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On the Chow Rings of Classifying Spaces for Classical Groups.

LUISALBERTOMOLINAROJAS(*) - ANGELOVISTOLI(**)

ABSTRACT- We show how the stratification method, introduced by Vezzosi in his study ofPGL3, provides a unified approach to the known computations of the Chow rings of theclassifying spaces ofGLn,SLn,Spn,OnandSOn.

1. Introduction.

To algebraic topologists, the cohomology of classifying spaces of linear algebraic groups (or, equivalently, of compact Lie groups) has been an important object of study for a long time. Recently, B. Totaro ([Tot99]) has introduced an algebraic analogue of this cohomology, the Chow ring of the classifying space of a linear algebraic groupG, denoted by AG. If HG de- notes theintegral cohomology of theclassifying spaceof G, there is a natural ring homomorphism AG!HG, which is, in general, neither sur- jective not injective.

Remarkably, the Chow ring AG seems to be smaller and easier to control than HG, while still containg a lot of information: for example, ifGis a finiteabelian group AGis the symmetric algebra on the group of char- acters, while HGis much larger (unlessGis cyclic). This is truly surprising to someone who is familiar with the theory of Chow rings of smooth pro- jective algebraic varieties, because these tends to be infinitely more complicated and less computable than their cohomology.

Rationally, the situation is very well understood. If G is a connected algebraic group, then the homomorphism AGQ!HGQ is an iso- morphism, and both rings coincidewith thering of invariants under the

(*) Indirizzo dell'A.: Dipartimento di Matematica, UniversitaÁ di Roma Tre, Largo San Leonardo Murialdo 1, I-00146 Roma, Italy; e-mail: molina@mat.uniroma3.it

(**) Indirizzo dell'A.: Dipartimento di Matematica, UniversitaÁ di Bologna, Piazza di Porta San Donato 5, I-40126 Bologna, Italy; e-mail: vistoli@dm.unibo.it

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Weyl group in the symmetric algebra of the ring of characters of a maximal torus; this is classical, due to Leray and Borel, in the case of cohomology, and to Edidin and Graham ([EG97]) for theChow ring. Furthermore, this ring of invariants is always a polynomial ring, as was shown by Chevalley.

With integral coefficients, the situation is much more subtle.

TheChow ring AGhas been computed for the classical groups GLn, SLn, Spn, On or SOn, but not for thePGLn series. The results are as follows.

Each of the groups above comes with a tautological representation, of di- mensionn(or 2n, in thecaseof Spn). Every representationV of an alge- braic groupGhas Chern classes ci(V)2AiG. WhenGis a classical group, we denote the Chern classes of the tautological representation simply byci.

Burt Totaro ([Tot99]) and R. Pandharipande ([Pan98]) described AG when GˆGLn, SLn, Spn, On and SOn when n is odd. Wewill usethe following notation: ifRis a ring,t1;. . .;tnare elements ofR,f1;. . .;frare polynomials inZ[x1;. . .;xn], wewrite

RˆZ[t1;. . .;tn]= f1(t1;. . .;tn);. . .;fr(t1;. . .;tn)

to indicatethetheringRis generated byt1;. . .;tn, and the kernel of the evaluation mapZ[x1;. . .;xn]!Rsendingxitotiis generated byf1;. . .;fr. When there are nofithis means thatRis a polynomial ring in theti.

First thecaseof thespecial groups.

THEOREM[B. Totaro].

(1) AGLnˆZ[c1;. . .;cn].

(2) ASLnˆZ[c2;. . .;cn].

(3) ASpnˆZ[c2;c4;. . .;c2n].

The first two cases follow very easily from the well known description via generators and relations of the Chow ring of a Grassmannian.

In all threecases, theChow ring is isomorphic to thecohomology ring.

THEOREM[R. Pandharipande, B. Totaro]

(1) AOn ˆZ[c1;. . .;cn]=(2codd).

(2) If n is odd, thenASOnˆZ[c2;. . .;cn]=(2codd).

Thenotation 2coddmeans ``all the elements 2ciforiodd''.

In these cases the Chow ring is not isomorphic to the cohomology ring:

thering HOn was computed independently by Brown (see [Bro82]) and Feshbach ([Fes83]); the result is considerably more involved. The fact that these formulae are so simple is another manifestation of the tamer nature of AG, as opposed to HG.

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Whennis odd, then On'SOnm2, and this allows to obtain theresult for SOn from that for On. When nis even this fails, and the situation is more complicated. Even rationally, the Chern classes of the tautological representation do not generate the Chow ring, or the cohomology. It is well known that when nˆ2m the tautological representation has an Euler class em2H2mSOn, whosesquareis ( 1)mcn: this class, together with the even Chern classesc2,c4;. . .;cn 2generate ASOnQˆHSOnQ. Totaro noticed that whennˆ4 theclass e2 is not in theimageof ASOn; shortly afterwards, Edidin and Graham ([EG95]) constructed a classym2AmSOn, whoseimagein HSOnis, rationally, 2m 1em.

