A NNALI DELLA
S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze
Z IV R AN
Semiregularity, obstructions and deformations of Hodge classes
Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 4
esérie, tome 28, n
o4 (1999), p. 809-820
<http://www.numdam.org/item?id=ASNSP_1999_4_28_4_809_0>
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Semiregularity, Obstructions
andDeformations of Hodge Classes
ZIV RAN
Abstract. We show that the deformation theory of a pair (X, tl), where X is a compact Kahler manifold and 17 is a (p, p) class on X, is controlled by a certain
sheaf
.c1]
of differential graded Lie algebra on X; consequently, we show thatrelative obstructions to deforming a pair (X, Y), where Y is a codimension-p
submanifold of X, relative to deforming X so that the fundamental class of Y remains of type (p, p), (in particular, deformations of Y fixing X) lie in the kernel of the semiregularity map 7rl : of Bloch et al. We also give a number of extensions and applications of this result.
Mathematics Subject Classification (1991): 14D15 (primary), 14D07, 14C30 (secondary).
To a
codimension-p embedding
Y c X of compactcomplex
manifoldsone may associate at least 3 deformation
problems: deforming
Y,fixing
X(the
local Hilbertscheme); deforming
thepair (Y, X) ; deforming
X so that thecohomology class q
-[Y]
EH2p (X )
maintains agiven Hodge
p.These
problems- obviously
interrelated- are all influencedby Hodge theory,
viathe so-called
semiregularity
map(which
has antecedents in Severi and was morerecently
consideredby Kodaira-Spencer, Mumford, Bloch ... )
normal bundle.
Roughly speaking
obstructions which apriori
lie in areactually
inker(7r,). Thus,
e.g. a lower bound on the rank of 7r,yields
estimates on thedimension of deformation spaces etc. The
precise
statement is as follows.THEOREM 0. Let X be a compact
complex manifold
and Y C X a connectedsubmanifold of
codimension p, with normal bundle N,and fundamental
class 1] =[Y]
E Let 7r, : : be thesemi-regularity
map(reviewed below).
ThenPervenuto alla Redazione il 2 luglio 1998 e in forma definitiva il 24 settembre 1999.
(i)
obstructions todeforming
Y in X lie in ker 7ri;(ii) if
moreover X is Kählerian then obstructions todeforming
thepair (X, Y),
relative to
deforming
X so that q EH2p (X )
remainsof
type(p, p),
lie inker J 1.
[In
moredetail, (ii)
means:given
an artin localC-algebra (S, m),
an idealI S with mI =
0,
a deformation a of(X, Y)
overS/I,
a deformation a’ of X over S, which induces the same deformation as cx overS/I
and in whichthe
(Gauss-Manin)
flat liftof 17
hasHodge
level p, obstructions tolifting
aover ’ S lie in
ker(03C01)
0I.]
Theorem 0 was in essence proven
by
Bloch[B]
for the case of deformationsover an artin
ring
of the form however neither the result nor theproof yield
thegeneral
artin local case. In thepresent generality
Theorem 0 wasfirst stated in
[RO]
where theargument
was based on the notion of "canonical element"controlling
a deformation(see [R3]
for adevelopment
of thetheory
and
required properties
of canonicalelements).
The main purpose of this paper is to
develop
some methodspertaining
tothe
interplay
of "canonical" or "Lie-theoretic" deformationtheory
andHodge theory
andapply
them to aproof
of Theorem0;
theproof
of part(i)
inparticular
is short and
essentially
self-contained. A central role in these methods isplayed by
a certain differentialgraded
Liealgebra
,C =£q which,
as we prove with themethod of
[R3],
controls deformations of X in which agiven class q
maintainsa
given Hodge
level. Modulo this fact(which
moreover is unnecessary for part(i)),
theproof
of Theorem 0 isquite simple
andconceptual:
indeed itboils down to
constructing
a Liehomomorphism : N [-1 ] ---->Ln ("sheaf-
theoreticsemiregularity")
andrealizing
.7r, as thecohomology
map inducedby
jr.Following
theproof
we present someapplications
to deformations of maps andintegral
curves on K3 surfaces. See[RO]
for otherapplications.
As our foundational reference for
(Lie algebra-controlled)
deformation the- ory, we shall use[R2], [R3];
however for theproof
of part(i) (which
isalready
sufficient for most
applications), essentially
anyreference,
e.g.[GM],
will do.PROOF OF THEOREM. Let T =
Tx
and T’ C T be the subsheaf of vectorfields tangent to Y
along
Y, i.e.preserving
the ideal sheafI y.
