that any f∈EndChow(k;Fp)(V) which vanishes in the (complex) topological
realization is nilpotent?
As we saw, by Conjecture 4.7, for a flexible
field, the triviality of the topological realization should imply the triviality of all local realizations.
Remark 4.14
Note, that the stronger variant of Question 4.13(2) fails. Namely, C.Soule and C.Voisin produced an example
of a class c∈Ch3(X), for some smooth projective X, such that c vanishes in HTop6(X;Fp), but c is not
smash-nilpotent (that is, c×r=0∈Ch3r(X×r), for any r) - [13, Theorem 5].
If we are interested, instead, only in the triviality of local realizations, it is sufficient to take the image x of any torsion
class x from CH1(X), whose topological realization in HTop2(X;Fp) is non-trivial. Then, since the degree pairing is defined
integrally, x∣E∼Num(p)0, for any E/k. Thus all local realizations of x are trivial by Theorem 4.11(2).
At the same time, its topological realization is non-trivial, and so, not smash-nilpotent. Hence,
x is not smash-nilpotent either.
*
△*
A weaker variant of Question 4.13 with ”topological realization”
replaced by the ”restriction to the algebraic closure” is a safer bet.
In this form, the question (2) becomes the Rost Nilpotence Conjecture.
4.3 The proof of the Main Theorem
4.3.1 Divisors and zero-cycles
We start the proof of Theorem 4.11 with the case of divisors (item (2)), which is, actually, the base for the whole technique.
Proposition 4.15
Let k be a flexible field and u∈Ch1(X) be ∼Num(p)0. Then u=0∈Chk/k1(X).
Proof:
Adding to an effective divisor representing u a p-multiple of a very ample divisor,
we may assume that u is represented by a very ample divisor D.
Let (Pn)∨=Proj∣D∣ be the projective linear system of D. This defines the embedding of X into Pn. From
Statement 6.3,
the embedding ι:Dη→X of the generic representative of our linear system into X induces a surjective map ι∗:Ch1(X)↠Ch0(Dη).
But since D∼Num(p)0, the degree of the zero-cycle ι∗(v) is zero, for any v∈Ch1(X).
Hence, Dη is anisotropic. Thus, over k((Pn)∨), our class u is represented by the class of an
anisotropic divisor Dη.
Since k is flexible, it is represented by an anisotropic class already over k (by Proposition 1.3).
□
Since the theory Chk/k∗ has the structure of push-forwards and pull-backs, we obtain:
Corollary 4.16
Let k be a flexible field.
The projection Ch∗↠Chk/k∗ passes through Chalg∗=Ch(1)∗.
Proof:
A class u∈Ch∗(X) is algebraically equivalent to zero, if it can be presented as f∗(y⋅g∗(v)), where
X⟵fX×C⟶gC are natural projections, C is a smooth projective curve,
y∈Ch∗(X×C) and v∈Ch0(C) is a zero cycle of degree zero. Since v∼Num(p)0, Proposition 4.15
implies that v=0∈Chk/k∗(C), and so, u=0∈Chk/k∗(X).
□
Since any zero-cycle on a smooth projective variety X is a push-forward of some zero-cycle from a curve, we also get the case of zero-cycles.
Corollary 4.17
Let k be a flexible field and u∈Ch0(X) be ∼Num(p)0. Then u=0∈Chk/k;0(X).
Our general strategy of proving that the class u∼Num(p)0 is anisotropic will be to find an appropriate blow-up
π:X→X, so that π∗u may be represented by a cycle supported on a smooth connected divisor Z⊂X,
which is ∼Num(p)0 already on Z. Then we use induction on the dimension of X and the fact that u=π∗π∗u.
In order to achieve this, we will need first to present u by the class of a smooth connected subvariety S,
and make the appropriate characteristic classes of it ∼Num(p)0 on X.
4.3.2 3-folds and 1-cycles
We will be moving up the dimension of varieties.
The above statements settle the case of curves and surfaces. Our
next aim are 3-folds, where only the case of 1-cycles remains open.
Proposition 4.18
Let k be a flexible field and X be a smooth projective variety over k of dimension 3.
Let u∈Ch1(X) be ∼Num(p)0. Then u=0∈Chk/k;1(X).
Proof: We will show that there is a blow-up π:X→X such that π∗(u) is represented by the class of a smooth
anisotropic curve on X. Since π∗π∗(u)=u, this will show that the class u is anisotropic.
Here, as in many statements below, we will be gradually reducing
a general case to the one having better and better special properties.
Lemma 4.18.1
We may assume that u is represented by a class of a smooth curve S on X,
and moreover, deg(c1(NS⊂X)⋅[S])=0(modp).
Proof:
By Corollary 6.2, after some blow-up, we may represent u by the class of a smooth curve S on X (we keep the same name for
the variety).
Note, that c1(NS⊂X)=c1(TX)+c1(−TS) and deg(c1(TX)⋅[S])=0, since [S]∼Num(p)0 and c1(TX) is a
class defined on X.
Now we need to treat separately p=2 and odd primes. Such separate treatment of different primes is the feature which we will see repeatedly below.
(p=2) Our degree is equal to the deg(c1(−TS)⋅[S])=deg(P1([S])), where P1 is the homological
Steenrod operation Sq2. But deg(P1([S]))=deg(P1(ε∗[S])), where ε:S→Spec(k) is the projection, and ε∗[S]=0.
(p=2) Let [Z] be a smooth very ample divisor on S representing 21c1(−TS) in Ch0(S).
Let π:X→X be the blow-up of X at Z. Let S be the proper pre-image of S in X.
Then by [5, Thm 6.7], we have:
[TABLE]
where [PZ1] is the class supported on the special divisor PZ2.
And so, π∗([S]) is represented by the class of a smooth curve S′=S∐PZ1 (we can always choose the curve PZ1 not
intersecting S).
Note, that S≅S. Then
[TABLE]
□
Now, we can make our class to be, in addition, supported on
some smooth surface.
Lemma 4.18.2
We may assume that u is represented by the class of a smooth (possibly, disconnected) curve S which is contained in some smooth
(possibly, disconnected) surface E on X, and the curve S satisfies also: deg(c1(NS⊂X)⋅[S])=0.
Proof:
By Lemma 4.18.1, we can assume that u=[S], where S⊂X is a smooth curve, and moreover,
deg(c1(NS⊂X)⋅[S])=0.
Consider X=BlS(X) with the
projection π:X→X. Then π∗(u) is supported on E=PS(NS⊂X), which is a smooth surface.
More precisely, it is represented by ρ+ε∗(c1(NS⊂X)), where ε:E→S is the natural projection
and ρ=c1(O(1))=−[E].
By adding a p-multiple of a very ample divisor, we can assume (by Statement 6.4) that π∗(u)
is represented by a very ample divisor on every
component of E, and so, is represented by a smooth curve S′ on E. Moreover, c1(NS′⊂X) is
the restriction of ε∗(c1(NS⊂X)) to S′. Hence, deg(c1(NS′⊂X)⋅[S′])=deg(c1(NS⊂X)⋅ε∗([S′]))=deg(c1(NS⊂X)⋅[S])=0.
a □
In view of Corollary 6.12, it remains to make our curve and surface connected.
Lemma 4.18.3
We may assume that u is represented by the class of a smooth connected curve contained in a smooth connected divisor E on X,
and the curve S satisfies also: deg(c1(NS⊂X)⋅[S])=0.
Proof:
By Lemma 4.18.2 we may assume that u=[S], where S is smooth and S⊂E′⊂X, where E′ is a (possibly, disconnected)
smooth surface and deg(c1(−TS)⋅[S])=deg(c1(NS⊂X)⋅[S])=0.
By Statement 6.5 applied to the divisor E′ considered as a single component,
over some purely transcendental extension of k, there is an irreducible divisor E′′ on X,
containing S and smooth outside an anisotropic subset.
Since k is flexible, we may assume that the divisor E′′ of X is defined already over k.
Let π:X→X be the embedded desingularization of E′′.
Let E be the proper pre-image of E′′ and Y be the proper pre-image of S. Then π∗(u) is equal to [S] plus
some classes supported on the special divisors of our blow-up. But these special divisors are anisotropic (since the singularities were).
Hence, modulo anisotropic classes, π∗(u) is equal to the class [S] supported on a smooth connected surface E.
And since S≅S, we have deg(c1(−TS)⋅[S])=deg(c1(−TS)⋅[S])=0.
Our class is a divisor on E. Adding a p-multiple of an appropriate very ample divisor,
we may assume that our divisor is very ample (by Statement 6.4),
and so, is represented by a smooth connected curve on E. Note, that this procedure doesn’t change the
deg(c1(−TS)⋅[S])=0∈Fp.
□
Proposition 4.18 follows now from Corollary 6.12 and flexibility of k.
□
Now, the case of varieties of dimension ⩽3 is settled,
which, due to the presence of push-forwards and pull-backs,
implies that isotropic Chow groups factor through the second theory of higher type.
Proposition 4.19
Let k be a flexible field. The projection Ch∗↠Chk/k∗ factors through Ch(2)∗.
Proof:
A class u∈Ch∗(X) is =0∈Ch(2)∗, if it can be presented as f∗(y⋅g∗(v)), where
X⟵fX×Q⟶gQ are natural projections, Q is a smooth projective variety of dimension 3,
y∈Ch∗(X×Q) and v∈Ch∗(Q) is ∼Num(p)0. Then, by Proposition 4.15, Corollary 4.17 and Proposition 4.18,
v=0∈Chk/k∗(Q), and so, u=0∈Chk/k∗(X).
□
The case of surfaces and 3-folds permits to start induction and deal with 1-cycles on a variety of an arbitrary dimension.
Proposition 4.20
Let k be a flexible field and X be a smooth projective variety over k.
Let u∈Ch1(X) be ∼Num(p)0. Then u=0∈Chk/k;1(X).
Proof:
Induction on n=dim(X).
(base) The case n=1 is trivial. The cases n=2 and n=3 follow from Propositions 4.15 and 4.18, respectively.
(step (n−1)→(n)) We may assume that n>3.
First of all, we need to make our class supported
on a smooth divisor.
Lemma 4.20.1
We may assume that u is represented by a class supported on some smooth
(possibly, disconnected) divisor Z on X.
Proof:
By Corollary 6.2, we may assume that u is represented by the class of a smooth curve S on X.
Consider the blow-up π:X=BlS(X)⟶X. Then π∗(u) is supported on the special divisor
E=PS(NS⊂X) which is smooth.
□
Now we can make the supporting (smooth) divisor connected and,
in addition, can make all co-dimension 1 classes on it restrictions of some classes from X, at least, modulo anisotropic classes.
Lemma 4.20.2
We may assume that u is represented by a class supported on some smooth
connected divisor Z on X such that the restriction Chk/k1(X)↠Chk/k1(Z)
is surjective.
Proof:
By Lemma 4.20.1, we may assume that u is represented by the class of a curve S contained in a smooth divisor Z.
By Statement 6.5 and flexibility of k, S is contained in some irreducible divisor Z′,
smooth outside an anisotropic subset, and such that the restriction
Chk/k1(X)↠Chk/k1(Z′\S) is surjective.
Since dim(Z′)−1>1=dim(S), we also get the surjection Chk/k1(X)↠Chk/k1(Z′).