Subsequently, Pandharipande computed ASO4: heshowed that it is generated byc2,c3,c4andy2, and gave the relations (his description of the classy2is different, but equivalent to that of Edidin and Graham). Finally, in her Ph.D. thesis Rebecca Field obtained the general result ([Fie04]), which is as follows.

THEOREM[R. Field]. When nˆ2m is even, then

ASOnˆZ[c2;. . .;cn;ym]= y2m ( 1)m2n 2cn; 2codd; ymcodd : Furthermore there are many results, due to Totaro himself ([Tot99]), to P. Guillot ([Gui04a] and [Gui04c]), and to N. Yagita ([Yag02]), for finite groups. Chow rings of classifiying spaces of exceptional groups have been studied by Yagita (see [Yag04], [Yag05]) and Guillot ([Gui04b]).

As we already mentioned, the PGLn series is much harder (this is an example of a universal phenomenon, that of all the classical groups, these are the ones giving rise to the deepest problems). Fornˆ2 wehavethat PGL2ˆSO3, and for this group everything is well understood. The co- homology withZ=3Zcoefficients of the classifying space of PGL3has been computed in [KMS75], and that of PGLn with Z=2Z coefficients when n2 (mod 4) in [KM75] and [Tod87]; furthermore, several results on the cohomology of PGLpwithZ=pZcoefficients were proved in [VV03]. To our knowledge, not much else was known about the cohomology of the classi- fying spaceof PGLn withZ=pZcoefficients, whenpdividesn.

Concerning the Chow ring, for nˆ3 there is a difficult paper of G. Vezzosi ([Vez00]), where he describes APGL3almost completely. Here is his basic idea. The fundamental tool is the equivariant intersection theory that Edidin and Graham ([EG98]) have forged starting from Totaro's idea.

Vezzosi stratifies the adjoint representationsl3of PGL3by typeof Jordan canonical form, compute the Chow ring of each stratum, and then get generators for APGL3using the localization sequence for equivariant Chow

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groups. To get relations he restricts to appropriate subgroups of PGL3. His technique has been refined and improved by the second author in [Vis05], where he studies the Chow ring and the cohomology of the clas- sifying spaceof PGLp, wherepis an odd prime.

Thepurposeof this articleis to show how this stratification method provides a unified approach to all the known results on the Chow ring of classical groups. Consider a classical group G with its tautological representation V. Then one stratifies V in strata in which thestabi- lizers are, up to an extension by a unipotent group, smaller classical group. Using thelocalization sequence for equivariant Chow groups this gives generators for the Chow rings, with relations that come out naturally. To show that therelations suffice, one restricts to appro- priatesubgroups ofG: a maximal torus first, to show that therelations sufficeup to torsion, then to somefinitesubgroup to handletorsion.

This turns out to bereasonably straightforward for all theclassical groups, except for PGLn. From our point of view, this is due to the fact that the natural representation to use for PGLn, which is theadjoint representation, has a much more complicated orbit structure then in thecases of theother groups.

For thecases of Spn and On, Totaro's proofs, based on his very inter- esting and important [Tot99, Proposition 14.2], are much simpler. In the caseof SOnfor evenn, Totaro's method, as implemented by Field, does not seem easier than the stratification method. In the case of PGLn, the stratification method provides the best known results; but there is also a very recent preprint of Kameko and Yagita where they also compute the additivestructureof APGLnand HPGLn, with completely different methods, using the Adams spectral sequence for Brown-Peterson cohomology ([KN05]).

A few words about the future (1). Despite its elementary nature, the stratification methods is powerful; also, as was pointed out to the second author by N. Yagita, it might yield interesting results when applied to more general cohomology theories. However, it seems clear that to pro- ceed much further one will eventually need to introduce substantial amounts of homological machinery, as provided by the theory of motivic cohomology of Voevodsky and Morel. Thus, the way is indicated by the work of N. Yagita (see for example [Yag03] and [Yag05]).

(1) The authors are well aware of the risks involved in making predictions, as people always play Chesterton's game ``Cheat the Prophet''.

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Acknowledgments. ± Pierre Guillot pointed out an error in the first version of this paper. We thank him heartily. We are also grateful to the referee, who did an extremely careful and competent job.

The second author would like to acknowledge the very interesting discussions he has had with Nobuaki Yagita and Andrzej Weber on the subject of this paper.

2. Preliminaries and notation.

In this section we recall some definitions and notations, and state some tecnical results that will be used throughout this paper.

All schemes and algebraic spaces are assumed to be of finite type over a fixed fieldk. All algebraic groups will be linear algebraic group schemes overk, and all representations will bek-representations. IfXis a scheme overkandk0is an extension ofk, wesetXk0defˆ XSpeckSpeck0.

Thenotation for algebraic groups will bestandard: thusGmwill bethe multiplicativegroup overk, andmnthegroup schemeofnthroots of 1.

LetGa linear algebraic group overk, andX a smooth scheme overk with aG-action.

