C OMPOSITIO M ATHEMATICA
Y VES A NDRÉ
Mumford-Tate groups of mixed Hodge structures and the theorem of the fixed part
Compositio Mathematica, tome 82, n
o1 (1992), p. 1-24
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1
Mumford-Tate groups of mixed Hodge
structuresand the theorem of the fixed part
YVES
ANDRÉ
CNRS, Institut H. Poincaré, Il rue P. et M. Curie, 75231 Paris 5, France
Received 12 April 1988; accepted 14 April 1991
© 1992 Kluwer Academic Publishers. Printed in the Netherlands
This paper grew out of an
attempt
ofunderstanding group-theoretically
theconsequences
of Hodge theory
which areexplained
inDeligne [D2] II 4,
with aneye towards
applications
toalgebraic independence.
After some
preliminaries
aboutrepresentations
of linearalgebraic
groups, we define andstudy
Mumford-Tate groups of mixedHodge
structures overnoetherian
subrings
R of the fields of real numbers.Though
in thesequel
werestrict ourselves to the crucial case R =
Z,
we refer to theappendix
for astudy
of some
pathologies
which may occur in the case of otherground rings.
We thenturn to a more
precise study
of Mumford-Tate groupsarising
from 1-motives(see [D2] III 10).
In Section 4 a mild
generalization
of a resultby Deligne
about themonodromy
of variation ofHodge
structure isgiven;
we alsopresent
our mainobject
ofstudy,
that is Steenbrink-Zucker’s notionof a good
variation of mixedHodge
structure.In Section
5,
wegive
agroup-theoretic
formulation of the theorem of the fixedpart proved
in[SZ]:
for almost all stalks of agiven polarizable good
variation ofmixed
Hodge
structure, the connectedmonodromy
groupHx
is a normalsubgroup
of the derived Mumford-Tate group!0Gx.
We then statestraightfor-
ward consequences about
monodromy
groups. In the nextparagraph,
westudy
how
big
canHx
be inGx;
we endby applying
these considerations to thestudy
of
algebraic independence
of abelianintegrals depending
on someparameters.
1. Some facts about linear
algebraic
groupsLet K be a field of characteristic
0,
and V ééKN
some K-vector space. We shall consider a closedalgebraic subgroup
G ofGL(V)
=GLN.
Fornon-negative integers
m, n, we set Tm,n =Tm,n(v)
=V@m
(Dj1@n,
wherej1
denotes the dualspace of V
(with
thecontragredient
action ofGLN). By ’representation
of G’ or’G-module’,
we shallalways
mean a finite-dimensional rational one. Thefollowing
twoproperties
are well-known[W] 3.5, §16.1, [DM] 1,
3.1:(1)
everyrepresentation
of G is asubquotient representation
of a finite directsum of
Tm,ns,
(2)
G is the stabilizer of some one-dimensional L in some finite direct sum0153
Tmi,ni: G = Stab L.For any
representation
W ofG,
and any characterx E XK(G)
of G overK,
we denoteby WG
the fixedpart
of W under G andby
WX the submodule of W onwhich G acts
according
to x. We writeEndG W
for theendomorphisms
of the G-module W,
so thatEndG W = (EndK W)G,
and we denoteby Z(EndG W)
its center.LEMMA 1. Assume that G is
connected,
and let H c G be a closedsubgroup.
Thefollowing
conditions areequivalent:
(i)
H aG,
thatis,
H is normal inG,
(ii) for
every tensor spaceT m’n, and for
every X EX K (H), (Tm,n)x
is stable underG, (iii)
everyH-isotypical
componentof
anyrepresentation of
G is stable under G.If
moreover G isreductive,
these conditionsimply
thatZ(EndH V)
cZ(EndGV).
Proof. (iii)=>(ii)
isobvious,
and we shall first prove that(ii)=>(i), independently
of the connectedness
assumption
on G. We knowby (2)
that there exists someone-dimensional L in some
0153
T"‘l’"1 such that H = Stab L. Let W be the G- modulespanned by
L. The line L defines a characterX EX K(H);
we haveL c
W x,
and WX = W n(OE) Tmi,n1)~
=W, according
to thehypothesis (ii).
Let ç be the naturalmorphism
G ~GL(End W);
it is clear that H c ker 9.Conversely
ifg E ker 9, g commutes with any
endomorphism
ofW,
thatis, g
isscalar;
thisimplies that g
stabilizesL,
sothat g
E H. Hence H =ker ç
is a normalsubgroup.
We now prove
(i)=>(iii).
Let W be aG-module,
and W’ the G-submodule of thesum of its irreducible submodules. It suffices to prove that the
H-isotypical components
of W’ are G-stable. LetH’,
G’ denote the naturalimages
of H and Grespectively
inGL(W’),
so that H’ r> G’. Thenormality property implies
that(End W,)H’
is stable underG’,
inside the G’-module End W’. For w EEndH, W’,
letCw
be the kernel of the commutator map[w,.]
inEndH’W’.