Let π:X→X be the embedded resolution of singularities of Z′. Since the singularities of Z′ were anisotropic, so will be the
special divisors of X. Let Z′ be the proper pre-image of Z′ and S be the proper pre-image of S.
Then Chk/k∗(Z′)=Chk/k∗(Z′), and so,
the map f∗:Chk/k1(X)↠Chk/k1(Z′), induced by the natural projection f:Z′→X, is surjective.
The image of π∗(u) in Chk/k∗(X)=Chk/k∗(X)
is represented by the class of S supported on Z′.
□
Since the restriction, j∗:Chk/k1(X)↠Chk/k1(Z) is surjective, u=j∗(u′), for some class
u′∈Chk/k;1(Z), and u∼Num(p)0 on X, we get that u′∼Num(p)0 on Z.
As Z is smooth connected projective variety of dimension n−1,
by the inductive assumption, u′=0∈Chk/k;1(Z). Then the class u is equal to 0∈Chk/k;1(X) as well.
Proposition 4.20 is proven.
□
4.3.3 4-folds
The next target is 4-folds, where only the case of co-dimension 2 cycles is left.
Proposition 4.21
Let k be a flexible field and X be a smooth projective k-variety of dimension 4.
If u∈Ch2(X) is ∼Num(p)0, then u=0∈Chk/k2(X).
Proof:
Our strategy will be to find an appropriate blow-up π:X→X such that π∗(u) is supported on some smooth connected
divisor Z and is ∼Num(p)0 on it.
By Corollary 6.2, we may assume that u is represented by the class of a union of smooth complete intersections of very ample divisors with components meeting transversally.
In such a situation (of transversal smooth components), let us denote as c12(NS⊂X)⋅[S] the sum
∑ic12(NSi⊂X)⋅[Si], and similar for other characteristic classes.
The case of a prime 2 requires certain preparations to be made
still at this level of transversal complete intersections, before passing to a single smooth subvariety (to be done in the next step).
Lemma 4.21.1
We may assume that u is represented by the class of ∪iSi, where each Si is a complete intersection of very ample divisors,
with components meeting transversally. For p=2, we may moreover assume that deg(c12(NS⊂X)⋅[S])=0.
Proof:
Let p=2 and [S]=∑ixiyi, where xi and yi are classes of very ample divisors. Then, in Ch2, we can substitute
this presentation by
[TABLE]
where all the divisor classes involved are very ample, and so, components can be made transversal.
Then c12(NS′⊂X)⋅[S′]=∑i(xiyi(xi+yi)2+xi(xi+yi)yi2+yi(xi+yi)xi2+0)=0.
□
For a surface S=∪iSi with smooth transversal components, let us denote Λ2[S]:=∑{i,j}[Si]⋅[Sj]
in Ch0(X), where the sum is over all 2-element subsets of the set of components.
The following result permits to combine our transversal components into a single smooth connected surface. Moreover, there is some control over the characteristic classes of the surface obtained
this way.
Lemma 4.21.2
Let S=∪iSi be a surface on X with smooth transversal components. Then there exists a blow-up η:X^→X
such that η∗([S]) is represented by the class of a smooth connected surface S^
contained in a smooth connected divisor Z^, and
deg(c12(NS^⊂X^)⋅[S^])=deg(c12(NS⊂X)⋅[S]−2Λ2([S])).
If, moreover, [S]∼Num(p)0, then this degree is equal to the deg((c12+c2)(NS⊂X)⋅[S]).
Proof:
Let u=[∪iSi]=∑iui be the class of [S].
Let π:X→X be the blow-up of X in all components Si. Let Ei be the respective components of the special divisor
and ρi=c1(O(1)i)=[−Ei]. Then, by [16, Prop. 5.27], ui=π∗([Si])=[Ei]⋅(c1(NSi⊂X)+ρi)
is supported on Ei and may be represented by a smooth surface Si. Note, that
c1(NSi⊂X)=π∗(c1(NSi⊂X)), and so,
deg(c12(NS⊂X)⋅[S])=deg(c12(NS⊂X)⋅[S]).
Let Ti,j=Ei∩Ej be
the intersection of the components of the special divisor, and ti,j=[Ti,j]. We have:
deg(ui⋅uj)=deg(ui⋅uj), while deg(ui⋅ti,j)=deg(−[Ei]3⋅[Ej])=0
and deg(ui⋅tj,k)=0, for any i∈{j,k}, as well. Finally,
deg(ti,j2)=deg([Ti,j]⋅ρi⋅ρj)=deg(ui⋅uj), while ti,j⋅tk,l=0, for {i,j}={k,l}.
Now, for all pairs (i,j) of distinct numbers let us choose signs ε(i,j)∈±1 with the condition that
ε(i,j)+ε(j,i)=0. Let us substitute classes ui by ui′:=ui+∑j=iε(i,j)ti,j.
Note, that the sum ∑iui′ is still equal to the ∑iui=π∗(u).
On the other hand,
[TABLE]
Since these classes ui′ are divisors on (connected) Ei, we can make them very ample (by adding a p-multiple of some
very ample divisor) and so, can move them around and make them smooth connected and transversal to any given subvariety.
Let Si′ be the generic representative of the respective linear system ∣ui′∣ on Ei. It is a
smooth connected surface on Ei representing ui′.
We now have a divisor with
strict normal crossings E=∪iEi and a surface S′=∪iSi′ on it, with Si′ smooth connected,
transversal to each other and to the other components of E.
Since deg(ui′⋅uj′)=0, for i=j, by the arguments of the proof of Proposition 4.15,
all the intersections Si′∩Sj′ are anisotropic.
Since k is flexible, we may assume that Si′ is defined already over k (by Proposition 1.3).
Finally, denoting γi=π∗(c1(NSi⊂X)),
since ρiρjγi, ρiρj3, ρiρjρk are zero, for distinct i,j,k, we have
[TABLE]
If [S]∼Num(p)0, then deg(2Λ2([S]))=deg([S]⋅[S]−∑i[Si]⋅[Si])=−deg(c2(NS⊂X)⋅[S]).
Thus, in this case,
deg(c12(NS⊂X)⋅[S]−2Λ2([S]))=deg((c12+c2)(NS⊂X)⋅[S]).
After all, we managed to present our cycle by the class of the union of smooth surfaces transversal to each other and all intersections
anisotropic.
It remains to use Statement 6.6.
□
In order to apply Corollary 6.12, we need to eliminate (numerically) the powers of the 1-st Chern class of the normal bundle of our surface. We will proceed from highest to smallest powers.
Lemma 4.21.3
We may assume that u is represented by the class of a smooth connected surface S which is contained in a smooth connected
divisor Z, and deg(c12(NS⊂X)⋅[S])=0∈Fp.
Proof:
By Lemmas 4.21.1 and 4.21.2,
we may assume that u is represented by the class of a smooth connected surface S contained in a smooth connected divisor Z, and
(again by the same Lemmas) we already know the case (p=2).
We need to treat separately p=3 and the remaining primes.
(p=3) Let d1=c12+c2. This characteristic class of degree 2 corresponds to the reduced power operation
P1:Chr→Chr+2. Namely, P1([S])=d1(NS⊂X)⋅[S]. By Proposition 4.6,
deg(d1(NS⊂X)⋅[S])=0∈F3, since [S]∼Num(p)0.
On the other hand, deg(c2(NS⊂X)⋅[S])=deg([S]⋅[S])=0 (by the same reason).
Hence, deg(c12(NS⊂X)⋅[S])=0∈F3.
(p=2,3) Let R be a smooth zero-cycle representing the complete intersection (of very ample divisors)
21c1(NS⊂X)⋅31c1(NS⊂X) on S.
Let π:X=BlR(X)→X be the blow-up of X at R,
and E→εS be the special divisor of π, with ρ=c1(O(1))=−[E].
Then π∗([S])=[S]+[F], where S is the proper transform of S, and
[F]=[E]⋅(ε∗(c1(NS⊂X))+ρ).
We have: c1(NS⊂X)=2ρ+πS∗(c1(NS⊂X)), while c1(NF⊂X)=ε∗(c1(NS⊂X)).
Hence, (taking into account that π(E) is zero-dimensional),
[TABLE]
where S⟵πSS⟶jX are natural maps.
On the other hand,
[TABLE]
By Lemma 4.21.2, there exists a blow-up μ:X→X, such that μ∗π∗([S])∈Chk/k2(X)
is represented by a smooth connected
surface S contained in a smooth connected divisor Z with
[TABLE]
□
It remains to treat the first power of the 1-st Chern class.
Lemma 4.21.4
We may assume that u is represented by the class of a smooth connected surface S which is contained in a smooth connected
divisor Z, with c12(NS⊂X)⋅[S]∼Num(p)0 and c1(NS⊂X)⋅[S]∼Num(p)0.
Proof:
By Lemma 4.21.3, we may assume that u=[S], where S⊂Z⊂X are smooth connected, with the needed condition on c12.
It remains to terminate c1. We need to treat separately p=2 and larger primes.
(p=2) The characteristic class c1 corresponds to the reduced power operation P1:Chr→Chr+1 (modulo 2).
Since [S]∼Num(p)0, by Proposition 4.6, c1(NS⊂X)⋅[S]=P1([S])∼Num(p)0.
(p=2) Let R be a smooth connected curve on S representing 21c1(NS⊂X)⋅[S].
Let π:X=BlR(X)→X be the blow-up at R, with the (connected) special divisor
E→εS and ρ=c1(O(1))=−[E].
Then π∗([S])=[S]+[F], where S is the proper pre-image of S, and
[F]=[E]⋅(ε∗(c1(NS⊂X))+ρ) is supported on E. Note, that πS:S→S is an isomorphism.
Then
[TABLE]
since ρ+πS∗(21c1(NS⊂X))=0 on S.
Since c12(NS⊂X)⋅[S]∼Num(p)0 on X, and R is connected, we have that c1(NS⊂X)⋅R∼Num(p)0 on R,
which implies that [E]⋅ε∗(c1(NS⊂X))∼Num(p)0 on E. Hence,
[TABLE]
Finally, [S]⋅[F]=[S]⋅(−ρ)⋅(πS∗(c1(NS⊂X))+ρ)=[S]⋅πS∗(21c1(NS⊂X))⋅πS∗(21c1(NS⊂X))∼Num(p)0 on S, since
c12(NS⊂X)⋅[S]∼Num(p)0 on S.
Substituting F by the generic representative of the (very ample) linear system ∣F∣ on E, by the proof of Proposition 4.15,
we may assume that the intersection S∩F is anisotropic. Then, by Statement 6.6, there exists a blow-up
μ:X→X such that μ∗π∗([S]) is represented by the class of a smooth connected surface S contained in a smooth
connected divisor Z, and such that c1m(NS⊂X)⋅[S]∼Num(p)μ∗(c1m(NS⊂X)⋅[S]+c1m(NF⊂X)⋅[F])∼Num(p)0, for m⩾0.
□
Now Proposition 4.21 follows from Corollary 6.12 and flexibility of k.
□
4.3.4 2-cycles
The case of 4-folds is completed. Our next destination is 2-cycles. The main difficulty here is the case of 2-cycles on a 5-fold, which (together with the treated 4-folds) will form a base
of our induction.
Proposition 4.22
Let k be a flexible field and X be a smooth projective k-variety of dimension 5.
If u∈Ch2(X) is ∼Num(p)0, then u=0∈Chk/k;2(X).