Edidin and Graham ([EG98]), expanding on the idea of Totaro, have defined theG-equivariant Chow ring ofX, denoted AG(X), as follows. For eachi0, choose a representationVofGwith an open susbschemeUV on whichGacts freely (in which case we call (V;U) agood pair for G), and such that thecodimension ofVnU is greater thani. Theaction ofGon XUis also free, and the quotient (XU)=Gexists as a smooth algebraic space; then Edidin and Graham define

AiG(X)defˆAi (XU)=G

;

where the right hand term is the usual Chow group of rational equivalence classes of cycles of codimensioni. This is easily seen to be independent of thegood pair (V;U) chosen. Then one sets

AG(X)defˆM

i0

AiG(X):

IfGacts freely onX, then there is a quotientX=Gas an algebraic space of finitetypeover k, and theprojectionX!X=GmakesXinto a G-torsor over X=G; and in this casethering AG(X) is canonically isomorphic to A(X=G).

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Totaro's definition of the Chow ring of a classifying space is a particular caseof this, as

AGˆAG(Speck):

The formal properties of ordinary Chow rings extend to equivariant Chow rings. We recall briefly the properties that we need, which will be used without comments in the paper, referring to [EG98] for the details.

Iff:X!Yis an equivariant morphism of smoothG-schemes there is an induced ring homomorphism f:AG(Y)!AG(X), making AG into a contravariant functor from smooth G-schemes to graded commutative rings. Furthermore, iff is proper there is an induced homomorphism of groupsf:AG(X)!AG(Y); the projection formula holds. This means that if h2AG(Y) andj2AG(X), then

f(jfh)ˆfjh;

in other words,fis a homomorphism of AG(Y)-modules.

There is also a functoriality in the group: ifH!Gis a homomorphism of algebraic groups, the action ofGonXinduces an action ofHonX, and there is homomorphism of graded rings AG(X)!AH(X). When H is a subroup ofGwewill refer to this as arestriction homomorphism.

IfHis a subgroup ofG, then there is anH-equivariant embeddingX intoXG=H, defined in set-theoretic terms by sendingxinto (x;1). Then thecompositeof therestriction homomorphism AG(XG=H)!

!AH(XG=H) with thepullback AH(XG=H)!AH(X) is an iso- morphism.

Of paramount importance is the localization sequence; ifYis a closed G-invariant subscheme ofX, and wedenotebyi:Y,!Xandj:XnY,!X the inclusions, then the sequence

AG(Y) !i AG(X) !j AG(XnY)!0 is exact.

Furthermore, if E is a G-equivariant vector bundle on X, there are Chern classes ci(E)2AiG(X), enjoying the usual properties. Also, the pullback AG(X)!AG(E) is an isomorphism.

In particular, since the equivariant vector bundles over Speckarethe representations of G, we get Chern classes ci(V)2AiG for every re- presentation ofG; and thepullback AG!AG(V) is an isomorphism.

We also need other easy properties of equivariant Chow rings, for which we do not have a suitable reference.

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LEMMA2.1. Let G a linear algebraic group, X a smooth G-scheme, H a normal algebraic subgroup G. Suppose that the action of H on X is free with quotient X=H. Then there is canonical isomorphism of graded rings

AG(X)'AG=H(X=H):

PROOF. Le t (V;U) bea good pair forG, such that thecodimension of VnUis greater theni. Then

AiG(X)ˆAi (XU)=G

ˆAi ((XU)=H)=(G=H)

ˆAiG=H (XU)=H :

Now, thequotient (XV)=His aG=H-equivariant vector bundle over X=H, (XU)=His an open subscheme of (XV)=Hwhose complement has codimension larger thani. This yields isomorphisms

AiG=H (XU)=H

'AiG=H (XV)=H 'AiG=H(X=H):

Theresulting isomorphisms AiG(X)'AiG=H(X=H) yield the desired ring isomorphism AG(X)'AG=H(X=H).

LEMMA2.2. Let G be an affine linear group acting on a smooth scheme X, E!X an equivariant vector bundle of rank r. Call E0E the com- plement of the zero section of E. Then the pullback homomorphism AG(X)!AG(E0)is surjective, and its kernel is generated by the top Chern classcr(E)2ArG(X).

PROOF. Call s:X!E the zero-section. Then the statement follows immediately from the exactness of the localization sequence

AG(X) s! AG(E)!AG(E0)!0;

from thefact that thepullbacks:AG(E)!AG(X) is an isomorphism, and from the self-intersection formula, which implies that the composite AG(X) s! AG(E) s! AG(X) is multiplication by cr(E).

LEMMA 2.3. Let H a linear algebraic group with an isomorphism f:H'Ank of varieties, such that for any field extension kk0 and any h2H(k0), the automorphism ofAnk0that corresponds underfto the action of h on Hk0 by left multiplication is affine. Furthermore, let G be a linear

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algebraic group acting on H via group automorphisms, corresponding to linear automorphisms ofAnk underf.

If G acts on a smooth scheme X, form the semidirect product Gj H, and let Gj H act on X via the projection Gj H!G. Then the homo- morphism

AG(X)!AGHl (X)

induced by the projection Gj H!G is an isomorphism.

PROOF. Le t (V;U) (resp. (V0;U0)) bea good pair forGj H(resp.G).