It is easy to derive the formulagCw = Cgw,
so thatZ(EndHW) = nWEEndH’W’ Cw
isagain
a G’-module. But
Z(EndH’W’)
is a finite-dimensionalsemi-simple algebra
over K.Moreover G’ acts on
EndH- W’ by gç(x)
=g~(g-1x),
henceg(~ 03C8)
= g~°g03C8,
andthis
gives
rise to amorphism
from G’ to the étale group schemeAutK(Z(EndH’W’)). By
the connectedness ofG’,
thismorphism
has trivialtarget,
thatis, Z(EndH’W’)
is a trivial G’-module. Now theH-isotypical components
of W’ aregiven by p. W’, where p
runs among the minimalindempotents
ofZ(EndH’W’). We just proved
that p commutes with the action of G’ onW’,
andthis
implies
thatp. W’
is stable under G’.When G is
reductive,
we haveV’ = V,
and the aboveproof
showsthat
Z(EndHV)
is a trivialG-module,
whence an obviousimbedding
Z(EndHV)
cZ(EndG v).
D2. Mumford-Tate groups and mixed
Hodge
structuresWe first recall some definitions. Let R be some noetherian
subring
of R such that K :=R ~ZQ
is a field. Let V be a noetherian R-module. A(pure R-) Hodge
structure of
weight
M ~ Z on V is amorphism
h:Resc/R Gm -+ GL(V~R R)
suchthat
hw(x)
is themultiplication by x";
here w denotes theembedding GmR Resc/R Gm given by
Rx c C’.Equivalently,
it is abigraduation
onV ~R C =-
Yp’q withVp,q = Yq’p,
or adecreasing
filtration FP onCc
such thatF Vc (Fp = Vp’,M-p’).
Forinstance,
there isone and
only
oneHodge
structure ofweight - 2M
on V =(203C01)M R,
calledthe
’Tate-Hodge
structure’ and denotedby R(M).
Apolarization
of theHodge
structure
(V,h)
ofweight
M is amorphism
ofHodge
structures(in
the obvioussense)
such that is a scalarproduct
onVR:= V & R.
Elements ofTm,"(V,):= V~m
Q(Hom(V, R))~n (8)z
0(endowed
with the naturalK-Hodge-structure of weight (m - n)M)
which are oftype (0,0)
are called’Hodge
tensors’. In factHodge
tensors arenothing
butelements of
F0(Tm,n(VC)) ~ Tm,n(VK)
ofweight
0(and
thus m =n).
A mixed
R-Hodge
structure(MHS)
is a noetherianR-module E together
witha finite
increasing
filtration W. of theK-space YK := V~ZQ,
and a finitedecreasing
filtration F* ofVC
such that foreach n, (GrWn(VK), GrWn(F))
is a K-Hodge
structure ofweight
n. We say that a M.H.S. V is oftype
e c Z x 7 if itsHodge
numbers hp’q are 0 for(p, q) ~ 03B5,
and that it is trivial if it isof type {(0, 0)1.
The
category
of mixedK-Hodge
structures in an abelian K-linear tensorcategory ([D2]
Th.1.2.10),
which isrigid
and has an obvious exact faithful K-linear tensor functor co:
(VK, W, F) ~ YK.
For a fixed mixedR-Hodge
structure(V, W, F’), let V>
denote the Tannakiansubcategory generated by ( YK, W, F’),
and Wy the restriction of the tensor functor w
to V>;
in otherwords, V>
is thesmallest full
subcategory containing (V., W, F*)
and the trivialK-M.H.S.,
andstable under
ED, p,
andtaking subquotients.
Then the functorAut~(03C9V)
isrepresentable by
some closedK-algebraic subgroup
G =G(V)
ofGL(VK),
and 03C9V defines anequivalence
ofcategories V> RepK G,
cf.[DM] II, 2.11.
We call Gthe Mumford-Tate group
of (V, W, F’).
LEMMA 2.
(a) Any tensor fixed by
G in some Tm,n is aHodge
tensor(an
elementof FO(Tm,n(vc))
nWo Tm,n(vK)),
and G is thebiggest subgroup of GL(YK) which fixes Hodge
tensors.(b) If (V, W, F*)
arisesfrom
pureHodge
structure(V, h),
G is the K-Zariski closureof
theimage of
h inGL(VK) (hence
G isconnected),
andif
moreover V ispolarizable,
then G is reductive.(c)
1 ngeneral,
G preservesW,
and theimage of G
inGL(GrWVK)
isG(GrWVK);
infact G(V)
is an extensionof G(GrWVK) by
someunipotent
group(hence
it isconnected);
inparticular if
V ispolarizable, G(GrWVK)
is thequotient of
Gby
itsunipotent
radical.REMARK. This definition of Mumford-Tate group is
slightly
different from thatgiven
in[DM] 1,
3.2 in the case of pureHodge
structures; if theweight
isnon-zero,
however,
this leads to anisogenous
group.Proof of
the lemma.(a) Any
invariant tensor 1 under G spans a trivialrepresentation LK corresponding
to aMHS,
sayL,
such thatL>
isequivalent
to
VectK.