Proof:
The strategy, as usual, is to find an appropriate blow-up, so that the pull-back of u is supported on some smooth connected
divisor Z and is ∼Num(p)0 already on Z.
We start by presenting u by the class of a disjoint union of smooth complete intersections and eliminating numerically its
2-nd (normal) Chern class.
Lemma 4.22.1
We may assume that u is represented by the class of a smooth surface S on X, with all components complete intersections and
deg(c2(NS⊂X)⋅[S])=0∈Fp.
Proof:
By Corollary 6.2, we may assume that u is represented by the class of a disjoint union of smooth complete intersections:
u=[S]=[∐iSi]. We need to treat separately the case p=2 and that of odd primes.
(p=2)
The characteristic class c2 corresponds to the reduced power operation P2 (modulo 2), that is,
P2([S])=c2(NS⊂X)⋅[S]. But [S]∼Num(p)0, and so, by Proposition 4.6, P2([S])∼Num(p)0 too.
Hence, deg(c2(NS⊂X)⋅[S])=0∈F2.
(p=2) If the degrees of c2 of all the components are trivial, there is nothing to prove.
Otherwise, there is a component Sl given by x1x2x3 such that deg(x12x22x3)=r=0∈Fp.
Let R be a disjoint union of d copies of the curve x12x22, where one factor of x1 and x2 here is the same as in Sl
and the other one is generic, so that Q=R∩Sl is given by the d disjoint copies of x12x22x3 and R doesn’t meet
other components of S. Let π:X→X be the blow-up at R with the special divisor E and ρ=c1(O(1))=−[E].
Then, by [5, Thm 6.7], π∗([Sl])=[Sl]+[V], where Sl⟶πSSl is the proper transform of Sl and
V=PQ2 is a subvariety of the Q-fiber of the P3-bundle E→R. Here
Sl is a complete intersection (x1+ρ)(x2+ρ)x3, while V is a complete intersection −ρ2⋅x3.
We can move [Q] along R and make V disjoint from Sl (it is automatically disjoint from other components).
On Sl, xi⋅ρ=0 (since πS(S∩E) is zero-dimensional) and ρ2=−πS∗[Q], while on V=PQ2, xi=0 and ρ2 is the class of a section
Q→PQ2.
Hence, the
[TABLE]
Since p=2, by choosing d appropriately, we can always make the total degree of c2(NS⊂X)⋅[S] to be zero
(in Fp), while keeping all the components complete intersections.
□
Having made the 2-nd (normal) Chern
class of our surface numerically trivial,
now we will do the same with
every connected component of it. This will make the mentioned
Chern class numerically trivial already on the surface itself
(not just after the push-forward to X).
Lemma 4.22.2
We may assume that u is represented by the class of a smooth surface S on X, and for each component Sl of S, we have
deg(c2(NSl⊂X)⋅[Sl])=0∈Fp.
Proof:
By Lemma 4.22.1, we may assume that u is represented by the class of a disjoint union of smooth complete intersections:
u=[S]=[∐lSl] with deg(c2(NS⊂X)⋅[S])=0.
Let Sl be represented by the intersection x1x2x3 of very ample divisors.
Let R{i,j}⊂X be the complete intersection xi2xj2, where one copy of xi and xj is the same as in Sl,
but the other copy is generic, so that R{i,j} meets Sl at a zero-cycle xi2xj2xm (where {m}={1,2,3}\{i,j}),
and doesn’t meet other components of S. Let R=∐{i,j}∈(23)R{i,j} (we can make components disjoint).
Note, that [R∩Sl] represents the class c2(NSl⊂X) on Sl.
Let π:X→X be the blow-up at R, where
E{i,j}⟶π{i,j}R{i,j} are the components of the special divisor,
ρ{i,j}=−[E{i,j}] and ρ=∑{i,j}ρ{i,j}.
Let Sl⟶πSSl be the proper transform of Sl.
The Chern roots of NSl⊂X are
xi+∑j=iρ{i,j},i=1,2,3.
Moreover, Sl is still a complete intersection: [Sl]=∏i(xi+∑j=iρ{i,j}),
and on Sl we have identities: xi⋅ρ{j,k}=0, while ρ{i,j}2=−πS∗[R{i,j}∩Sl] and
ρ{i,j}⋅ρ{i′,j′}=0, for {i,j}={i′,j′}. Then, on Sl,
[TABLE]
Let Q{i,j}=Sl∩R{i,j}.
By [5, Thm 6.7], π∗([Sl])=[Sl]+[V], where
V=∐{i,j}∈(23)[V{i,j}],
V{i,j}=PQ{i,j}2 given by ρ⋅π{i,j}−1(Q{i,j}) and contained in the P3-bundle
E{i,j}→R{i,j} is a complete intersection −ρ{i,j}2xm (m as above). We can move the class [Q{i,j}]
along R{i,j}, and so can make PQ{i,j}2 disjoint from Sl (and it is automatically disjoint from the other components of S).
The Chern roots of NV⊂X are −ρ,0,ρ, and so,
[TABLE]
Let P{i,j} be the (p−1) (disjoint) copies of PQ{i,j}1 contained in π{i,j}−1(Q{i,j}), but not in
PQ{i,j}2. Let P=∐{i,j}P{i,j} and μ:X→X be the blow-up at P. Let
G=∐{i,j}G{i,j} be the special
divisor of μ, with projections μ{i,j}:G{i,j}→P{i,j} and α=c1(O(1))=−[G].
Let V{i,j} be the proper transform of V{i,j}, and
F{i,j}=μ{i,j}−1(PQ{i,j}2∩P{i,j})⋅α (which is isomorphic to the disjoint union of
(p−1) copies of PQ{i,j}2) whose class
is given by −α⋅α⋅ρ{i,j}. Let F=∐{i,j}F{i,j}.
By [5, Thm 6.7], μ∗([V{i,j}])=[V{i,j}]+[F{i,j}].
The Chern roots of
NV{i,j}⊂X are α−ρ,α,ρ. Hence,
[TABLE]
where q is the class of a section Q{i,j}→V{i,j}=PQ{i,j}2.
The Chern roots of NF{i,j}⊂X are −α,α,0. So, the
deg(c2(NF⊂X)⋅[F])=deg(−α2⋅[F])=−(p−1)∑{i,j}deg([Q{i,j}])=deg(c2(NSl⊂X)⋅[Sl]).
Let us apply the above construction to every component Sl of S, and denote the respective objects by the subscript l.
Now, after applying μ∗π∗, the degree of c2(NS⊂X)⋅[S] is concentrated in the F-components, where
[Fl] is given by −αl⋅αl⋅ρl. Then [F]=∑l(−αl⋅αl⋅ρl).
But since ρl⋅αk=0, and αl⋅αk=0, for l=k, this can be rewritten as
−α⋅α⋅ρ, where α=∑lαl and ρ=∑lρl.
We can substitute −α, α and ρ by very ample divisors and represent [F] by (the class of)
a smooth connected surface with the same deg(c2(NF⊂X)⋅[F]), not meeting other components of S.
Now, the whole degree of c2(NS⊂X)⋅[S] is concentrated in a single component F. But, by Lemma 4.22.1,
this total degree is zero.
Now we can finish the proof of Proposition 4.22.
By Lemma 4.22.2, we may assume that u is represented by the class of a smooth surface S with
c2(NS⊂X)∼Num(p)0 on S.
Let π:X→X be the blow-up at S, with the special divisor E⟶πES and ρ=c1(O(1))=−[E].
Let c1=πE∗c1(NS⊂X). By [5, Prop. 6.7], π∗([S])=(ρ2+c1ρ)⋅[E] in Chk/k∗(X),
since c2(NS⊂X)∼Num(p)0 on S (and by Corollary 4.17).
Being a complete intersection on E, this class may be represented by a smooth surface
S on E. Note also, that ρ(ρ2+c1ρ)⋅[E]=0 and that the Chern roots of NSi⊂X are
−ρ,ρ,ρ+c1, and so, the deg(c2(NSi⊂X)⋅[Si]) is still zero.
By Statement 6.5 and flexibility of k,
there is an irreducible divisor Z, containing S, smooth outside an anisotropic closed
subscheme of S, and such that the restriction Ch∗(X)↠Ch∗(Z\S) is surjective.
Let μ:X→X be the embedded desingularization of Z and S (note, that we may assume that no component of
S belongs to the singular locus of Z, since this locus is anisotropic). Let Z and S be the proper pre-image of Z
and S, respectively. Then, Z is smooth connected and, modulo anisotropic classes, μ∗([S]) is represented by
[S] supported on Z. Since the maps Z\S⟵Z\μ−1(S)⟶Z\S
induce isomorphisms Chk/k∗(Z\S)→=Chk/k∗(Z\μ−1(S))←=Chk/k∗(Z\S), we obtain that the group Chk/k2(Z) is generated by the image
of j∗:Chk/k2(X)→Chk/k2(Z) and the classes [Si] of all the connected components of S.
Since S∼Num(p)0 on X, the image of j∗ is orthogonal to [S] on Z. Finally, on Z
[TABLE]
since c2(NSi⊂X)=c2(NSi⊂Z)+c1(NSi⊂Z)⋅c1(NZ⊂X),
where
c1(NZ⊂X)=μ∗c1(NE⊂X)=−μ∗ρ∈Chk/k1(X) (since S coincides with S,
Z coincides with Z and X coincides with X modulo anisotropic subvarieties) and ρ⋅[Si]=0∈Ch∗(X).
Hence, [S]∼Num(p)0 on Z. By Proposition 4.21, the class [S] is represented by an anisotropic subvariety
on Z, and so, on X. Proposition 4.22 is proven.
□
Having treated 2-cycles on 4 and 5-folds, now the general case
follows by an easy induction.
Proposition 4.23
Let k be a flexible field and X be a smooth projective k-variety.
If u∈Ch2(X) is ∼Num(p)0, then u=0∈Chk/k;2(X).
Proof:
Induction on n=dim(X).
The case n=2 is trivial, while the cases n=3,4,5 are covered by Propositions 4.15, 4.21 and 4.22, respectively.
This gives the base of induction.
(step) Let dim(X)>5. By Corollary 6.2, we may assume that u is represented by a class of a smooth
(possibly, disconnected) surface S on X. Let π:X→X be the blow-up at S, with the special divisor E.
Then π∗(u) has support on a smooth divisor E, and is represented there by a class of some surface S′ (possibly, non-smooth).
By Statement 6.5 and flexibility of k,
there is an irreducible divisor Z, containing S′, smooth outside an anisotropic closed
subscheme of S′, and such that the restriction Ch∗(X)↠Ch∗(Z\S′) is surjective.
Let μ:X→X be the embedded resolution of singularities of Z, with Z and S - the proper transforms
of Z and S′, respectively. Then Z is a smooth connected divisor on X and μ∗([S′]) is represented by
[S]∈Chk/k∗(X) supported on Z (since the remaining ingredients are anisotropic).
Since Z, respectively, S,
coincides with Z, respectively, S′, modulo anisotropic subvarieties, the restriction
Chk/k2(X)↠Chk/k2(Z\S)=Chk/k2(Z) is surjective
(note, that dim(Z)⩾5). But [S]∼Num(p)0 on X, hence, it is ∼Num(p)0 on Z as well.
By inductive assumption, [S] is represented by the class of an anisotropic surface on Z, and so, on X.