Weidentify
thenormal sheaf N with the
complex
indegrees -1, 0
and endow
N [ -1 )
with a structure of DGLA sheafgiven by
(the
1/2 factor is needed to make i d a Liederivation).
We thus have an exacttriangle
of DGLA’s -(i.e. N[-1]
is a Lie ideal inT’),
and thesecontrol, respectively,
the deformations of Yfixing
X, of thepair (X, Y),
of X(see
e.g.[R2], [R3]
for more detailson
this).
On the other
hand,
to anyclass 11
E Hq(QP)
we may associate a DGLA ,C =12r¡
as follows:differential = interior
multiplication by
17, bracket = usual one on T, Lie deriva- tive T xQP-1 --* S2p-1,
zero otherwise.More
concretely,
we may represent£° (resp. ,C-q ) by
the Cechcomplex
of T
(resp.
ofQP-1 shifted q places
to theleft).
Thus we have an exacttriangle
of DGLA’s 1with an abelian ideal in ,C.
By
the localcohomology description of q
=[~’] given,
e.g. in[B]
it followsdirectly
that interiormultiplication by q
vanishes(in
the derivedcategory)
onT’ c T, and
consequently
we have a commutativediagram
of exacttriangles
7r, = be taken as the definition of 7Tl but it is immediate that this definition coincides with the one
given
in in[B].
It may be noted that isnone other than the infinitesimal Abel-Jacobi map associated to Y. Now we shall prove below
that,
for XKahlerian,
,~ controlsprecisely
the deformations of Xwhere q
remains of type(p, p).
Giventhis,
the Theorem followsimmediately
from
( 1 ):
indeedby
anygeneral theory (e.g. [GM], [R2]),
obstructions areinduced
by
Lie bracket and lie inH2
of thecontrolling
Liealgebra
and thusrelative obstructions as in the Theorem lie in
kerH2(7T’) =ker(7r,).
0Note that for the purpose of part
(i)
theinterpretation
of .C isirrelevant,
so this part does not
require
the Kahlerianhypothesis (nor
for that matter any of the rest of thepaper).
It remains to establish the deformation-theoretic
significance
of ,C.Precisely,
we will show the ,C controls deformations
X/S plus Cech
cochainswhere ~
= constant liftof q,
modulo coboundaries (o= 8(T).
To this end we first review the universal variation of
Hodge
structureassociated to X, as
developed
in[R3],
which willprovide
us with anexplicit
representative
for the GM-constant lift of acohomology
class on X. Considerthe
following
doublecomplex Jm (T, Q)
on X m > x X inbidegrees [0,n]
x[-m, 0]:
with horizontal arrows induced
by
exterior derivative and vertical arrows of the form(i.e. Jm (T, Q)
isjust
the standardcomplex
for Q8 asT -module,
with variablesseparated.)
Asexplained
in[R3],
the De Rhamcohomology
ofthe universal m -th order deformation
Xml Rm
of X,together
with itsHodge
filtration
(i.e.
the universal m-th order VHS associated toX)
is obtainedby applying
a pure linearalgebra
construction to a suitable Kunneth component of thecohomology
ofJm(T, Q), (i. e.
the onemapping
toC)
Q9Hr(X)
under thequasi-isomorphism
C ~S2’),
so onemight
as well work with the latter groupdirectly.
Thanks to Cartan’s formulafor Lie
derivative,
thecomplex Jm (T, Q8)
is"split",
i.e.isomorphic
to thecomplex
with the same entries and trivial action of T onQ8,
theisomorphism
in
question being
assembled from ± interiormultiplication
mapsThe induced map on
cohomology
is the Gauss-Maninisomorphism
The "constant lift" of a
class 17
E issimply
the mapgiven by G(.
01]).
Moreexplicitly
onCech cohomology,
may be described as follows. We may represent an element
(~i,... ,
whereb
being
the map inducedby
bracket. On the other hand Xbeing
Kahlerq E
Hp~q (X ),
say, may berepresented by
aCech cocycle
with values in the sheafS2p
of closedp-forms (which
in effect meanschoosing
a liftof 17
toand may be
represented by
We are now in
position
to consider the obstruction to the constant lift(v) having Hodge
level p(in cohomology).