Thus L is a trivialMHS,
that is to say, 1 is aHodge
tensor.By (1.2),
weknow that G is the stabilizer of some line
LK
in~ Tmi,nï,
whichcorresponds
to aM.H.S. of rank one
(up
toisogeny),
thatis,
to someTate-Hodge
structureL =
R(N1).
If theweight
of V is zero,N 1=
0 and G =Fix(l)
for anygenerator
of L. If theweight
of V is non-zero, there exists aninteger
N such that theweight
ofDet
WN(VK),
sayN2,
is non-zero.Taking
if necessaryVK
instead ofVK,
one canassume moreover that
N1
andN2
have the samesign.
Let r be the rank of the MHSWN(VK)
overK,
and let 1 be agenerator
of the one-dimensionalsubspace
L~|N2|K ~ (^rWN(VK))~2|N1|
inside(~ Tmi,ni)~|N2|
Q.
Then G =Fix(l).
(b)
Thearguments given
in[DM] 1, 3,
4-6 prove the statement about pureHodge
structures.(c)
G preserves W because eachWK
is a mixedK-Hodge
substructure ofVK.
Infact since
GrWVK>
is a Tannakiansubcategory of V>,
G maps ontoG(GrWVK).
Now let P be the
subgroup
ofGL(VK)
whichrespects
theweight
filtrationW.,
andN be the
subgroup
of P which actstrivially
onGrW(VK).
Then G c P and N isunipotent.
MoreoverG(GrWVK)
is theimage
of G inPIN.
Hence G is anextension of
G(GrWVK) by
a(necessarily unipotent) subgroup
of N. 1:1REMARK. The
description
of Mumford-Tate groupsby
their invariant tensorsimplies
some restrictions on the groups which may occur; forexample,
G cannotbe a Borel
subgroup
ofGL(VK),
cf.[DM] 1,
3.2.However,
there are other restrictions on the structure of Mumford-Tate groups, as we shall see now:LEMMA 3. Let G be the
Mumford-Tate
groupof
some M.H.S. overR, say V,
such that
GrW V is polarizable.
Then the abelianized groupGab = G/DG
isa torus. The group
of
realpoints of
itsquotient G bIG b
nGm
is compact(G.
=homothety group).
Proof.
Since allmorphisms in V>
arestrict,
one hasGrWV’ ~ ObGrWV>
forany V’ E Ob V),
thusGrWV’
ispolarizable.
Take for V’ the MHScorresponding
to a faithful
representation VK
of thequotient
U ofGab by
its maximal torus. We find thatG(GrWV’)
= 0(see
Lemma2).
ThusV’,
which is a successive extension of trivialHS,
is also a trivialHS,
andG(V’)
= U = o. Now let V’correspond
to afaithful
representation
of thequotient
ofGab by
its homotheties. The Tate-Hodge
structure Det V’ must betrivial,
i.e. V’ hasweight
0. Therefore thepolarization
is a scalarproduct.
BecauseGab/Gab .G.
actsby orthogonal
transformations,
it iscompact.
DREMARK. The same
argument
shows in the same situation that if G isnilpotent,
then G =G.
x T(or
G = T if V is pure ofweight 0),
where T denotes acompact
torus.3. Mumford-Tate groups of 1-motives
We recall that a 1-motive over
C,
denotedby M = [HE],
is thefollowing
data:
(i)
an extension 0- T-E-A -0 of an abelianvariety
Aby
a torusT, (ii)
amorphism
u from a free abeliangroup X
toE(C).
One associates to a 1-motive a mixed
Hodge
structure V =V(M) = (VZ, W, F.), given by:
Vz = {(l, x)
e Lie E xH/exp
1 =u(x)}
Wo vu
W-1 = H1(E)
Q Q(thus Gr-1 ~ H1(A)
ispolarizable) W-2 = H1(T)~Q
FO
=Ker(Ve ~C ~
LieE).
Morphisms
of 1-motivesbeing
defined in the obvious way, this rule M ~V(M)
defines a functor which is an
equivalence
ofcategories
with thecategory
of torsion-free Z-MHS oftype {(0, 0), (0, -1), ( -1, 0), ( -1, -1)}
withpolarizable Gr-1 ([D2] III, 10.1.3).
We denoteby
G the Mumford-Tate groupof E
andby G-1
that ofW-1.