Induction step and Proposition 4.23 are proven.
□
4.3.5 Co-dimension 2 cycles on a 5-fold
The last remaining case of Theorem
4.11 is that of the co-dimension 2 cycles
on a 5-fold.
This is, by far, the hardest one, which will require various new tools and extensive computations.
Proposition 4.24
Let k be a flexible field and X be a smooth projective variety of dimension 5. If
u∈Ch2(X) is ∼Num(p)0, then u=0∈Chk/k2(X).
Proof:
By Corollary 6.2, we may assume that u is represented by the class [S]=∑ixiyi, where xi,yi are classes of very ample
divisors. In particular, all the components of S are smooth and transversal to each other.
We start by eliminating (numerically) certain zero-dimensional characteristic classes of S. This needs to be done still
at the level of the union of complete intersections (before passing to a single component). In the case of a prime 2, we
also need to make numerically trivial the square of the
1-st Chern class of S at this stage.
Lemma 4.24.1
We may assume that u is represented by the class [S], where components of S are smooth complete intersections
transversal to each other, with
c13(NS⊂X)⋅[S]∼Num(p)0 and c1c2(NS⊂X)⋅[S]∼Num(p)0 on X. For p=2, we may assume, in addition,
that c12(NS⊂X)⋅[S]∼Num(p)0 on X.
Proof:
We need to treat separately the case p=2 and that of odd primes.
(p=2) Replace [S]=∑ixiyi by
[S′]=∑i(xiyi+(xi+yi)xi+(xi+yi)yi+(xi+yi)(xi+yi)).
Then
[TABLE]
On the other hand, (c13+c1c2)(NS′⊂X)⋅[S′]=P2P1([S′]), where Pl is the reduced power operation (modulo 2).
By Proposition 4.6, since [S′]∼Num(p)0 on X, so is P2P1([S′]). Thus, c1c2(NS′⊂X)⋅[S′]∼Num(p)0 on X.
Finally,
[TABLE]
(p=2)
In the case of an odd prime, we need to complement the above method with blowing certain zero-cycles on S. This keeps the result in the form of a union of complete intersections, while
modifying the degrees of the needed zero-dimenional Chern classes. How exactly it does it is described by the following result.
Sublemma 4.24.1.1
Let π:X→X be a blow-up at a smooth point of degree 1 on S. Then
π∗([S]) may be represented by the class of S′, where the components of S′ are smooth complete intersections
(transversal to each other), and
deg(c1c2(NS′⊂X)⋅[S′])=deg(c1c2(NS⊂X)⋅[S])−2, while
deg(c13(NS′⊂X)⋅[S′])=deg(c13(NS⊂X)⋅[S])−8.
Proof:
Clearly, we may assume that S consists of a single smooth complete intersection. Let E=P4 be the special divisor of
π and ρ=c1(O(1))=−[E].
By [5, Thm 6.7], π∗([S])=[S]+[F], where S is the proper transform of S and F=P3 is a divisor on E given by
ρ. We can make S and F transversal. If [S]=xy, then S is a complete intersection (x+ρ)(y+ρ), and F is a
complete intersection −ρ⋅ρ. On S we have:
ρ⋅x=ρ⋅y=0, while ρ3 is the minus class of a point. Then
[TABLE]
Similarly,
[TABLE]
□
Denote as c13 the deg(c13(NS⊂X)⋅[S]) and similar for c1c2.
For [S]=∑ixiyi, let us denote [Sexp]=∑i(xiyi−(xi+yi)xi−(xi+yi)yi+(xi+yi)(xi+yi)),
which represents the same class.
This operation affects the degrees of Chern classes as follows.
Sublemma 4.24.1.2
The substitution of [S] by [Sexp] acts on characteristic numbers as follows:
[TABLE]
Proof:
It is sufficient to treat the case of a single complete intersection [S]=xy. Then
[TABLE]
□
Now we can combine both methods.
Substituting S by Sexp and blowing up the zero-cycles 25c13(NS⊂X) and 21c1c2(NS⊂X)
on it (note, that p=2), we obtain [S′′]=π∗([S]) such that all the components of S′′ are still smooth complete intersections
transversal to each other, and by Sublemma 4.24.1.1,
[TABLE]
Applying this procedure twice, we obtain c13=0 and c1c2=0.
Lemma 4.24.1 is proven.
□
The next step is to make S into a single connected component. This will be possible due to the preparations we made
(trivial zero-dimensional Chern classes).
Lemma 4.24.2
We may assume that S is smooth connected with c13(NS⊂X)⋅[S]∼Num(p)0,
c1c2(NS⊂X)⋅[S]∼Num(p)0. For p=2, we may assume, in addition, that c12(NS⊂X)⋅[S]∼Num(p)0
Proof:
By Lemma 4.24.1 we may assume that S=∪iSi consists of smooth transversal complete intersections and the needed
conditions on the characteristic classes are satisfied.
Let π:X→X be the blow-up at all intersections Si∩Sj, i=j.
Let E{i,j}⟶π{i,j}Si∩Sj be the respective component of the special divisor, ρ{i,j}=−[E{i,j}] and ρ=∑{i,j}ρ{i,j}.
By [5, Thm 6.7], π∗([S])=[S]+[F]+[G], where S=∐iSi is the proper transform of S,
while F=∐{i,j}F{i,j} where
[TABLE]
Let S′=S∪F∪G. Here ρ{i,j} satisfies:
ρ{i,j}4+ρ{i,j}3(xi+yi+xj+yj)+xiyixjyj=0, where [Sk]=xkyk.
Of course, one can get rid of the G-term by considering
[TABLE]
This will work for odd primes. But for p=2, this term really makes a difference.
The following result computes the degrees of characteristic
classes of S, F, G and their intersections in terms
of those of S.
Proof:
Let ρi=∑j=iρ{i,j}. The Chern roots of Si are ρi+xi,ρi+yi, while the Chern roots
of F{i,j} are −ρ{i,j},ρ{i,j}+xi+yi+xj+yj. Denote: ai=xi+yi, bi=xiyi, and a{i,j}=ai+aj,
b{i,j}=bibj.
Using the equation for ρ{i,j}
and the fact that ρ{i,j}, multiplied by any monomial of degree ⩾2 in x and y’s, is zero, we get:
[TABLE]
since ∑jxjyj=[S]∼Num(p)0 on X. Analogously,
[TABLE]
again, since [S]∼Num(p)0 on X. Using the same properties, we obtain:
[TABLE]
Clearly, deg(c13(NG⊂X)⋅[G])=0 and deg(c1c2(NG⊂X)⋅[G])=0, since
c1(NG⊂X)=0.
As a result, deg(c13(NS′⊂X)⋅[S′])=deg((c13+4c1c2)(NS⊂X)⋅[S]).
Finally, deg(c1(NS⊂X)⋅[S]⋅[F])=
[TABLE]
[TABLE]
□
For the prime 2 we also need to control the square of the 1-st Chern class of S.
Sublemma 4.24.2.2
For p=2, we have:
[TABLE]
Proof:
Using the fact that the centers of the blow-up π were 1-dimensional, we obtain:
[TABLE]
□
We may assume that our class is represented by the class of S′=S∪F∪G, where S, F and G
are smooth (possibly, disconnected)
and transversal to each other (note, that we don’t have triple intersections of Si’s),
and [G]=(−ρ)⋅ρ, for some divisor ρ.
Moreover, both S and F have trivial c13 and c1c2 characteristic numbers and
deg(c1(NS⊂X)⋅[S∩F])=0 and deg(c1(NF⊂X)⋅[S∩F])=0.
Since components of S, respectively F, are disjoint,
by Statement 6.6, there exists a blow-up μ:X→X such that μ∗([S]) and μ∗([F]) are
represented by the classes [S] and [F] of smooth connected transversal subvarieties, such that
S∩F is connected, with trivial c13 and c1c2 characteristic numbers for both S and F and
with deg(c1(NS⊂X)⋅[S∩F])=0 and deg(c1(NF⊂X)⋅[S∩F])=0.
For p=2, we have, in addition, c12(NS⊂X)⋅[S]∼Num(p)0 and
c12(NF⊂X)⋅[F]∼Num(p)0.
As a next step, we will combine S∪F into a single component. We start with the following general statement about co-dimension 2 subvarieties on a variaty of an arbitrary dimension.
Sublemma 4.24.2.3
Let Y=∪iYi be a divisor with strict normal crossings on X such that Yi’s and all the intersections
Y{i,j}=Yi∩Yj, for i=j, are connected.
Let S=∪iSi be a union of smooth transversal components, where Si⊂Yi are divisors.
Suppose, that [Si∩Sj]∼Num(p)0 on Y{i,j}. Then [S]=[S′], where S′=∪iSi′, with Si′⊂Yi smooth connected
and transversal to each other, and all the intersections Si′∩Sj′ anisotropic.
This procedure doesn’t change the characteristic classes of NS⊂X in Ch∗(X).
Proof:
Adding to Si a p-multiple of a very ample divisor on Yi, we may assume that Si is given by a very ample divisor on Yi
(this doesn’t change the characteristic classes (mod p)). Let Si′ be the generic representative of the linear system ∣Si∣.
Then Si′ is connected and, by Statement 6.3, the restriction
Ch2(Yi∩Yj)↠Ch0(Si′∩Sj′) is surjective.
This implies that Si′∩Sj′ is anisotropic, since [Si∩Sj]∼Num(p)0 on Yi∩Yj. Since [Si′→Yi] is cobordant
to [Si→Yi] in Ω∗(Yi), all the characteristic classes are preserved.
Finally, since k is flexible, we may assume that S′ is defined over k.
□
Using this result we can make S∪F into a
single smooth component with the needed Chern classes
numerically trivial. This is done with the help of the following
statement, specific to dimension 5.
Sublemma 4.24.2.4
Let S=S1∪S2 with S1,S2 smooth connected transversal to each other and connected S{1,2}=S1∩S2.
(1)
Suppose, deg(c1(NSi⊂X)⋅[S{1,2}])=0,
deg(c1c2(NSi⊂X)⋅[Si])=0, for i=1,2, deg(c13(NS⊂X)⋅[S])=0, and for p=2,
c12(NS⊂X)⋅[S]∼Num(p)0 on X. Then there exists a blow-up ε:X^→X such that ε∗([S])
is represented by the class of a smooth connected subvariety S^ with
deg(c1c2(NS^⊂X^)⋅[S^])=0, deg(c13(NS^⊂X^)⋅[S^])=0, and for p=2,
c12(NS^⊂X^)⋅[S^]∼Num(p)0 on X^.
(2)
If [S]∼Num(p)0 and deg(c1c2(NSi⊂X)⋅[Si])=0, then
deg(c1(NSi⊂X)⋅[S{1,2}])=0.
Proof:
(2) Denote Ni=NSi⊂X. Then deg(c1(N1)⋅[S{1,2}])=deg(c1(N1)⋅[S1]⋅[S2])=deg(c1(N1)⋅[S1]⋅[S])−deg(c1(N1)⋅[S1]⋅[S1])=−deg(c1c2(N1)⋅[S1])=0, as [S]∼Num(p)0,
and similarly, deg(c1(N2)⋅[S{1,2}])=0.
(1)
Let π:X→X be the blow-up in the components of S, with the components Ei⟶πiSi
of the special divisor, and ρi=−[Ei]. Note, that E1,E2 and E{1,2}=E1∩E2 are connected.