ThenGj Hacts onU0via theprojectionGj H!G: it follows thatGj H acts onXHUU0, and sincetheaction ofGj HonHis transitive, and thestabilizer of theorigin isG, there is an isomorphism

(XHUU0)=(Gj H)ˆ(X(GjH)=HUU0)=(Gj H) '(XUU0)=G:

Look at thefollowing commutativediagram:

Notethatp1 is an affine bundle: in fact, it is a fiber bundle with fiber isomorphic to An, and structuregroup Gj Hthat acts onAn by affine transformations, sincetheaction ofGonHis affineand theaction ofHon itself is affine. It follows from [Gro58a, p. 35] thatp1is an isomorphism. On theother hand, sinceUU0 is an open set of VV0 on which G acts freely,p2 is theidentity on theequivariant Chow ring AG(X), up to a de- gree that can be made arbitrarily large: so we have a commutative triangle

where the horizontal arrow is exactly the map induced by the projection Gj H!G.

Here is another auxiliary result: it is well known (see for instance [Vez00]) that Amn'Z[j]=(nj), where j is thefirst Chern class of the

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character given by the inclusionmn,!Gm. IfGis an algebraic group, we will denote by j2AGmn theimageof junder the map Amn!AGmn in- duced by the projection Gmn !mn. Using theprojectionGmn!G, wecan consider AGmnas an AG-algebra. Then AGmnadmits thefollowing description:

LEMMA2.4. As anAG-algebra,AGmnis generated by the elementj, and the kernel of the evaluation map AG[x]!AGmn sending x intoj is the ideal(nx). In other words,

AGmnˆAG[j]=(nj):

PROOF. See [Vis05, Lemma 4.3].

3. The special groups:GLn,SLnandSpn.

Let us fix a fieldk: wewriteGLn, SLnand Spn for thecorresponding algebraic groups overk.

These groups are always much easier to study: they are special, in the sense that every eÂtaleprincipal bundleis Zariski locally trivial (this ter- minology is due to Grothendieck, see [Gro58b]). For GLnand Spntheidea works in a very similar way: let us work out Spn, which is marginally harder. We proceed by induction onn, thecasenˆ0 being trivial.

Consider V ˆA2n, the tautological representation of Spn, with its symplectic formh:VV !kgiven in coordinates by

h(x1;. . .;x2n;y1;. . .;y2n)ˆx1yn‡1‡. . .‡xny2n xn‡1y1 . . . x2nyn: Denote bye1;. . .;e2n thecanonical basis ofV.

Theorbit structureofVis very simple: there are two orbits, the origin and its complementUdefˆ Vn f0g. Consider the subspace

V0ˆ he1;. . .;en 1;en‡1;. . .;e2n 1i;

therestriction of h to V0 is a non-degenerate symplectic form, and V ˆV0 hen;e2ni. This induces an embedding Spn 1,!Spn, identifying Spn 1with thestabilizer of thepair (en;e2n).

Let G the stabilizer of the element en: then we have that Spn 1GSpn. Thefirst inclusion admits a splitting: ifA2G, thenA stabilizes the orthogonal complement h ien ?. It follows that A induces a linear endomorphism on the quotient h ien ?=h i 'en V0, and this en-

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domorphism is easily seen to preserve the symplectic formhjV0, so it is an element of Spn 1. Thus wehavea projectionG!Spn 1: le tHits kernel, so thatGˆSpn 1j H.

ThestructureofHis as follows; thematrices inHareexactly thosefor which there are scalarsa1;. . .;a2n 1 such that

Aeiˆ

ei ai‡nen if i ˆ 1; . . . ; n 1

en if i ˆ n

ei‡ai nen if i ˆ n‡1; . . . ; 2n 1

a1e2‡. . .‡a2n 1e2n 1‡e2n if i ˆ 2n:

8>

>>

><

>>

>>

:

This yields an isomorphism of varieties H'A2n 1. It is not hard to see that the conditions of Lemma 2.3 are satisfied for the action of Spn 1onH;

hence the embedding Spn 1G induces an isomorphism of rings AG'ASpn1, so thecomposite

ASpn(U)!ASpn1(U)!ASpn 1(en)ˆASpn1

is an isomorphism. The restriction of the representationVto Spn 1is the direct sum ofV0 and of a trivial 2-dimensional representation: hence the Chern classes ciˆci(V) restrict to the ci(V0). From theinduction hy- pothesis, we conclude that ASpn(U) is generated by the images of c2;. . .;c2n 2.

From Lemma 2.2 we conclude that every class in ASpncan bewritten as a polynomial in c2;. . .;c2n 2, plus a multipleof c2n. By induction on the degree we conclude thatc2;. . .;c2n generate ASpn.

To prove their algebraic independence, let us restrict to ATn, where Tn'Gnm is thestandard maximal torus in Spn, consisting of diagonal matrices with entries (t1;. . .;tn;t11;. . .;tn1). Then ATn is thepolynomial

ring Z[j1;. . .;jn], where ji is thefirst Chern class of the1-dimensional

representation given by theithprojectionTn!Gm. Then the total Chern class of therestriction ofVn toTn is

(1‡j1). . .(1‡jn)(1 j1). . .(1 jn)ˆ(1 j21). . .(1 j2n);

hence the restriction of c2i is the ith elementary symmetric function of j21;. . .; j2n. This proves the independence of thec2i.