Let E’ be the connectedcomponent of identity
in the Zariski closure ofu(H),
and let us write F : =(End E’) Q
Q.PROPOSITION 1. Let H G such that
WH0 ~ W-1 (for
instance wemay take
H = G).
Let us assume that E is asplit
extension(E = A
xT).
Then
U(H): = Ker(H~G(W-1))
iscanonically isomorphic
toU:=
HomF (F . u(H); H1(E’)
QQ).
Proof (inspired by
Kummer’stheory
of divisionpoints
on abelianvarieties).
Let us first remark that the
0-MHS Vu
does notchange
if onereplaces Y by
anysubgroup
of finite index. After such areplacement (which
therefore does notaffect
G),
one may assume thatu(H)
has notorsion,
and that E’ is the Zariski closure ofu(H).
Given m =
(1, x)
EVz,
the mapU(H) ~ W- 1:
a H 6m - mdepends only
on
u(x)
and therefore defines aG-equivariant homomorphism U(H) HomZ(u(H); W- 1).
Thevanishing
of~(03C3) implies
that a- fixesWo,
which isa faithful
representation
ofH;
thus6 =1,
and this shows theinjectivity
of (P.Because of Poincaré’s
complete reducibility
lemmaapplied
toproducts
ofabelian varieties and
tori,
the exact sequence of 1-motives0 ~
[X -+ E’]
~[H ~ E] ~ [0 - E/E’] ~
0splits (up
toisogeny,
i.e. in thecategory
ofQ-MHS).
From this follows an
equality
of kernels:Ker(H -+ G(W-1))
=Ker(H - G(H1(E’)))
nKer(H ~ G(H1(E/E’))
~
Ker(H’ ~ G(H1(E’))),
where H’ = H n
G(V([H E’])). Thus 9
factorizesthrough Homz(u(f!l); Hi(E’)
(8)Q);
also it is
easily
seen that elements in theimage
of ç are F-linear in the sense that~(U(H)) ~ if.
Replacing
Eby
E’ and Xby u(H),
we may now assume that u is a dominantembedding
andidentify
lt andu(H).
Since E is a
split extension,
we have F ~EndG W-1
1(this
is because thecategory
ofproducts
of abelian varieties and tori up toisogeny
isequivalent
tothe
category
ofpolarizable Q-Hodge
structures oftype {(-1, -1), ( -1, 0), (0, -1)}),
whenceEndG_1 U ~ (EndF FH)op;
also W- 1, whenceÛ (with
trivialaction of G-1 on
FX),
is asemi-simple
G-1-module.
Thus~(U(H))
is the kernel of some G-i-equi variant endomorphism gl
ofÛ;
that is to say, there existsf ~
Fsuch that
(03C8~(03C3))·
Va EU(H),
~m E FY. If(p(U(H» if,
then03C8 ~ 0,
therefore we can find x ~ FY such thatU(H)x
= x and x ~ 0.We set
Hx = Zx, Mx = [Hx E],
and we denoteby
asubscript
x theobjects Gx, vx
etc. associated to this 1-motive. BecauseU(H)x = x,
there is a naturalinjection Hx=HnGx ¿ GL(WX, - 1).
Since Esplits, Wx, -1 ~ W- 1 is
a direct sumof
polarizable
pureHodge
structures, so thatHx Gx
is reductive. ThereforeWx,-1
is a direct summand in theHx-module Wx,o,
which means that we couldchoose
x~Wx,-1
so thatHxx = x : indeed, Hx
actstrivially (like Gx)
onWx,0/Wx,-1
whosetype
is(0,0).
Recall thatWH0 ~ W-1;
thisimplies
thecorresponding
inclusionWHxx,0 ~ Wx,-1
since H commutes with the action of F.Therefore we
get
acontradiction,
and deduce that~(U(H))
=if.
COROLLARY.
If
Esplits,
with non-trivial abelian part, one has asplit
exactsequence 0 ~
Û ~
G -G(H1(A)) ~
0.REMARK. If one
drops
theassumption
that Esplits, U(G)
can be much smaller thanif.
In ’Deficientpoints
on extensions of abelian varietiesby Gm’
J. NumberTheory (1987),
O.Jacquinot
and K. Ribet have constructed someexamples (by
means of
endomorphisms
of A which areantisymmetric
withrespect
to apolarization)
whereU(G) = 0, corresponding
to some self-dual 1-motives.4. Variations of mixed
Hodge
structureIn the
sequel
we shall concentrate on the case R = Z(see
theAppendix
for otherground rings). By
a variation ofMHS,
we shall mean afinitely
filteredobject
inthe
category
of localsystems
of noetherian Z modules over a fixed connectedcomplex
manifoldX, (yz, W.), WnVZ ~ Wn+1VZ,
together
with adecreasing
filtration of thecomplex bundle Vi
attached toVC: = Vz 0 C by
sub-bundlesFP,
such that on each fibreVZ,s, (W, F*)
induces aMHS and that the flat covariant derivative V satisfies VFP c
Fp-1 ~ 03A91X.