Then π∗([Si])=[Ei]⋅(ρi+πi∗c1(Ni)).
Consider the classes [E1](ρ1−ρ2+π1∗c1(N1)) and [E2](ρ1+ρ2+π2∗c1(N2)).
We may assume that these classes are represented by the classes of smooth connected subvarieties S1′ and S2′, contained
in E1 and E2, respectively, and transversal to each other and to E{1,2}. Let S′=S1′∪S2′. Then [S′]=π∗([S]).
Using the equation ρi2+ρiπ∗c1(Ni)+π∗c2(Ni)=0, on E{1,2} we get:
[TABLE]
where π{1,2}:E{1,2}→S{1,2}=S1∩S2 is the projection. Here S{1,2} is a smooth connected curve, with
deg(c1(Ni)⋅[S{1,2}])=0. Because S{1,2} is connected, this implies that
[S1′∩S2′]∼Num(p)0 on E{1,2}.
By Sublemma 4.24.2.3, we can substitute Si′ by smooth connected Si, transversal to each other, with
anisotropic S1∩S2, without changing characteristic classes in Ch∗(X). Let η:X→X
be the blow-up in S1, S2, with the special divisor V.
Here V is smooth outside an anisotropic subscheme (the intersection of components), and so, we can treat it as a single component.
η∗([S]) is represented by the class of a subvariety S of V whose characteristic classes are
η∗ of those of S, and which is smooth outside an anisotropic subscheme.
Then using Statement 6.5 (with V treated as a single component) and flexibility of k, we can find an irreducible
divisor Z on X, smooth outside an anisotropic subscheme, and containing S. Let μ:X^→X be the embedded
desingularization of Z, and Z^, S′′ be the proper pre-images of Z and S.
Since the singularities of Z are anisotropic, the map μ∗:Chk/k∗(X)→=Chk/k∗(X^)
is an isomorphism, and μ∗([S])=[S′′]. Let S^ be a smooth connected variety representing [S′′]
on the smooth connected divisor Z^. Since S′′ is smooth outside an anisotropic subscheme,
the characteristic classes of S^ with values in Chk/k∗(X^) coincide with μ∗ of those of S.
It remains to check that the needed characteristic classes of S^ are trivial. Using the fact that E{1,2} is a
P1×P1-bundle over a curve S{1,2}, and the equation ρi2+ρiπi∗c1(Ni)+πi∗c2(Ni)=0 on Ei, we get:
[TABLE]
Similarly,
[TABLE]
Finally, for p=2, the fact that c12(NS^⊂X^)⋅[S^]∼Num(p)0
follows from Sublemma 4.24.2.5.
□
Proof:
In the notations of the proof of Sublemma 4.24.2.4,
denoting ν=η∘μ, and using
the fact that E{1,2} is a
P1×P1-bundle over a curve S{1,2}, the equation ρi2+ρiπi∗c1(Ni)+πi∗c2(Ni)=0 on Ei, and
[5, Thm 6.7], we obtain:
[TABLE]
since c1(Ni)∼Num(p)0 on S{1,2} (note, that S{1,2} is connected).
Here j{1,2}:E{1,2}→X is the closed embedding.
□
The subvariety S∪F satisfies the conditions of
Sublemma 4.24.2.4(1). Thus, we may substitute it by a single connected component and assume that our class is represented
by the class of T∪G, where [G]=(−ρ)⋅ρ, for
some divisor ρ, and T is a smooth connected subvariety
with c13(NT⊂X)⋅[T]∼Num(p)0, c1c2(NT⊂X)⋅[T]∼Num(p)0, and for p=2, in addition,
c12(NT⊂X)⋅[T]∼Num(p)0.
We may assume T and G transversal, with G and T∩G connected. Clearly, c13(NG⊂X)⋅[G]∼Num(p)0,
c1c2(NG⊂X)⋅[G]∼Num(p)0, and for p=2, c12(NG⊂X)⋅[G]∼Num(p)0 as well.
Since [T]+[G]∼Num(p)0, applying Sublemma 4.24.2.4(2) and (1) again, we may represent our class by [S],
where S is smooth connected with
c13(NS⊂X)⋅[S]∼Num(p)0, c1c2(NS⊂X)⋅[S]∼Num(p)0, and for p=2, in addition,
c12(NS⊂X)⋅[S]∼Num(p)0. Lemma 4.24.2 is proven.
□
Now as S is smooth connected with numerically trivial
zero-dimensional Chern classes, we can move up the dimension
and make the square of the 1-st Chern class numerically
trivial as well. This is already achieved for the prime 2. It
remains to treat the odd primes. We will, actually, make the mentioned c12 numerically trivial not only on X, but
already on S itself. This will be important for the next step.
Lemma 4.24.3
We may assume that S is smooth connected with c13(NS⊂X)⋅[S]∼Num(p)0,
c1c2(NS⊂X)⋅[S]∼Num(p)0 and c12(NS⊂X)⋅[S]∼Num(p)0 on X.
We also may assume that c12(NS⊂X)∼Num(p)0 on S.
Proof:
By Lemma 4.24.2, we have all the needed conditions, aside from that on c12.
Let us first make c12(NS⊂X)⋅[S]∼Num(p)0 on X.
For p=2 we already have it by Lemma 4.24.2.
(p=2,3)
Let π:X→X be the blow-up in the smooth connected complete intersection
R=21c1(NS⊂X)⋅31c1(NS⊂X) (of very ample divisors on S).
Let E be the special divisor of π, and ρ=−[E]. Then π∗([S])=[S]+[F], where S is the proper transform
of S and F is a smooth connected (very ample) divisor on E, transversal to S, with connected S∩F and
with [F]=[E](ρ+πE∗c1), where
cl=cl(NS⊂X). Also, c1(NS⊂X)=2ρ+πS∗c1 and c1(NF⊂X)=πE∗c1, where
πS:S→S and πE:E→R are natural projections.
Since ρ satisfies the equation ρ2+65πS∗c1⋅ρ+61πS∗c12 on S, and dim(R)=1,
we have:
[TABLE]
since −[S]ρ is represented by the class of a P1-bundle P=PR(NR⊂S) over R, and c1∼Num(p)0 on R,
as deg(c13⋅[S])=0 and R is connected.
By the same reason,
[TABLE]
At the same time, since ρπS∗c1∼Num(p)0 on S, as we saw above, and [S]c13∼Num(p)0, by assumption,
[TABLE]
again, since dim(R)=1 and c1∼Num(p)0 on R. Using the same arguments,
[TABLE]
Let ε:X^→X be the blow-up from Sublemma 4.24.2.4 applied to S∪F. Then we get a smooth
connected subvariety S^ on X^ such that c13(NS^⊂X^)⋅[S^]∼Num(p)0 and
c1c2(NS^⊂X^)⋅[S^]∼Num(p)0. Finally, by Sublemma 4.24.2.5,
[TABLE]
The case (p=2,3) is done.
(p=3)
Let d1=c12+c2 be the characteristic class of degree 2 corresponding to the reduced power operation P1:Ch∗→Ch∗+2
(modulo 3). Since [S]∼Num(p)0, by Proposition 4.6,
d1(NS⊂X)⋅[S]=P1([S])∼Num(p)0 as well. On the other hand, c2(NS⊂X)⋅[S]=[S]⋅[S]∼Num(p)0.
Hence, c12(NS⊂X)⋅[S]∼Num(p)0 too. The case (p=3) is done.
Thus, we managed to make c12(NS⊂X)⋅[S]∼Num(p)0, while keeping c13(NS⊂X)⋅[S]∼Num(p)0 and
c1c2(NS⊂X)⋅[S]∼Num(p)0. Let us now make the complete intersection
c1(NS⊂X)⋅c1(NS⊂X) on S anisotropic.
By blowing-up S, we may assume that S⊂Y, where Y is smooth connected divisor on X. Note, that the new
c13,c1c2 and c12 characteristic classes
are the pull-backs of the old ones, and so, are still numerically trivial. By Statement 6.5 and flexibility of k, there
exists an irreducible and smooth outside an anisotropic subscheme (of S) divisor Z containing S, such that the restriction
Ch1(X)↠Ch1(Z\S) is surjective. Let π:X→X be an embedded desingularization of Z and S,
with proper pre-images Z and S, which are smooth connected subvarieties. Since singularities were anisotropic, the maps
π∗:Chk/k∗(X)→=Chk/k∗(X) and
πZ∗:Chk/k∗(Z\S)→=Chk/k∗(Z\S) are isomorphisms, and so, the restriction
Chk/k1(X)↠Chk/k1(Z\S) is surjective as well.
Thus, the group Chk/k1(Z) is generated by the image of j∗:Chk/k1(X)→Chk/k1(Z) and the class
[S].
Also, on X, the classes
c13(NS⊂X)⋅[S], c1c2(NS⊂X)⋅[S] and
c12(NS⊂X)⋅[S] are ∼Num(p)0.
Since c12(NS⊂X)⋅[S]∼Num(p)0 on X, this class
will be orthogonal to the im(j∗) on Z. While, on Z,
[TABLE]
since c12(NS⊂X)⋅[S]∼Num(p)0 on X and c1(NZ⊂X) is in the image of j∗.
Hence, c12(NS⊂X)⋅[S]∼Num(p)0 already on Z.
Since this class is a complete intersection on Z, the intersection of generic representatives of the respective
(very ample) linear systems is anisotropic by Statement 6.3. The respective subvariety S is smooth connected,
and c13 and c1c2 characteristic classes are preserved.
Since k is flexible, we may assume that our varieties are defined over k.
Lemma 4.24.3 is proven.
□
In order to apply Corollary 6.12 and finish the proof of Proposition 4.24, it remains to terminate numerically the 1-st Chern class of our S.
Lemma 4.24.4
We may assume that S is smooth connected and c1m(NS⊂X)⋅[S]∼Num(p)0, for m⩾0.
Proof:
By Lemma 4.24.3, we may assume that S is smooth connected variety with the numerically trivial c13, c1c2 and c12
characteristic classes. It remains to make c1 numerically trivial.
We need to treat separately the case p=2 and that of odd primes.
missing(p=2)
Let R be the generic representative of the (very ample) linear system ∣21c1(NS⊂X)∣ on S.
It is a smooth connected surface and, by Statement 6.3, we have the surjection Ch1(S)↠Ch1(R).
Since k is flexible, we may assume that it is defined over k.
Let π:X→X be the blow-up at R,
with the special connected divisor E and ρ=−[E]. Then π∗([S])=[S]+[F], where S is the proper pre-image of S and
F is a smooth connected divisor on E transversal to S, with connected S∩F and with
[F]=[E](ρ+πE∗c1), where cl=cl(NS⊂X).
We have:
[TABLE]
since, on S≅S, ρ=−[R], and
c1⋅[R]∼Num(p)0 on R, as c12(NS⊂X)∼Num(p)0 on S and Ch1(S)↠Ch1(R). On the other hand, on R=S∩E,
[TABLE]
and moreover, we may assume the intersection S∩F to be anisotropic.
By Statement 6.6, there exists a blow-up μ:X→X,
such that μ∗([S∪F]) is represented by the class
of a smooth connected subvariety S and such that the characteristic classes of S in Chk/k∗ are μ∗ of the
respective classes of S∪F. In particular, the c1-class of it is numerically trivial.