As we mentioned, the argument for GLnis very similar. For SLn, one can proceed similarly, but it is easier to use the fact that, if GLn acts freely on an algebraic variety U, theinduced morphism U=SLn!

!U=GLn makes U=SLn into a principal Gm-bundleon U=GLn, asso- ciated with the determinant homomorphismdet:GLn!Gm. He nce , by

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Lemma 2.2, wehavean isomorphism ASLn 'AGLn=(c1), which gives us what wewant.

REMARK 3.1. All these arguments work with cohomology, when kˆC. The localization sequence in cohomology does not quite work in the sameway, as therestriction homomorphism from thecohomology of the total space to that of an open subset is not necessarily surjective. However, ifYis a smooth closed subvariety of a smooth complex algebraic varietyX, of purecodimensiond, then there is an exact sequence

!HiG2d(Y)!HiG(X)!HiG(XnY)!HiG2d‡1(Y)! : Hence if we know that either the pullback HG(X)!HG(XnY) is surjec- tive, or the pushforward HG(Y)!HG(X) is injective, we can conclude that we have an exact sequence

0!HG(Y)!HG(X)!HG(XnY)!0;

and this is sufficient to mimic the arguments above and give the result for cohomology.

REMARK 3.2. These results can also be proved very simply from a result of Edidin and Graham (see [EG97]): ifGis a special algebraic group, T a maximal torus andW theWeyl group, thenatural restriction homo- morphism AG!(AT)W is an isomorphism.

4. The Chow ring of the classifying space ofOn.

Let us fix a fieldkof characteristic different from 2. IfV ˆkn is ann- dimensional vector space, we define a quadratic form q:V !k in the standard form

q(x1;. . .;xn)ˆx1xm‡1‡. . .‡xmx2m

whennˆ2m, and

q(x1;. . .;xn)ˆx1xm‡1‡. . .‡xmx2m‡x22m‡1

when nˆ2m‡1. Wewill denoteby On the algebraic group of linear transformations preserving this quadratic form.

THEOREM4.1. [R. Pandharipande, B. Totaro].

AOnˆZ[c1;. . .;cn]=(2codd):

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REMARK 4.2. Let V0 beanother n-dimensional vector space overk, with a non-degenerate quadratic form q0:V0!k. Wecan associatewith this another algebraic group O(q0), which will not beisomorphic to OnˆO(q), in general, unlesskis algebraically closed.

However, one can show that there is an isomorphism of Chow rings AOn 'AO(q0), such that theclasses ci(V) in theleft hand sidecorrespond to theclasses ci(V0) in theright hand side. Theprinciplethat allows to prove this has been known for a long time ([Gir71, Remarque 1.6.7]): it is the existence of a bitorsor I!Speck. This is the scheme representing the functor of isomorphisms of (V;q) with (V0;q0). OnIthere is a left action of O(q0) and right action of On, by composition. These two actions commute, and make I into a torsor under both groups (because (V;q) and (V0;q0) become isomorphic after a base extension).

In general, assume thatGandG0are algebraic groups over a fieldk(in fact, any algebraic space will do as a base), and I!Speck is a (G0;G)- bitorsor: that is, onIthere is a right action ofGand left action ofG0, and this makesIinto a torsor under both groups. IfXis ak-algebraic space on whichG0acts on the left, then we can produce ak-algebraic spaceIGX on whichGacts on theleft, by dividing theproductISpeckXby theright action ofG, defined by the usual formula (i;x)gˆ(ig;g 1x). Theleft action of G0 is by multiplication on thefirst component: thequotients GnX and G0n(IGX) arecanonically isomorphic.

This operation gives an equivalence of the category of G-algebraic spaces with the category of G0-algebraic spaces. When applied to re- presentations, it yields representations, and gives an equivalence of the category of representations of G and of G0. Furthermore, given a re- presentationVofG, with an open subsetUVon whichGacts freely, we get a representation V0ˆIGV with an open subset U0ˆIGU on whichG0acts freely, so that the quotientsGnUandG0nU0areisomorphic.

In Totaro's construction this gives an isomorphism of AGwith AG0. So, in particular, the result that we have stated for On also holds for O(q0) for any other non-degeneraten-dimensional quadratic formq0, and wehave

AO(q0)ˆZ[c1;. . .;cn]=(2codd):

The proof of the Theorem will be split into two parts: first we show that thecigenerate AOn, then that ideal of relations is generated by the given ones.

For the first part we proceed by induction onn.

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Fornˆ1,q(x)ˆx21, and O1ˆm2, so

AO1ˆAm2 'Z[c1]=(2c1):

For n>1, let Bˆ fv2An jq(v)6ˆ0g, and set Qˆq 1(1). Then q:B!Gmis a fibration, with fibers isomorphic toQ. This fibration is not trivial, but it becomes trivial after an eÂtale base change. Set

Be ˆ f(t;v)2GmBjt2ˆq(v)g;

and consider the cartesian diagram

wherethefirst column is projection onto thefirst factor, and thetop row is defined by the formula (t;v)7!tv.