Amorphism
of variation of MHS is amorphism
of localsystem
whichrespects
W and whosecomplexification respects
the filtration FPpointwise.
Thisyields
anabelian
category (any morphism
isstrictly compatible
with thefiltrations).
One calls such a variation
(Vz, W, F*)
a(graded-) polarizable
one if each of thelocal
systems GrWnVZ
carries a bilinear form with values inZ(-n)X
which is amorphism
of localsystems
andpointwise
apolarization. Any subquotient
of apolarizable
variation and anyobject isogenous
to apolarizable
one arepolarizable.
Theintegral
relativecohomology
modules of thecomplement
of adivisor with
relatively
normalcrossings
in aprojective
smooth scheme over analgebraic variety
X furnishexamples
ofpolarizable
variations of MHS over X(see [Kz]
4.3 forinstance).
For a variation ofMHS,
and for apoint
x ofX,
wedenote
by Hx
the connectedmonodromy
group, that is the connected compo-nent of
identity
of the smallestalgebraic subgroup
ofGL(PoJ containing
theimage of 03C01(X, x).
We also denoteby Gx
the Mumford-Tate group of the MHS carriedby
the stalkVZ,x.
LEMMA 4
(cf. [D3] 7.5).
On the(pathwise connected) complement X of
somemeager subset
of X, Gx
islocally
constant.If
the variation ispolarizable,
thenHx
cGx for
anyx E X.
Proof.
For apolarizable
variation of pureHodge
structure, this is stated in loc. cit. We shall write down a detailedproof, though (thanks
to Lemma2)
thereis no new
complication
in the mixed case. LetX
be the universalcovering
of(X, 0),
for some basepoint
0 E X. The inverseimage
of the(polarized)
variationof MHS is a
(polarized)
variation of MHS overX, whose underlying
filteredlocal
system (VZ, W.)
is constant. For l ETm,n(0393VQ) ~ Tm,n(Va,o),
we setSince
FOWo
is asubbundle, X(l)
is ananalytic subvariety
ofX,
and its naturalprojection rc*X(l)
on X is ananalytic subvariety
too. We setwhich is a
(dense)
countable intersection of dense open subsets of X.By
definition
of X,
any 1 ETm,n(0393VQ),
whose stalk at some xo En -1 X
is aHodge
tensor, is in fact a
Hodge
tensor at everypoint
ofX.
For xE X, Gx
is then thebiggest subgroup
ofGL(VQ,x)
which fixes the various tensors inTm,n(VQ,x)
whichlift to
F0Tm,n(0393VC).
ThereforeGx
islocally
constant onX .
We now assume that the variation ispolarized
and we shall see that03C01(X, x)
acts(through
a finitegroup)
on the spacesHTm,nx
ofHodge
tensors inTm,n(VQ,x)
forany x ~ X;
this willbe sufficient to prove the
lemma,
sinceGx
can be described asFix(l),
for oneelement 1 of one space
~HTmi,nix.
We have seen thatHTm,nx (for x~X)
is thesubspace
ofTm,n(VQ,x) composed
of tensors which lift toF0Tm,n(0393VC);
inparticular
thissubspace
islocally
constant. HenceHTm°"
is the rational stalk atx associated to a sub-variation of MHS
(Yz, W, F’*)
of(Tm,n(VZ), Tm,n(W.), Tm,n(F·)),
which isactually
pure oftype (0, )
and which inherits apolarization.
This
polarization 03C8
onV’R,x
is a scalarproduct,
invariant under03C01(X, x).
Thus03C01(X, x)
factorsthrough
the discrete group AutVZ,x
on one hand andthrough
the
compact orthogonal
groupO(V’R,x, 03C8)
on the otherhand;
hence theconnected group
Hx
actstrivially
onHTxm .
REMARK. A variation of MHS
Y is
said to besemi-simple
if for anyx E X,
the relevantcategory Vx>
issemi-simple (notations of §2).
It iseasily
seen that apolarizable
MHS issemi-simple
if andonly
if it is a finite direct sum of variationsof pure
HS up toisogeny. Indeed,
it is easy to see that both conditionsimply
thereductivity
ofGx
for any XEX.Conversely,
assume that for somex ~ X, Gx
isreductive. Then
by
localconstancy
ofGy on X,
the same is true forGy
for anyyEX.
Next consider a section 6 of the inclusion
(Wm)y ç; (Wm+ 1)y
in thecategory Vy>,
and let 03B3y,z be apath (up
tohomotopy) from y
to anearby point
z inX.