It remains to check c12
and c13 characteristic classes of S∪F. We have:
[TABLE]
on X, since (2ρ+πS∗c1)=0 on S, and deg(c13(NS⊂X)⋅[S])=0 while R is connected.
Similarly,
[TABLE]
by the same and dimensional reasons.
The case (p=2) is done.
missing(p=2)
The characteristic class c1 corresponds to the reduced power operation P1:Ch∗→Ch∗+1 (modulo 2).
Since [S]∼Num(p)0, by Proposition 4.6, c1(NS⊂X)⋅[S]=P1([S])∼Num(p)0 as well.
Lemma 4.24.4 is proven.
□
Proposition 4.24 now follows from Corollary 6.12 and flexibility of k.
□
As Conjecture 4.7 was established for all varieties
of dimension ⩽5, from the existence of push-forward and
pull-back structure we obtain that isotropic Chow groups form
a quotient of the 3-rd theory of higher type associated to
Ch.
Proposition 4.25
Let k be a flexible field. The projection Ch∗↠Chk/k∗ factors through Ch(3)∗.
Proof:
A class u∈Ch∗(X) is =0∈Ch(3)∗, if it can be presented as f∗(y⋅g∗(v)), where
X⟵fX×Q⟶gQ are natural projections, Q is a smooth projective variety of dimension 5,
y∈Ch∗(X×Q) and v∈Ch∗(Q) is ∼Num(p)0. Then, by Proposition 4.15, Corollary 4.17, Proposition 4.18,
Proposition 4.22 and Proposition 4.24,
v=0∈Chk/k∗(Q), and so, u=0∈Chk/k∗(X).
□
5 Thick local categories
In this section we extend the definition of local motivic category to arbitrary finite coefficients Z/n and
introduce the thick versions of it which have better conservativity properties.
Definition 5.1
Let n∈N. Let P and Q be smooth varieties of finite type over k. We say that XQ>nXP, if P is n-isotropic
over every generic point of Q, while
Q is n-anisotropic over some generic point of P.
Let E/k be some finitely generated extension and P be smooth connected variety with k(P)=E.
Let Qn be the disjoint union of all smooth connected varieties Q of finite type with XQ>nXP and
[TABLE]
Generalizing Definition 2.3, we can define the local motivic category with Z/n-coefficients.
Definition 5.2
The local motivic category with Z/n-coefficients
[TABLE]
If we are interested in a p-localized situation,
we can define the thick local motivic categories.
Definition 5.3
The p-local motivic category of thickness r and F-coefficients
[TABLE]
In particular, the local category with Z/pr-coefficients DM(E/k;Z/pr) is the p-local motivic category
of thickness r and Z/pr-coefficients DM({E/k}r;Z/pr).
Since XQ>nXP implies that XQ>mXP for m∣n, we get natural functors
[TABLE]
for any r⩾s and m∣n,
commuting with the natural functors φEZ/n:DM(k;Z/n)→DM(E/k;Z/n).
In the usual way, we can introduce local geometric motives, local Chow motives and local Chow groups.
Exactly as in Proposition 2.16 we get the description of isotropic Chow groups:
Proposition 5.4
[TABLE]
Similarly, for the thick local Chow groups, we have:
[TABLE]
Since every n-anisotropic class is numerically equivalent to zero modulo n, we obtain the surjection:
[TABLE]
Question 5.5
Let k be flexible. Is it true that CHk/k(X;Z/pr)=CHNum(X;Z/pr)?
Using the arguments of Proposition 4.15 and Corollary 4.17, we see that the answer is positive for divisors and for zero-cycles.
In particular, the projection CH(X;Z/pr)↠CHk/k(X;Z/pr) factors through CHalg(X;Z/pr).
Also, it is easy to see that it is true for
cycles of dimension 1, provided p>2, and so, the mentioned projection factors through CH(2)(X;Z/pr), in this case.
With the increase of r (and fixed s), the family of functors
[TABLE]
for all f.g. extensions E/k, becomes more and more conservative. But the target categories are getting more complicated.
At the same time, the categories DM(E/k;Z/pr) (that is r=s) should be simpler, and the natural strategy to
improve conservativity is to pass to Z(p)-coefficients.
The local motivic category with Z(p)-coefficients DM(E/k;Z(p))
should be the local category of ∞* thickness* DM({E/k}∞;Z(p)).
This should be defined as a limit limrDM({E/k}r;Z(p)) of categories of finite thickness
and will be considered in a separate paper.
6 Auxiliary results
6.1 Up to blow-up, Chow ring of a variety is generated by divisors
The following result is crucial for most of our constructions.
Theorem 6.1
Let X be a smooth projective variety and y∈CHr(X). Then there exists a blow-up π:X→X such that
π∗(y) is a Z-polynomial in divisor classes.
Proof:
Induction on the dim(X). Below we will denote this induction as Ind1.
(Ind1 base)dim(X)=0. Nothing to check.
(Ind1 step) Can assume that r>0. Then y has support on some divisor.
By blowing X up we can assume that this divisor has
strict normal crossings, and by the following Lemma, can assume that y has support on a smooth divisor D.
Lemma 6.1.1
If y=∑iyi, and the statement is true for each yi, then it is true for y.
Proof:
Suppose, for each i, there exists such blow-up
πi:Xi→X that πi∗(yi) is a polynomial in divisorial classes. Then, by the results of Hironaka [7], there
exists a blow-up π:X→X, which covers πi, for each i. Then, clearly, π∗(y) is a polynomial in
divisorial classes.
□
Let now jD:D→X be a smooth divisor and y is supported on D.
Let us say that the pair (D,X) has a special structure with the base B if D is a consecutive projective bundle over B where the canonical
line bundles O(1) of all these fibrations are the restrictions of some line bundles from X.
Every pair (D,X) possesses a ”trivial” special structure with the base B=D.
We will prove our statement by the induction on the dim(B). We will denote this induction as Ind2 below.
(Ind2 base)dim(B)=0. Then D is a disjoint union of consecutive projective bundles whose all canonical bundles O(1)
are restrictions of some line bundles from X. Then CH∗(D) is generated by jD∗(c1(L)), for some line bundles L on X.
Since y=(jD)∗(y), for some y∈CH∗(D), it is a polynomial in divisorial classes.
(Ind2 step) We have: y=(jD)∗(y), where y=∑lε∗(ul)⋅rl with ul∈CH∗(B), ε:D→B is the natural projection, and rl is a monomial
in ρt’s, where ρt=c1(O(1)t) is the restriction of some divisorial class from X. By Lemma 6.1.1, we can
assume that y=ε∗(u), where u∈CH∗(B).
Since dim(B)<dim(X), by the inductive assumption of Ind1, there exists a blow-up τ:B→B, such that
τ∗(u) is a polynomial in divisorial classes. We have a cartesian diagram of blow-ups:
[TABLE]
Let φ:X→X be a blow-up of X in the same centers as τD, and jD:D→X.
Then φ∗((jD)∗ε∗(u))=(jD)∗τD∗(ε∗(u))+∑mvm, where vm are supported on the components Em
of the special divisor E=∪mEm of the blow-up φ - see [5, Thm 6.7] (or [16, Prop. 5.27]).
Let Xm be a variety obtained after m blow-ups with the special divisor
jEm:Em→Xm of the m-th blow-up and the projection φm:X→Xm whose restriction to Em is
the blow-up αm:Em→Em. Then (again by [5, Thm 6.7]), the image of
[TABLE]
has support on ∪n>mEn, while the map
[TABLE]
is surjective (since ∪n⩾mEn\∪n>mEn is an open subvariety of Em). Hence, the map
[TABLE]
covers the image of (jE)∗.
The pair (Em,Xm) has a special structure with the base of dimension smaller than B (namely, the center of the m-th blow-up of
τ), where c1(O(1)) of the external projective fibration is the restriction of [−Em] from Xm, and all the other (internal)
canonical bundles are induced by the special structure on (D,X), and so, are restrictions of some divisorial classes from X.
By the inductive assumption of Ind2, any element in (jEm)∗CH∗(Em) is a polynomial in divisorial classes over some
blow-up Xm→Xm. By Lemma 6.1.1, we obtain that ∑mvm is a polynomial in divisorial classes
over some blow-up of X. Hence, it remains to deal with (jD)∗τD∗(ε∗(u)).
We know that τD∗(ε∗(u))=ε∗τ∗(u) is a polynomial in divisorial classes by construction. Let us denote this
element again as y and the divisor (on which it is supported) as D.
By Lemma 6.1.1,
we can assume that y is a monomial x1⋅…⋅xr−1 in very ample divisorial classes on D.
We will use induction on r. Below it will be denoted as the Ind3.
(Ind3 base) When r=1 there is nothing to prove as y=(jD)∗(y)=[D].
(Ind3 step) Consider the chain of co-dimension 1 regular embeddings
D⟵i1Y1⟵i2Y2⟵i3…, where [Yk+1] represents the restriction of x1
to Yk. Construct the chain of blow-ups
X⟵π1X1⟵π2X2⟵π3… in co-dimension-two centers
Zk→Xk−1 inductively as follows.
The special divisor Ek of πk is a consecutive projective line fibration Ek→φkYk and
Zk+1=φk−1(Yk+1). In particular, Ek→εkZk is a projective line fibration and
φk=ε1∘…∘εk. Let ik=i1∘…∘ik and yk=φk∗(ik)∗(y) be the class supported on Ek.
Then we have a cartesian diagram
[TABLE]
with Ek=Ek and yk+1=εk+1∗α∗yk.
By (the Chow group version of) [16, Prop. 5.27], we have:
[TABLE]
Here, by the inductive assumption of Ind3, the first summand
(jEk)∗yk=(jEk)∗(x1⋅x2⋅…⋅xr−1)=[Ek+1]⋅(jEk)∗(x2⋅…⋅xr−1)
is expressible as a polynomial in divisorial classes over some
blow-up of Xk+1, so (using Lemma 6.1.1) the question about yk supported on Ek→Xk is reduced to
the question about yk+1 supported on Ek+1→Xk+1. Thus, it is sufficient to show that
our statement is true for yk supported on Ek→Xk, for at least, one k.
But for k=dim(X)−r, the class (ik)∗(y) is zero by dimensional reasons.
Hence, the (Ind3 step) is proven. This implies (Ind2 step) and (Ind1 step).
The Theorem is proven.
□
Corollary 6.2
Let X be a smooth projective variety and y∈CHr(X). Then there exists a blow-up π:X→X, such that
π∗(y) is represented by a linear combination of classes of smooth complete intersections of very ample divisors which are
transversal to each other. In particular, for r>dim(X)/2, it is represented by the difference of classes of two smooth disjoint
subvarieties.
6.2 General position results
In this section we present various general position arguments which permit to replace
cycles by the classes of connected subvarieties and, in some cases, reduce the anisotropy of a class [S]
to the numerical triviality of some characteristic classes of S.
The following simple and well-known ”Chow group shadow” of the Lefshetz theorem is one of our key ingredients.
Statement 6.3
Let X be a scheme with a map X→fPn and
ι:Dη→X be the generic hyperplane section of X (over k((Pn)∨)).
Then the pull back ι∗:CH∗(X)↠CH∗(Dη) is surjective.
If X is a smooth variety, so is Dη.
Proof:
Consider Y⊂X×(Pn)∨ given by Y={(x,H)∣f(x)∈H}.