There are obvious commuting actions of m2 and On onB, thefirst de-e fined by e(t;v)ˆ(et;v), and thesecond byM(t;v)ˆ(t;Mv). Thequo- tientB=me 2is isomorphic toB, and theinduced action of Onon thequotient coincides with the given action onB. From Lemma 2.1, we obtain an iso- morphism

AOn(B)'Am2On(B):e

Then there is an isomorphism ofGm-schemesBe 'GmQdefined by theformula (t;v)7!(t;v=t). Thegiven actions ofm2and of On onBe induce commuting actions on GmQ given by e(t;v)ˆ(et;ev) for e2m2 and M(t;v)ˆ(t;Mv) forM2On. These define an action ofm2OnonGmQ, and AOn(B) is isomorphic to Am2On(GmQ).

This action of m2On on GmQ extends uniquely to an action of m2OnonA1Q, defined by the same formulae. This action is defined by two separate action onA1andQ, and theaction onA1is linear, defined by thenon-trivial character ofm2through theprojectionm2On!m2. Callj the first Chern class of this representation. From Lemma 2.2, we have an isomorphism

Am2On(GmQ)'Am2On(Q)=(j):

…4:1†

To investigate Am2On(Q) wewill also usean orthogonal basise01;. . .;e0n ofV, in whichqhas theform

q(x1e01‡. . .‡xne0n)ˆx21‡. . .‡x2m x2m‡1 . . . x2n

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whennˆ2m, and

q(x1e01‡. . .‡xne0n)ˆx21‡. . .‡x2m‡1 x2m‡2 . . . x2n whennˆ2m‡1.

Now, theaction ofm2OnonQis transitive; letHthestabilizer of the pointe012Q. ThestructureofHis as follows. SetV0defˆhe02;. . .;e0ni, so that Vis theorthogonal sumhe01i V0, and callq0therestriction ofqtoV0. Then thegroup Oq0 of linear automorphisms of V0 preserving q0 is naturally embedded into On, as thestabilizer ofe01. Noticethat in an appropriate basisq0has thestandard form

q0(x1;. . .;xn 1)ˆx1xm‡1‡. . .‡xmx2m

whennˆ2m‡1, and theoppositeof thestandard form q0(x1;. . .;xn 1)ˆ (x1xm‡. . .‡xm 1x2m 2‡x22m 1)

when nˆ2m; in both cases the orthogonal group O(q0) is isomorphic to On 1, and weidentify it with On 1.

Thestabilizer ofe01 inm2On is thegroupm2On 1, embedded into m2On with theinjectivehomomorphism

(e;M)7!(e;eM):

It follows that

Am2On(Q)'Am2On (m2On)=(m2On 1) 'Am2On1:

Weobtain a chain of isomorphisms

AOn(B)'Am2On(Q)=(j) Am2On 1=(j):

Finally, from Lemma 2.1 we get an isomorphism Am2On1=(j)'AOn1[j]=(j)

'AOn1:

ThecompositeAOn!AOn(U)!AOn1 is thepullback induced by theem- bedding On 1On.

Therestriction ofV to On 1 is thedirect sum ofV0 and a trivial 1-di- mensional representation, hence the restriction AOn !AOn1carriesciinto ci(V0). Therefore, by induction hypothesis, the images ofc1;. . .;cn 1gen- erate AOn(B).

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Next, we claim that the restriction homomorphism AOn(Ann f0g)!

!AOn(B) is an isomorphism. To see this, set Cˆ fv2Ann f0g jq(v)ˆ0g

with its reduced scheme structure, and consider the fundamental exact sequence

AOn(C) !i AOn(Ann f0g)!AOn(B)!0:

We need to show that i is thezero map. In fact, q:Ann f0g !A1 is smooth, sincethecharacteristic of thebasefield is not 2, so C is the scheme-theoretic inverse image of f0g. The map q:Ann f0g !A1 is On-equivariant, if we let On act trivially on A1; and thefundamental class [0]2AOn(A1) equals zero. Sincetheinverseimageof [0] in AOn(Ann f0g) is [C], wecan concludethat

[C]ˆ02AOn(Ann f0g):

Next we show that the pullbacki:AOn(Ann f0g)!AOn(C) is surje ctive : in this case, for every a2AOn(Cn f0g), wehaveaˆib for some b2AOn(Ann f0g), so

i(a)ˆii(b)ˆ[C]bˆ0

by theprojection formula, and i is the zero map, as claimed.

To show surjectivity, notice that the action of OnonCis transitive. Let us investigate the stabilizer G of e12C. Se t nˆ2m or nˆ2m‡1, as usual. If wedefine

V0ˆ he2;. . .;em;em‡2;. . .;eni

then the restriction ofqtoV0has thestandard form, andVis theorthogonal sumV0 he1;em‡1i. This gives an embedding On 2On, identifying On 2

with thestabilizer of thepair (e1;em‡1).