Thus consider whathypercoboundary
would
push
intoFPQ8),
i.e. kill all terms off thep-th
column.Working
from the bottom up,starting
inposition (p - 1,
-m +1)
werequire
first a cochain
Clearly
the latterright-hand
side is acocycle,
so the obstruction to 1existing
is in 0 Note that onceexists,
wehave
so all other terms
along
the bottomdiagonal,
i.e. inposition ( p - k -
1, -m +k + 1), k = 0, ... , m - 1,
can be killed too. Next, to kill off the term inposition (p -
1, -m +2) requires
a cochainwhere d and L denote the horizontal and vertical differentials in the
complex Jm ( T ,
S2’ ) .Again
it is easy to see the latterright-hand
side is acocycle.
So the obstruction to cvm-2
existing (provided does)
is inS,-2 H’(T)
0Hq+l
andagain
once úJm-2 exists all elements in thediagonal {(a, b),
a+b = p - m -f- 1, a p ~
may be killed too. We continue in this way up to the 0-th row where what isrequired
isTurning
to thealgebra
,C and its deformationtheory,
we claim that the obstructions are the same as forkeeping
of level p, which it sufficesto show in the universal situation. For the first-order case this is clear:
given
v E
H 1 (T),
the datarequired
to lift v to isprecisely
a cochain WI Eeq(op-1)
=i (v) (r~),
same obstruction as for to be of level p. Next we turn to the second-order case. Thecomplex ~2(~)
takes the formGiven v E the
assumption Gq(u)
is of level p to first ordermeans that
writing
we have some with
To lift this data to
requires precisely
In other
words,
the obstruction is[L(úJl)
+i (Vl)(1J)]
E Onthe other hand as we saw above
(5)
the obstruction tobeing
of level p isNow X
being Kahler,
we have= 0,
so the two obstructions coincide.In the
general
m-th order case, the situation is similar:given
v EH°(Jm (T)) plus
data c~m _ 1, ... , womaking
of level p, the datarequired
to lift v toconsists of cochains
6~_~
... ,wb
withso
again
the obstructions are the same. 0We conclude with a brief
partial
treatment ofsemiregularity
for maps, insofar as results follow from the above. Letbe a
generically
finite map of compact Kahler manifolds of dimensions n - p,n, and let
f
c Y x X be thegraph
off. Assuming,
say, thatit is well known that deformations of Y x X are of the form Y’ x X’ with
Y’, X’
deformations of Y, X,
respectively,
and it followseasily
that deformations of thetriple ( f,
Y,X) correspond bijectively
with deformations of thepair (Y
x X,Y),
hence the above results
apply.
Note thatwhile is "the same" as the
pullback
mapor its
dual,
theGysin
mapand being
of type(n, n)
meansn~*
preservesHodge
levelor n*
raisesHodge
level
by
p, so we conclude thatCOROLLARY 2.
Assuming (6),
obstructions todeforming f,
relative todeforming
X, Y so that
ry*
raisesHodge
levelby
at ynost p, lie inConsider next the case of deformations of
f
with X fixed. As is well known[AC],
these are controlledby
the normal sheaf which fits in an exactdiagram (identifying
= 0Again N f [-1 ]
forms a DGLA sheaf on Y and obstructions todeforming (Y, f )
are in and come from the bracket mapN f
xN f ~ Nj. [ I ].
On the other
hand,
xX)
has as one Kunneth componentand
by
its definition thesemiregularity
map for Y factorswhere is induced
by
interiormultiplication by
the component of[Y]
inHn-p,n-p(Y)0HP,P(X)
so we conclude(note
this does not useassumption (6)):
COROLLARY 3. Obstructions to
deforming ( f, Y), fixing
X, relative todeforming
Y so that
ry*
raisesHodge
levelby
p, lie inker,71,f.
Note that there are many cases, e.g. Y is a curve and
(Ox)
=0,
wherethe
cohomological
conditionon 17
is vacuous, for thenry*
issimply given by
In
particular,
suppose Y is a smooth connected curve of genus g and X isa K 3 surface. Then from
(7)
we get a nonzero mapand the
semiregularity
map factorsthrough
-~ Serre dual to=
H°(Oy),
which map isclearly
nonzero, hence so is Jr 1, f because - issurjective,
Ybeing
a curve. On the otherhand
Ky,
soX (Nf )
= g - 1. We conclude then that the deformation space of( f, Y)
is at leastg-dimensional.