Then Y is a projective bundle: Y=ProjX(V), where V=W/O(−1) (with (Pn)∨=P(W)).
Let Yη be the generic fiber of the projection
Y→(Pn)∨. This is the ”generic” hyperplane section Dη.
By the projective bundle theorem and localization, we have surjections
CH∗(X)[ρ]↠CH∗(Y)↠CH∗(Yη), where ρ=c1(O(1)). Since ρ is the pull-back
of the class of a hyperplane on (Pn)∨, it is zero in CH∗(Yη). Thus, we get the surjection
CH∗(X)↠CH∗(Yη). Finally, if X is smooth, so is Y and Yη.
□
The next result shows that any closed subscheme of an effective Cartier divisor can be made the base set of the respective linear system (which, in turn, can be made very ample), if we modify the divisor by an
n-multiple of some other divisor, for a given natural n.
Statement 6.4
Let X be an irreducible quasi-projective variety and n∈N.
Let E be an effective Cartier divisor on X, and S⊂E be a closed subscheme.
Then there exists a very ample divisor D such that the linear system ∣E+n⋅D∣S consists
of very ample divisors and S is the base set of it.
Proof:
There are very ample divisors F1,F2 on X such that [E]=[F1]−[F2]. Then the class [E+nF2]=[F1+(n−1)F2]=[H] is very ample
and defines an embedding X↪PN. Let S be the closure of the image of S in this embedding.
The coordinate ring of S has relations of degree ⩽m.
In other words, the base set of the linear system ∣kH∣S is S, for any k⩾m. Take k=nm+1. Then
[kH]=[(nm+1)(E+nF2)]=[E+n(mF1+((n−1)m+1)F2)]=[E+nD], where D=mF1+((n−1)m+1)F2 is very ample.
□
The following result will enable us to substitute a multi-component divisor with only n-anisotropic singularities, which
contains a given closed subscheme, by a single component one.
The same can be done with a collection of such divisors and
subschemes with the result having all the faces connected, if
the original collection of divisors was with strict normal crossings modulo n-anisotropic subvarieties.
This will be our key tool below.
Statement 6.5
Let n∈N, X be a smooth projective connected variety of dimension d and
E=∪iEi be a divisor on it with strict normal crossings
outside an n-anisotropic closed subscheme, with, possibly, reducible components Ei, and let
Si⊂Ei be some closed subschemes such that, for any subset I of the set of indices, dim(SI)<d−#(I), where
SI=∩i∈ISi.
Then, over some purely transcendental f.g. extension of k, there is a divisor Z=∪iZi, where [Zi]=[Ei]∈CH1(X;Z/n),
Si⊂Zi, for any I, the variety ZI=∩i∈IZi is irreducible, and Z has strict normal crossings outside an
n-anisotropic closed subscheme of S. Moreover, the restriction CH∗(X)↠CH∗(Zi\Si) is surjective.
Proof:
By the Statement 6.4, for any i, there exists a very ample divisor Di, such that the linear system
Φi=∣Ei+n⋅Di∣Si
consists of very ample divisors and has the base set Si. Let Zi be the generic element of this linear system
(defined over k(P(Φi))). Clearly, [Zi]=[Ei]∈CH1(X;Z/n) and Si⊂Zi.
Let us show that ZI=∩i∈IZi is irreducible. We will prove by induction on #(I) that, for any i∈I, the restriction
CH0(ZI\i)↠CH0(ZI) is surjective. The (base)I=∅ is empty.
(step) The linear system Φi defines an embedding of X\Si into a projective space, and for any subscheme
T⊂X defined over some field L and Zi defined over L(P(Φi)) as above, we have:
dim(T∩(Zi\Si))⩽dim(T)−1. By the Statement
6.3, we have a surjection
CH0(ZI\i\ZI\i∩Si)↠CH0(ZI\ZI\i∩Si).
We know that all the components of ZI have dimensions ⩾d−#(I). On the other hand, the scheme
ZI\i∩Si is the union ∪i∈J⊂IYJ, where
YJ=(∩j∈JSj)∩(∩j∈I\J(Zj\Sj)). Since dim(YJ)⩽dim(SJ)−#(I\J),
we obtain that dim(ZI\i∩Si)⩽max(dim(SJ)−#(I\J)∣i∈J⊂I)<d−#(I). Hence,
CH0(ZI)=CH0(ZI\ZI\i∩Si), and we get the surjection
CH0(ZI\i)↠CH0(ZI). Induction step is proven.
Thus, we have the surjection CH0(X)↠CH0(ZI), and since X is irreducible, so is ZI.
Our system Φi contains Ei+∣n⋅Di∣.
The generic representative of ∣n⋅Di∣ is n-anisotropic
(by Statement 6.3 and the arguments from the proof of Proposition 4.15).
Thus, the generic representative Gi of Ei+∣n⋅Di∣
has only n-anisotropic singularities and, modulo n-anisotropic subvarieties, the divisor G=∪iGi has strict normal crossings.
Consequently, the generic representative Zi of our system
∣Ei+n⋅Di∣Y will have only n-anisotropic singularities too, and the divisor Z=∪iZi will have strict normal crossings
modulo n-anisotropic subvarieties.
Indeed, we have a divisor W on X×P, where P=∏iP(Φi) parameterizes (combinations of) elements of our linear systems.
The fiber over the generic point of P is Z, while the fiber over some special point is G.
Let R be a d.v.r. with the fraction field K and residue field κ, and WR be some divisor on X×Spec(R), with
fibers WK and Wκ over the generic and closed point of Spec(R), respectively.
Having a closed point T of WK, consider the closure of it in W.
We get a proper morphism f:T→Spec(R) of relative dimension
zero, whose fiber over Spec(κ) consists of points tl with multiplicities el - these are the specializations
of T. The specialization of a singular point is singular, and specialization of a point where components are not transversal has
the same property. At the same time,
[TABLE]
So, if [k(T):K] is not divisible by n, then one of [k(tl):κ] is.
This shows that Z should be a divisor with strict normal crossings at every point which is not n-anisotropic.
Since our linear system Φi is very ample on X\Si, the divisor Z has strict normal crossings outside S.
By the same reason and by Statement 6.3, we have the surjection CH∗(X)↠CH∗(Zi\Si).
□
This permits to represent some cycles of co-dimension 2 by single components.
Everywhere below we will denote:
[TABLE]
where n is some natural number (which should be clear from context).
Statement 6.6
Let S=∪iSi be the union of smooth connected transversal subvarieties of codimension 2 on a smooth projective variety
and n∈N.
Suppose, that all the intersections Si∩Sj are n-anisotropic. Then over some f.g. purely transcendental extension of k
there exists a blow-up μ:X→X, such that
μ∗([S])∈Chk/k∗(X) is represented by the class of a smooth connected variety
S whose characteristic classes in Chk/k∗ are μ∗ of the characteristic classes of S.
Moreover, if S=∪iSi and T=∪jTj are two subvarieties as above which are transversal to each other, then there exists
a blow-up μ:X→X with the properties as above for both S and T and such that S and T are smooth
connected, transversal to each other, and S∩T is connected.
Proof:
Let π:X→X be the blow-up in all the components Si of S, with Ei⟶πiSi
the components of the special divisor and
ρi=−[Ei]. Then, by [5, Prop. 6.7], π∗([S])=[F], where F=∪iFi, Fi is supported on Ei and
[Fi]=[Ei](ρi+πi∗(c1(NSi⊂X))). Note, that E=∪iEi is a divisor with strict normal crossings, with
all the intersections Ei∩Ejn-anisotropic. Note, that c1(NFi⊂X)=πi∗(c1(NSi⊂X))
and c2(NFi⊂X)=πi∗(c2(NSi⊂X)). Hence, the same is true about all other characteristic classes.
Since E is smooth outside an n-anisotropic subscheme, by Statement 6.5
(where we consider E as a single component), over
some f.g. purely transcendental extension of k, there is an irreducible divisor Z, containing F,
smooth outside an n-anisotropic closed subscheme of F.
Let ε:X→X be an embedded desingularization of Z. Let Z and F be the proper pre-images of Z and F.
Then ε∗:Chk/k∗(X)→=Chk/k∗(X) is an isomorphism and
ε∗([F])=[F]∈Chk/k2(X) is supported on the smooth connected divisor Z.
By adding an n-multiple of a very ample divisor, we can substitute [F] by a very ample divisor on Z.
Let S be the generic representative of the linear system ∣F∣ on Z. Then S is smooth and connected.
Since, modulo n-anisotropic subvarieties, X coincides with X and F with F, the characteristic classes of S in
Chk/k∗(X) are ε∗ of the respective classes of F.
For the pair of subvarieties S=∑iSi and T=∑jTj, consider the blow-up π:X→X at all the components of S and T.
Then the special divisor E=ES∪ET has strict normal crossings, where ES and ET are smooth outside n-anisotropic subschemes.
Applying Statement 6.5 to FS∪FT contained in ES∪ET (where we consider ES and ET as single components),
we obtain a divisor Z=ZS∪ZT containing S∪T,
with strict normal crossings outside an n-anisotropic subscheme,
with irreducible ZS,ZT and ZS∩ZT. Resolving n-anisotropic singularities and non-transversalities of Z, as above,
we obtain the needed smooth connected transversal subvarieties S and T having the needed characteristic numbers.
Since ZS∩ZT is irreducible, the intersection S∩T is connected.
□
The next statement represents an elementary block with the help
of which we will “deform” the chains of
co-dimension 1 embeddings of irreducible varieties.
Statement 6.7
Let n∈N, X be projective irreducible variety, smooth outside an n-anisotropic closed subscheme,
and S⊂Z⊂X be embeddings of co-dimension
1 of irreducible subvarieties, smooth outside n-anisotropic closed subschemes and such that S is not n-anisotropic.
Then, over some f.g. purely transcendental extension of k,
there exists Z′, such that S⊂Z′⊂X has the same properties, [Z′]=[Z] in Chk/k1(X) and the restriction
Chk/k∗(X)↠Chk/k∗(Z′\S) is surjective.
Proof:
This is a particular case of Statement 6.5, aside from the fact that we permit X to have anisotropic singularities.
But the same proof works.
Outside some closed n-anisotropic subscheme T of X, Z is a Cartier divisor and,
by the Statement 6.4, there exists a very ample divisor D on X\T, such that the linear system
Φ=∣Z+n⋅D∣S\S∩T on X\T consists of very ample divisors and has the base set S\T.
This linear system defines an embedding
of X\(S∪T) into a projective space.
Let Z′ be the closure in X of the generic element of this linear system
(defined over k(P(Φ))). Since S is not n-anisotropic, S\S∩T is non-empty, and so, Z′ contains S.
Clearly, [Z′]=[Z]∈Chk/k1(X)=Chk/k1(X\T).
By Statement 6.3, we have a surjection Chk/k∗(X)↠Chk/k∗(Z′\S),
and Z′ is irreducible. The same arguments as in the proof of Statement 6.5 show that Z′ has only n-anisotropic
singularities.
□
The previous result permits to deform the chains of co-dimension
1 embeddings in such a way that isotorpic Chow groups of a term of the new chain would be covered by those of the previous (ambient) term modulo such groups of the next (smaller) term of the original chain. Later it will enable us, subject to certain conditions, to make numerically trivial classes anisotropic.