An analysis very similar to that we have carried out for the stabilizer of a vector under Spnleads to the conclusion that the stabilizer Gofe1 is a semidirect product On 2j H, whereHis isomorphic toAn 1 as a variety, the action of an element ofHon itself is given by an affine map, and the action of On 2 on H is linear: by Lemma 2.3, the embedding On 2G induces an isomorphism of rings AG'AOn 2, so thecomposite

AOn(C)!AOn2(C)!AOn2(e1)ˆAOn2

is an isomorphism. But thecirestrict in AOn2 to theChern classes ofV0: hence, by inductions hypothesis, they generate AOn2. Hence the pullback

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AOn !AOn(C) is surjective, as claimed. This ends the proof that the ci

generate AOn. Let us investigate the relations.

Thequadratic formqinduces an isomorphism V 'V_ of representa- tions of On, hence for eachiwehaveci(V)ˆ( 1)ici(V). This shows that 2ciˆ0 wheniis odd.

To show that these generate the ideal of relations among the ci,

let JZ[x1;. . .;xn] be the ideal generated by 2x1, 2x3;. . .. Le t

P2Z[x1;. . .;xn] be a homogeneous polynomial such thatP(c1;. . .;cn

ˆ02AOn: we need to check thatPis inJ. By modifyingPby an element of J, wemay assumethatPis of theformQ‡R, whereQis a polynomial in the evenxi, whileRis a polynomial in which every monomial contains some xiwithiodd, and all of whose coefficients are either 0 or 1.

LetTm'Gmmbethestandard torus in On: the embeddingTmOnsends (t1;. . .;tm) into thediagonal matrix with entries (t1;. . .;tm;t11;. . .;tm1) if nˆ2m, and (t1;. . .;tm;t11;. . .;tm1;1) if nˆ2m‡1. Then ATmˆ

ˆZ[j1;. . .;jm], where ji is thefirst Chern class of theith projection

xi:Tn !Gm. Therestriction of V to Tn splits as rdefˆx1‡. . .‡xm‡

‡x11‡. . .‡xm1whenmis even, andr‡1 whennis odd. Hence the total

Chern class of the restriction ofV toTnis

(1‡j1). . .(1‡jm)(1 j1). . .(1 jm)ˆ(1 j21). . .(1 j2m);

and this means that the restrictions of theciis 0 wheniis odd, whilec2j restricts to thejthsymmetric function of j21;. . .; j2m. Hence the restric- tions of even Chern classes are algebraically independent. In the decom- position 0ˆP(c1;. . .;cn)ˆQ(c2;. . .;c2m)‡R(c1;. . .;cn) thesummand R(c1;. . .;cn) restricts to 0, soQ(c2;. . .;c2m) also restricts to 0. This implies thatQˆ0. So wehavethatPhas coefficients that are either 0 or 1.

Now takea basise01;. . .;e0nofVin whichqhas a diagonal form. Consider thesubgroupmnnOn consisting of linear transformations that take each e0iintoe0ior e0i. If wecallhithefirst Chern class of thecharacter obtained composing theithprojectionmnn!mn with the embeddingmn,!Gm, then by Lemma 2.4 we have

AmnnˆZ[h1;. . .;hn]=(2h1;. . .;2hn):

There is a natural ring homomorphism from Amn

ninto thepolymomial ring F2[y1;. . .;yn] that sends eachhiintoyi. Therestriction ofVtomnnhas total Chern class (1‡h1). . .(1‡hn); hence the image ofciinF2[y1;. . .;yn] is the ithelementary symmetric polynomialsiin theyi. Thesiarealgebraically independent inF2[y1;. . .;yn], theimageof 0ˆP(c1;. . .;cn) isP(s1;. . .;sn), and P has coefficients that either 0 or 1. This implies that Pˆ0, and completes the proof of the theorem.

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5. The Chow ring of the classifying space ofSOn.

Let kbe a field of characteristic different from 2, setV ˆkn, and let q:V !kbe the same quadratic form as in the previous section. Consider thesubgroup SOn On of orthogonal linear transformations of determi- nant 1.

Ifnis odd, ASOn can be easily computed from AOn, as was noticed in [Pan98] and [Tot99].

THEOREM5.1. [R. Pandharipande, B. Totaro]. If n is odd, then ASOn ˆZ[c2;. . .;cn]=(2codd):

PROOF. When is nodd there is an isomorphism On'mnSOn; the determinant characterdet:On!mn (whosefirst Chern class in AOn isc1) corresponds to the projection mnSOn!mn. Then from Lemma 2.4 we get that

ASOn'AOn=(c1) and theconclusion follows.

5.1 ±The Edidin-Graham construction

From now on weshall assumethatnis even, and writenˆ2m.

In this case, ASOnis not generated by the Chern classes of the standard representation, not even rationally. This can be seen easily fornˆ2. We havethat SO2consists of matrices of the form

t 0 0 t 1

and so is isomorphic toGm. Then

ASO2ˆAGm ˆZ[j];

wherejis the first Chern class of the tautological representationLˆA1, on whichGmacts via multiplication. HenceVˆLL_, so c2(V)ˆ j2.

For generaln, thevector spaceVwill still split as thedirect sum of two totally isotropic subspaces, one dual to the other: however, whenn>2 this splitting is not unique, and the totally isotropic subspaces are not invariant under the action of SOn, so V is not a direct sum of two nontrivial re- presentations (and V is in fact irreducible). Still, in topology V has an

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Euler classem2H2mSOn, whosesquareis ( 1)mcm. Let us recall Edidin and Graham's construction of an algebraic multiple ofem(see [EG95]).