Now suppose in addition that
f
is ofdegree
1 toits image
Y. It is then clear that unobstructed deformations of( f, Y)
must move Y, hence mustproject injectively
to and since is a subsheaf ofKY
withquotient
=tor
(supported exactly
on the ramification locus off),
itsho
is g unless g = 0 or tor=0;
and if tor=0,
i.e.f
isunramified,
thenNf -- KY
so isinjective
and( f, Y)
is unobstructed. Soputting things together
we concludeCOROLLARY 4. On a K 3
surface,
the locusof integral
curvesof geometric
genus g > 0 isgenerically
reduced,purely g-dimensional (or empty),
and smooth at any immersed curve.Appendix:
Thesemiregularity homomorphism
In the course of the
proof
of Part(i)
of theTheorem,
weimplicitly
alludedto the fact that the
semiregularity
map 7r is a Liehomomorphism,
whichimplies
that so is 7r’. As this may not be
generally known,
we include aproof
forcompleteness.
First we recall the local fundamental class and
semi-regularity
map. Takean
acyclic
cover U =( U« )
of an open subset U C X and let Y nUa
be definedby Fa = ( fa , ... , fa ) _ (o),
and setThis
yields
acocycle
inS2p) (S2p
= for the open cover(D¡,a = Ua - ( fa - 0)),
whence a classand these
glue together
toyield
which maps to the fundamental class
(More pedantically,
one computesHp-1 (U -
Y,QP)
from theCech
bicom-plex ( C ~ ~ , 81, 62)
associated to the biindexed cover of U - Y.Writing
onfor a suitable matrix A
expressed
as aproduct
ofelemetary matrices,
it is easy to see thatis a sum of terms with p distinct
fj
in thedenominator,
soby elementary properties
of localcohomology
there is anexplicit ( p - 2, 1)-cochain
withand is a
bicocycle representing
a class inHP- 1 (U - Y, S2p )
whoseimage
isryu.)
Now
by
a similar remark aboutdenominators,
note thatrya
is killedby
any functionvanishing
on Y nUa; likewise,
if Va Er(Ua, T’),
the interiorproduct
has
vanishing cohomology
classUsing
the Cechbicomplex
abovethese statements may be extended to U and hence
globalised:
thus the arrowsgiven by (interior) multiplication by q
vanish in the derived category; in
particular
interiormultiplication by 17
descendsto a map
(’sheaf-theoretic semi-regularity’)
which induced the
(cohomological) semi-regularity
as well as the infinitesimal Abel-Jacobi map
Now we come to the crux of the
(semi-regularity)
matter:LEMMA 1. The
composite
vanishes in the derived category; in other
words,
7r is a Liehomomorphism
in thederived category.
PROOF. First a calculus obervation: if w is a closed
p-form
and x, y vectorfields on a manifold then
(check!)
Now take sections , 1 So
note that the
cohomology
classescorresponding
tovanish,
hencev"])
isrepresented
Now consider the
diagram
where the top left arrow is
given by a
x 7r ED 7r x9, 9:~V-~ T[1] ]
the naturalmap. We have
just
proven that the left square commutes while theright
one doesobviously. Clearly
the top arrows compose to zero because N --~7~[1] ] ~ T[l] ]
do. Hence the
composite
N x N ~N [ 1 ] -~ ~’~[p+ 1] ] vanishes,
as claimed.REFERENCES
[AC] E. ARBARELLO 2014 M. CORNALBA, A few remarks about the variety of irreducible plane
curves of given degree and genus, Ann. Sci. Ec. Norm. Super. Ser. IV, 16 (1983), 467-488.
[B] S. BLOCH, Semiregularity and De Rham cohomology, Invent. Math. 17 (1972), 51-66.
[D] P. DELIGNE, Letter to H. Esnault (1992).
[GM] W. GOLDMAN 2014 J. MILLSON, The deformation theory of representations of the fundamental
group of compact Kähler manifolds, Publ. Math. IHES 67 (1988), 43-96.
[RO] Z. RAN, Hodge theory and the Hilbert scheme, J. Differential Geom. 37 (1993), 191-198.
[R1] Z. RAN, Derivatives of Moduli, Internat. Math. Res. Notices (1993), 93-106.
[R2] Z. RAN, Canonical infinitesimal deformations, J. Algebraic Geom. in press 1999.
[R3] Z. RAN, Universal variation of Hodge structure and Calabi-Yau Schottky relations, Invent.
Math. 138 (1999), 425-449.
Mathematics Department University of California
Riverside CA 92521 USA ziv@math.ucr.edu