Statement 6.8
Let n∈N and
Xr→jrXr−1→jr−1…→j2X1→j1X0
be embeddings of co-dimension 1 of irreducible subvarieties, smooth outside n-anisotropic closed subschemes, with
Xr- not n-anisotropic.
Then, over some f.g. purely transcendental extension of k, it can be complemented to a commutative diagram:
[TABLE]
where all maps are embeddings of co-dimension 1 of irreducible subvarieties, smooth outside n-anisotropic closed subschemes and
for any i, the map
[TABLE]
is surjective (for i=r, the map (jr′)∗ is surjective), and [Xi+1′]=[Xi+1]∈Chk/k1(Xi′).
Proof:
This follows from the inductive application of the Statement 6.7 from top to the bottom.
Finally, in the last step, we take Xr′ to be the closure of the generic representative of the respective (very ample)
linear system ∣Xr+n⋅D∣ without any base-set. Since Xr is not n-anisotropic, Xr′ is non-empty and irreducible.
By Statement 6.3, we have a surjection (jr′)∗:Chk/k∗(Xr−1′)↠Chk/k∗(Xr′)□
Note, that although, Xr−1′ is still not n-anisotropic, Xr′ may be, in principle, anisotropic.
We also have a ”smooth” version of the above result which is
what we will use below.
Statement 6.9
Let X0 be a smooth projective connected variety,
and Xr→jrXr−1→jr−1…→j2X1→j1X0
be regular embeddings of co-dimension 1 of connected varieties, with Xr-not n-anisotropic.
Then, over some f.g. purely transcendental extension of k, it can be complemented to a commutative diagram:
[TABLE]
where upper and lower horizontal maps are regular embeddings of co-dimension 1 of connected varieties, while
the vertical ones are blow-ups in n-anisotropic centers.
In particular, the maps πi∗:Chk/k∗(Xi)→=Chk/k∗(Xi) are isomorphisms.
Also, for any i, the map
[TABLE]
is surjective (for i=r, the map (jr′)∗ is surjective), and [Xi+1′]=(gi+1)∗[Xi+1]∈Chk/k1(Xi′).
Proof:
By Statement 6.8, we get the commutative diagram
[TABLE]
where Xi are irreducible varieties smooth outside some closed proper n-anisotropic subschemes, the maps
[TABLE]
are surjective, and [Xi+1]=[Xi+1]∈Ch1(Xi).
Let π0:X0′→X0 be the embedded
desingularization of Xr⊂Xr−1⊂Xr−2⊂…⊂X1⊂X0,
and εi:Xi′→Xi be the proper pre-images (with ε0=π0). Since special divisors are n-anisotropic, we have
isomorphisms εi∗:Chk/k∗(Xi)→=Chk/k∗(Xi).
Noting that Xi is not n-anisotropic, by blowing Xi at n-anisotropic centers,
we may resolve the indeterminacies of the maps
Xi→giXi−1⇢εi−1−1Xi−1′ and
Xi→jiXi−1⇢πi−1−1Xi−1
and obtain commutative squares
[TABLE]
and the needed commutative diagram.
Since the maps πi∗:Chk/k∗(Xi)→=Chk/k∗(Xi′) are isomorphisms, the maps
[TABLE]
are surjective (for i=r, the map (jr′)∗ is surjective), and [Xi+1′]=(gi+1)∗[Xi+1]∈Chk/k1(Xi′).
Finally, since [Xi]=(gi)∗[Xi]∈Chk/k1(Xi−1), we obtain that
[Xi′]=(gi)∗[Xi]∈Chk/k1(Xi−1′).
□
In the next key statement,
applying the above result repeatedly, we will deform a given
chain of codimension 1 regular embeddings keeping the classes
of all the subvarieties (of the chain)
in Chk/k∗(X)
unchanged, but making the image of Chk/k∗(Xr) (the smallest subvariety) in Chk/k∗(X) a
submodule generated by monomials in the 1-st
Chern classes of normal bundles of the (original) chain.
After that, to make Xr anisotropic, it will remain only
to eliminate the mentioned monomials numerically.
Let l=(l2,…,lr) be a vector of non-negative integers.
We say that l is i-good, if there exists an i+1⩽s⩽r+1 such that
lk>0 for i+1⩽k<s, while lk=0, for k⩾s. Any
i-good vector is (i+1)-good and every vector is r-good,
so we get a filtration.
Statement 6.10
Let Xr→jrXr−1→jr−1…→j2X1→j1X0
be regular embeddings of co-dimension 1 of smooth connected varieties.
Then over some f.g. purely transcendental extension there exists a blow-up in n-anisotropic centers X^0→X0
and a similar sequence of embeddings
X^r→j^rX^r−1→j^r−1…→j^2X^1→j^1X^0, where [X^r]=[Xr]∈Chk/k∗(X0)
and the image of the restriction fj∗:Chk/k∗(X^j)→Chk/k∗(X^r) as a
Chk/k∗(X0)=Chk/k∗(X^0)-module is generated
by monomials c^l=∏i=2rc1li(N^i), for j-good l,
where N^i=NX^i⊂X^i−1, and
the image of the map (f0)∗fj∗:Chk/k∗(X^j)→Chk/k∗+r(X^0) as a Chk/k∗(X0)-module is generated
by elements cl⋅[Xr]=∏i=2rc1li(Ni)⋅[Xr],
where Ni=NXi⊂Xi−1 and l runs over all j-good vectors.
(here fi:X^r→X^i is the embedding).
In particular, the image of (f0)∗:Chk/k∗(X^r)→Chk/k∗+r(X^0) as a Chk/k∗(X0)-module is generated
by elements cl⋅[Xr], where l runs through all vectors.
Proof:
Let us denote the original sequence as
Xr0→jr0Xr−10→jr−10…→j20X10→j10X00.
Either Xr0 is n-anisotropic, in which case there is nothing to prove, or we can produce a diagram as in
Statement 6.9.
We can iterate this process as long as the variety Xrm is not n-anisotropic and obtain diagrams:
[TABLE]
These induce maps on isotropic Chow groups:
[TABLE]
where αil=(jil)∗, βil=(gil)∗(πil−1)∗ and β-maps shift the codimension by (+1).
The maps
[TABLE]
are surjective. Either at some stage we will get an n-anisotropic Xrm, in which case we are done, or we can iterate the process
q=dim(X)+1 times. Set X^i=Xiq, etc. Then Chk/k∗(X^i) is generated by the elements of the form
ω(x), where ω is a composition of α’s and β’s and x∈Chk/k∗(X0). Here we are using the fact
that the number of β’s in such a composition can’t be more than dim(Xi) (as each β increases the codimension by 1),
and so, the chain has to start with X0. We also have maps
γil=(jil)∗ and
δil=(πil−1)∗(gil)∗ fitting commutative diagrams (recall, that (πim)∗ and (πim)∗ are isomorphisms)
[TABLE]
Note, that
[TABLE]
Using these relations, one can reduce ω(x) to the form θ(x), where θ is a combination of αiq’s
and γjq’s. The restriction of such an element to Chk/k∗(Xrq) is f0∗(x) times a monomial in
c1(NXiq⊂Xi−1q)=c1(N^i)’s, where each factor c1(N^i) corresponds to a loop
αiqγiq in θ. Thus, the image fj∗:Chk/k∗(X^j)→Chk/k∗(X^r)
as a Chk/k∗(X0)-module is generated by monomials in c1(N^i)’s. Since such a monomial corresponds to a closed path
from Xjq to itself, these will be exactly j-good monomials.
Also, we need to observe that c1(N^1)=c1(NX^1⊂X^0) is the restriction of a class from X^0.
Finally, from the same relations,
we get that (f0)∗c^n=γ1q…γrqc^n=γ10…γr0cn=cn⋅[Xr]. Hence, the image of (f0)∗(fj)∗:Chk/k∗(X^j)→Chk/k∗+r(X0) as a
Chk/k∗(X0)-module is generated by elements cl⋅[Xr], where l runs over
all j-good vectors.
□
With the previous result in hands we get a practical tool
ensuring the anisotropy of Chow group elements.
Corollary 6.11
Let Xr→jrXr−1→jr−1…→j2X1→j1X0
be regular embeddings of co-dimension 1 of smooth connected varieties with Ni=NXi⊂Xi−1.
Suppose, that cl⋅[Xr]∼Num0 on X0, for all monomials in c1(Ni)’s, i⩾2.
Then, over some f.g. purely
transcendental extension, [Xr]=0∈Chk/kr(X0).
Proof:
By Statement 6.10, over some f.g. purely transcendental extension of k, there exists a blow-up with n-anisotropic centers
π:X^→X and a sequence X^r→j^rX^r−1→j^r−1…→j^2X^1→j^1X^0 of regular embeddings of smooth
connected projective varieties, such that
[X^r]=[Xr]∈Chk/kr(X^0)=Chk/kr(X0) and
the image of the map
(f0)∗:Chk/k∗(X^r)→Chk/k∗′(X^0)
as a module over Chk/k∗(X0) is generated by cl⋅[Xr], for all
r-good (=all) l, where f0:X^r→X^0.
Since all these classes are ∼Num0
on X^0, the [math]-dimensional component of our image is zero. This means that X^r is anisotropic and so,
[X^r]=0∈Chk/kr(X^0).
□
In the case r=2, we get the following:
Corollary 6.12
Let S⊂X be a regular embedding of codimension 2 of smooth connected projective varieties.
Suppose, c1m(NS⊂X)⋅[S]∼Num0 on X, for any m⩾0.
Then, over some f.g. purely transcendental extension, [S]=0∈Chk/k2(X).
Proof:
By blowing X at S we may assume that S is contained in a smooth connected divisor Z. Note, that the ”new” characteristic classes
of S are pull-backs of the ”old” ones, and so, are numerically trivial as well. We obtain the triple S→Z→X.
Our statement now is a particular case of Corollary 6.11, where
it remains to observe that c1(NS⊂X)=c1(NS⊂Z)+c1(NZ⊂X), where the second
summand is defined on X.
□
Bibliography23
The reference list from the paper itself. Each links out to its DOI / PubMed record.
1[1] T. Bachmann, On the Invertibility of Motives of Affine Quadrics , Doc. Math., 22 (2017), 363-395.
2[2] P.Brosnan, Steenrod operations in Chow theory , Trans. Amer. Math. Soc. 355 (2003), no.5, 1869-1903.
3[3] D.-C. Cisinski, F.Déglise, Local and stable homological algebra in Grothendieck abelian categories , Homology, Homotopy and Appl. 11 (2009), no.1, 219-260.
4[4] J.-L. Colliot-Thélène, M. Levine, Une version du théorème d’Amer et Brumer pour les zéro-cycles , Preprint; available at: arxiv.org/abs/0911.4644
5[5] W.Fulton, Intersection Theory , Ergebnisse der Mathematik und ihrer Grenzgebiete (3) 2 , Springer-Verlag, Berlin-New York 1984.
6[6] S. Gille, A. Vishik, Rost nilpotence and free theories , Documenta Math. 23 (2018), 1635-1657.
7[7] H. Hironaka, Resolution of singularities of an algebraic variety over a field of characteristic zero. I,II , Ann. of Math., (2) 79 (1964), 109-203; ibid. (2) 79 (1964), 205-326.
8[8] D. Hoffmann, O. Izhboldin, Embeddability of quadratic forms in Pfister forms , Indag. Mathem., N.S. (2) 11 (2000), 219-237.