In what follows we will use the classical conventions for projectiviza- tions and Grassmannians; those seem a little more natural in intersection theory than Grothendieck's. So, ifWis a vector space, we denote byP(W) the vector space of lines inW, and byG(r;W) theGrassmannian of sub- spaces of dimensionr; and similarly for vector bundles.

Denote by I(m;V) thesmooth subvariety of G(m;V) consisting of maximal totally isotropic subspaces of V. It is well known that On acts transitively on I(m;V), and that I(m;V) has two connected components, each of which is an orbit under the action of SOn. Let us choose one of the orbits, for example, the one containing the subspace he1;. . .;emi. Every totally isotropic subspaceof dimensionm 1 ofV is contained in exactly two maximal totally isotropic subspaces, one in each connected component.

There is a well known equivalence of categories between On-torsors and vector bundles of ranknwith a non-degenerate quadratic form. IfEis a vector bundle on a schemeX with a non-degenerate quadratic form, this corresponds to a On-torsorp:P!X, the torsor of isometries betweenE and VX; with this torsor wecan associatea m2-torsor (that is, an eÂtaledoublecover) P=SOn!X via the determinant homomorphism det:On!m2. This cover can be described geometrically as follows.

Consider the subschemeI(m;E) of totally isotropic subbundles in the relative Grassmannian G(m;E)!X ; theprojection I(m;E)!X is proper and smooth, and each of its geometric fibers has two connected components. Let I(m;E)!eI(m;E)!X be the Stein factorization; then eI(m;E)!X is an eÂtale double cover, and is precisely the double cover P=SOn !X. This can be seen as follows.

OnPwe have, by definition, an isometry ofpEwithVP. InVP wehavea maximal totally isotropic subbundlehe1;. . .;emi P, so we get a maximal totally isotropic subbundleof pE. This defines a morphism P!I(m;E) over X; thecompositeP!I(m;E)!eI(m;E) induces the desired isomorphismP=SOn'eI(m;E).

Hence, giving a reduction of structure group of P!X to SOn is equivalent to assigning a sectionX!eI(m;E). This yields an equivalence of thegroupoid of SOn-torsors onX with the groupoid of vector bundles E!X of rank n with a non-degenerate quadratic form, and a section X!eI(m;E). We shall refer to such a structure as an SOn-structure on E.

Furthermore, given an SOn-structureonE, iff:T!Xis a morphism of algebraic varieties, andLis a totally isotropic subbundleoffEof rank m, wesay that L is admissible if theimageof T under the morphism

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T!I(m;X) corresponding toLis contained in the inverse image of the given embeddingXeI(m;E).

Here is the construction of Edidin and Graham ([EG95, Section 6]).

We will follow their notation. LetEbea vector bundleof ranknwith an SOn-structure on a smooth algebraic variety X. For e ach iˆ1;. . .;m consider the flag variety fi:Qi!X of totally isotropic flags

L1L2. . .Lm iE, with e achLs of ranks. For eachi, de note by

L1L2. . .Lm ifiEtheuniversal flag on Qi. Therestriction of

thequadratic form to L?m i is degenerate, with radical equal to Lm i; hence onQithere lives a vector bundleEidefˆ L?m i=Lm iof rank 2iwith a non-degenerate quadratic form. For each iˆ1;. . .;m 1 wehavea projection pi:Qi 1!Qi, obtained by dropping the last totally isotropic subbundlein thechain; and Qi 1 is canonically isomorphic, as a scheme overQi, to thesmooth quadric bundleinP(Ei) defined by the quadratic form on Ei. This me ans that Qi 1 is a family of quadrics of dimension 2(i 1) overQi. Le t us de note byhi2A1(Qi 1) therestriction toQi 1 of theclass c1 OP(Ei)(1)

2A1 P(Ei) .

Each bundleEihas a canonical SOn 2i-structure. Callpi:L?m i!Eithe projection. From each totally isotropic vector subbundle LEi of rank m i, we get a totally isotropic vector subbundle piLL?m ifiE of rankm; thenLis admissibleif and only ifpiLis admissible.

Theuniversal flagL1L2. . .Lm 1f1EonQ1can becompleted in a uniqueway to a maximal totally isotropic flag L1. . .Lm 1 Lmf1Ein such a way thatLmis admissible. Then Edidin and Graham define

ym(E)ˆf1 scm(Lm)

2Am(X) where we have set

sˆh22h43. . .h2mm 22A(Q1):

REMARK 5.2. In this formula each of the classes hishould bepulled back to Q1. Here, and in what follows, we use the following convention:

whenf:Y!X is a morphism of smooth varieties, andj2A(X), wewill also writejforfj2A(Y). Similarly, ifE!Xis a vector bundle, we will also write EforfE. This has theadvantageof considerably simplifying notation, and should not lead to confusion. With this notation, when f is proper the projection formula reads: ifj2A(X) andh2A(Y), then

f(jh)ˆjfh:

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