Then because of the
horizontality
of the filtration W and the localconstancy
of(GY)YEW,
the section03B3y,z(03C3)
deducedby transporting
6along
yy,z is a section of(Wm)z ~ (Wm+ 1)z
in thecategory Vz>.
ThusYI X
is a direct sum of variations of pure HS up toisogeny,
which extend to Xby continuity.
Thesemi-simplicity
ofV follows from this.
We shall now recall a
concept
introducedby
Steenbrink-Zucker[SZ] (cf.
also[HZ]).
Let us assume that X is a smooth connectedalgebraic variety
over C.The variation of mixed
Hodge
structure is consideredgood
if it satisfies thefollowing
condition atinfinity:
there exists acompactification X
ofX,
for whichX - X is a
divisor with normalcrossings,
such that(i)
TheHodge
filtration bundles FP extend overX
to sub-bundlesfP
of the canonical extensionVé
ofVe,
such thatthey
induce thecorresponding thing
forGrW(Yz, W, F.),
(ii)
for thelogarithm Ni
of theunipotent part
of a localmonodromy
transformation about a
component
ofXBX,
theweight
filtration ofNi
relativeto W exists.
The fact that these conditions are sufficient to
imply
those of[SZ] (3.13)
ispointed
out in[HZ] 1.5,
and follows from[K]
4 and[SZ]
A. Thefollowing
classes of variations of MHS are known to be
good:
(1) polarizable semi-simple
variations of MHS overalgebraic
bases[Sd], [CKS],
(2)
relativecohomology
modules of thecomplement
of a divisor withrelatively
normalcrossings
in aprojective
smoothX-scheme,
at least when X isa curve, see
[SZ]
5.7.Moreover,
thecategory of good
variations of MHS over X is stable under standard constructions of linearalgebra, EB, (8), duality,
see[SZ]
A.EXAMPLE. Smooth 1-motives. Recall from
[D2] III,
10.1.10 that a smooth 1- motive M over X is thefollowing
data:(i)
and extension0 ~ T ~ E ~ A ~ 0
of a(polarizable)
abelian schemeA
over X
by
a torus T overX,
(ii)
amorphism
u: H~E from a group scheme !!! over X toE;
one assumesthat
locally
for the étaletopology
onX,
H is constant and definedby
a free Z-module of finite
type.
The construction
V(M)=(TZ, W., F’):
Vz
=W0(VZ)
=Lie E/X E H defined by
theexponential
sequence,W-1
= Ker exp =R1fan*Z, W- 2
=(Xc(T)Y,
FO
=Ker(VcC ~
LieE/X),
which is fibrewise
compatible
with that of Section3, yields
apolarizable
variation of MHS over X.
LEMMA 5. Assume that X is a curve. Then the variation
V(M)
associated to the smooth 1-motive M isgood.
Proof (sketch of). According
to M.Raynaud [C.R.A.S.
262(1966) 413-416],
there exists a Néron model
É
of E over the smoothcompletion X of X,
such thatu extends to
note that the smooth group scheme
É/X
is not of finitetype
ingeneral.
Replacing H by
asubgroup-scheme
of finiteindex,
whichyields
anisogenous
variation
of MHS,
we may assume thatù (Y)
lies in theidentity component E0
ofÉ.
Condition(i) defining good
variations is fulfilled withIn order to
verify (ii),
we mayproceed by
induction since we know that bothW-1 (by point (2)
above: thegeometric situation)
andW0/W-2 (by duality
of 1-motives and
point (2)) satisfy (ii).
Granting (ii)
forW-1,
it follows from Theorem 2.20 of[SZ] (formula 2.21)
that(ii)
forWo
readsequivalently:
where(-2)M-l-1
is the relativeweight
filtration ofW-2,
which isW-1-1
sincethe
unipotent part
of the localmonodromy
ofW-2
is trivial(see [SZ] 2.14;
thepoint
is that T isnecessarily locally constant).
Therefore(*)
follows fromproperty (ii)
forW0/W-2.
D5.
Normality
We
keep
the notations of theprevious paragraph.
Thefollowing
result is asimple
consequence of the theorem of the fixedpart (Griffiths-Schmid- Steenbrink-Zucker).
THEOREM 1. Let
V = (VZ, W., F) be a (graded-) polarizable good
variationof
mixed
Hodge
structure over a smooth connectedalgebraic variety
X.Then for
anyx E
X, the
connectedmonodromy
groupHx
is a normalsubgroup of
the derivedMumford-Tate group !0Gx.
Proof.
We first prove thatHx a Gx, using
theimplication (ii)=>(i)
in Lemma 1.Since we
already
knowby
Lemma 4 thatHx
cGx
=G’,
it suffices to prove(ii)
for
Hx, Gx. Since 03C01(X, x)
acts on the free Z-moduleTm,n(VZ,x)/torsion,
any actionof
n1(X, x)
on a line insideTm,n(VQ,x)
must factorthrough 11 (the only possible eigenvalues).
Thus the connected groupHx
hasonly
trivial rationalcharacter.
Replacing
Xby
the finitecovering
definedby
the maximalsubgroup (of finite index)
ofni(X, x)
which factorsthrough
the connectedcomponent Hx
of themonodromy
group, we are reduced to prove that thelargest
constant sub-localsystem
offi
=Tm,n(VZ)
is a(constant)
sub-variation of MHS. For a finite directsum
of polarizable
variationof pure HS,
this isprecisely
the theorem of the fixedpart
ofGriffiths-Schmid,
see[CG], [Sd].
For ageneral polarizable good
variation of MHS in Steenbrink-Zucker’ sense, this is the theorem of the fixed
part
of theseauthors,
see[SZ]
4.19. Infact,
in loc.cit.,
this theorem is stated for aone-dimensional base
X,
but we can reduce to this caseby considering
curves inX,
see[Kz] §4.3.4.0,
for the detailedargument.
So far we have
proved
thatHx G,,;
to show thatHx a !0Gx,
we have toprove that the
algebraic subgroup H’x: = Hx/Hx
nDGx
ofGabx is
trivial. We firstnote that the
homothety
group inHx
is finite(by
the sameargument
as in thebeginning
of theproof).
It follows from this and Lemma 3 thatH’x|R
is acompact
torus.
Let V’ c
~Tmi,niVQ,x a
faithfulrepresentation
ofH’.
Asubgroup
of finiteindex
of 03C01(X, x)
acts on V’through GL( V’
n EBTmi,niVZ,x)
which isdiscrete,
andalso
through
acompact
torus. Because of the connectedness ofHx,
it follows thatV’ is a trivial
Hx-module,
and thenHx
is trivial. D As a consequence of thesegroup-theoretic arguments,
we recover:COROLLARY 1
(see [D2] 4.2.6-9).
The localsystem fa underlying
apola-
rizable variation
ofpure Hodge
structure issemi-simple;
eachisotypical
component carries a sub-variationof pure Hodge
structure; the centerof End(fo)
ispurely of type (0, 0).
For any x EX,
the connectedmonodromy
groupHx
issemi-simple.
Proof.
SinceHx a -9Gx
forx ~ X,
and since-9Gx
is asemi-simple
group(Lemma 2),
it follows thatHx
issemi-simple;
sinceHx
islocally
constant onX, Hx
is in fact
semi-simple
for any x ~ X. Thisimplies
thecomplete reducibility
of theaction of
n1(X, x)
onVQ,x
and the first assertion follows(the normality Hx Gx
would suffice
here). By (i)=>(iii)
in Lemma1, applied
toHx Gx
for x EX,
weget
on each stalk of each
isotypical component
of the localsystem faix
aHodge
sub-structure.
By continuity,
theseHodge
sub-structures extend acrossXBX
and
patch together
togive
rise to a sub-variation ofQ-Hodge
structure on theisotypical component
ofKu.
The third assertion follows from Lemma 1 in thesame manner.
COROLLARY 2
(see [D2] 4.2.9b).
The radicalof
the connectedmonodromy
group
Hx
associated to apolarizable
variationof
MHS isunipotent.
Proof.
LetPx
be thesubgroup
ofGL(VQ,x)
whichrespects
theweight
filtrationW,
andNx
thesubgroup
of P which actstrivially
onGrW(VQ,x).
ThenHx
cPx
and
Nx
isunipotent.
Moreover the connectedmonodromy
group, sayGrHx,
ofGrW(Vz)
at x is theimage
ofHx
inPxlNx.
HenceHx
is an extension ofGrHx,
which
(according
to theprevious corollary)
satisfiesGrHx = DGrHx, by
a(necessarily unipotent) subgroup
ofNx.
DREMARK.
Corollary
2 shows inparticular
that ifGx
is solvable for some x EX,
then the variation of MHS is
unipotent
in the sense of[HZ].
REMARK. Theorem 1
applies
to thegeometric
situations considered in Section 4 since in the course ofproving it,
we have made a restriction to curves.COUNTEREXAMPLE. We
produce
anexample, following
Steenbrink- Zucker(see [SZ] 3.16),
to show that some extrahypothesis
upon the variation of MHS is necessary.Consider a smooth 1-motive
M = [Zcn~xn Gm]
over X= Gmo
Here theset
X
isCxBCxtors.
Thecorresponding good
variation of MHSVis
an extension ofZ
by Z(1) inside C.
We denoteby
9 - 2 thegenerator
+ i ofZ(1)
~W-2
andby
eoany element
of VZBW-2;
then03B50,03B5-2>
spansVZ.
For some suitable deter- minationof log
x(depending
on the choiceof 80),
the sectionBo :
E -log x
E - ofVi
spansF°
and extends to a section ofVcC over pl.
We now combinenotations from Sections 3 and 4. For
XE X,
we haveU(Hx(M»)
=U(Gx(M)) =
U ~ Ga according
toProposition
1. On the other handHx(M) = U(Hx(M)) according
to theprevious corollary.
For any entire
function f,
let us now consider thefollowing perturbation Vf
of V:(VfZ; W.f)=(VZ; W.)
but(Ff)0
isspanned by 03B50+f03B5-2.
Thecorresponding
groups
Hx(Mf), Gx(Mf )
admit the samedescription.
Thefollowing
assertions areeasily
seen to beequivalent:
The group
Hx(Y’)
isisomorphic
toGa;
viewed as asubgroup
ofGl2
xGL2 acting
on(VQ,x Q VfQ,x),
its’typical’
element takes the formThe
’typical’
element ofGx(V’)
takes the forma
being independent
of c if(and only if) Vf
V. Therefore we see in thisexample
that
Hx(V’) -9G,,(V’)
if andonly
if V’ isgood.
6.
Maximality
Let
(Vz, W, F*)
apolarizable good
variation of mixedHodge
structures on X.Let
x ~
as in Lemma 3.By
thetheorem,
we know thatHx !0Gx.
We nowstudy
howbig Hx
can be in!0Gx.
PROPOSITION 2. Assume
that for
someYEX, Gy
isnilpotent (hence abelian,
according
to the remarkfollowing
Lemma3).
Thenfor
any x~ , Hx =!0G x.
Proof. According
to the remark which follows Lemma3, Gy
isactually
a torus.Since the assertion is invariant under
taking
finitecoverings
ofX,
it suffices to show that any tensor 1 ETm,nVQ,x
invariant under03C01(X, x)
spans aGx-module Wx
on which the action of
Gx
is abelian. It follows from the ’fixedpart’
theorem thatWx
is fixedby 03C01(X, x),
and the localconstancy
ofGx
onX, together
with anargument
ofcontinuity,
shows thatWx
extends to a constant sub-variation ofMHS,
say(V’, W’, F’’),
of(T’,» VU.
Inparticular
the action ofGx
onV’x = Yx
isthe same as the action of
Gy
onV’y,
which is abelian.For an
application
to smooth1-motives,
see Theorem 2 below.REMARK 1.
By
thenormality theorem,
theequality Hx = DGx (x ~ X)
holdswhenever
-9Gx
isQ-simple
and the variation of MHS does not become constantover any finite
covering
of X.By
way ofexample,
we consider a non-trivialpolarized family
of abelian varieties with manyendomorphisms
over acomplex algebraic
baseX; by this,
we mean that thegeneric
fibref~
off (that
makessense since
f
isautomatically algebraic) enjoys
thefollowing property:
(End f~) ~ZQ
is a divisionring
which contains a commutative field ofdegree dim £
over Q. Then the derived Mumford-Tate group of the stalk(R1f*Q)x
canbe
computed
for any Weilgeneric point
x of X(so
thatEnd £ =
Endfx) :
it turnsout that
DGx ~ ResZ+/QG,
whereZ+
denotes the maximaltotally
real subfield of the centerof (End f~) ~Z Q,
and G is anabsolutely simple
group overZ+ (in
factG|C ~ SL2) ;
thus in this case-9Gx
issimple
over Q(see
also theAppendix,
and[My]
Lemma2.3, [Al]
Th.2).(1)
REMARK 2. On the other
hand,
theequality Hx = DGx (x ~ )
may fail for trivial reasons,namely
when some Jordan-Hôlder constituentof(VZ, W, F’)
is alocally
constant variation ofMHS,
with non-abelian Mumford-Tate group.However this is not the
only
obstruction to themaximality
ofHx
ingeneral,
aswe shall now
show. (2)
SCHOLIE. There exists a non-isotrivial abelian scheme
A -
X over some curveX,
withsimple geometric generic fibre,
such thatHx =1= -9Gx
for anyXEX.
Proof.
We use M. Borovoi’s construction of asimple complex
abelianvariety
A of dimension 8 with Mumford-Tate group G =
ReszjQSL1(Dl
xD2),
whereDl
and
D2
arequaternion algebras
over some realquadratic
fieldZ,
with the sameinvariants at every finite
place
ofZ,
and oftype compact-non-compact (resp.
non-compact-compact)
at oo[B].
Infact,
suchpolarized
abelian varieties(with
(1)Other examples of Q-simple Mumford-Tate group are constructed in Mustafin’s paper cited in the final note.
(2)This contradicts the conjectural statement IX 3.1.6 in the author’s ’G functions and Geometry’
Vieweg 1989.