C OMPOSITIO M ATHEMATICA
D. B ARLET
A. N. V ARCHENKO
Around the intersection form of an isolated singularity of hypersurface
Compositio Mathematica, tome 67, n
o2 (1988), p. 149-163
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149
Around the intersection form of
anisolated singularity of hypersurface
D. BARLET* & A.N.
VARCHENKO~
Compositio
© Kluwer Academic Publishers, Dordrecht - Printed in the Netherlands
*Institut E. Cartan, Faculté des Sciences, Université Nancy I, BP 239, C.N.R.S. UA 750, F-54506 Vandoeuvre lès Nancy Cedex, France; IMath. Department, Moscow Gubkin Institute of Oil and Gas, Leninski Prospekt 65, 117917, GSP-1, Moscow, USSR Received 1 June 1987; accepted 3 February 1988
Introduction
Let P c- 0
[Xo,
...,Xn]
be aquasi-homogeneous polynomial
with anisolated
singularity.
For anypair
of monomials m, m’ theasymptotic expansion§
when s - 0 of the functionwhere o
EC~c(Cn+1) satisfies o -
1 near0,
has at most one term which isnot in
C[s, s].
Moreover this "non C~" term does notdepend
on the choiceof Q. So let
c(m, m’)
be the coefficient of this term which will beequal
now to
c(m, m’)susv
if u = v =1= 0 modulo Z or toc(m, m’)susv Log
ss if u, v E N
(u, v depend
onquasi-homogeneous weights
of m and m’relative to the
quasi-homogeneity type
ofP).
Now choose a monomial basis of the Q-vector space
and let 03BB be an
eigenvalue
of themonodromy
operatoracting
on thecohomology
of the Milnor fiber of P. The choice of 03BBcorresponds
to thechoice of monomials in our basis
having weights¶
a, a +1,
... , a + k§ The existence of an expansion (in a "general" context) is proved in [B.0]; here, use that P(dx/dP) is Coo on C"I’ to fit the general result.
1 Here the weight of the monomial m is by definition the quasi-homogeneous weight of m(dx/dP), assuming the weight of P is 1.
where
e-"1"" =
03BB: these monomials induce incohomology
a basis of theeigenspace
of themonodromy, corresponding
to theeigenvalue
03BB. Now let(mi)1~i~N
be the list of monomials in our basiscorresponding
to 03BBand 03BB
anddefine:
Although
the numbersc(mi, mi )
are ingeneral highly transcendental,
wehave:
THEOREM. For
any 03BB, 0394(03BB)
is a rational number.The idea of the
proof
is to consider two 0-lattices in thecohomology
ofthe Milnor fiber
of P (with complex coefficients).
The first one,L, is just
thelattice
given by
theintegral cohomology;
we shall call it theintegral lattice.
The second one,
L2,
is definedby
thecohomology
classes inducedby
monomial forms on
cn+I
1 or, moregenerally, by polynomial
forms withrational
coefficients;
we shall call it theholomorphic
lattice.Then we shall prove that some
nondegenerate
bilinear form defined overQ
(so having
rational values on theintegral
latticeL, )
has a rationaldeterminant on a basis
of L2 -
In fact we treatseparately
eachpair
ofconjuguate eigenvalues
of themonodromy operator.
For the
eigenvalues ~
1 the bilinear form issimply
the intersectionform,
and its relation to the "residue form"
given
in[V3]
achieves thecomputation
of the determinant. Then the relation between the intersection form and the canonical hermitian form
proved
in[B 1 ]
allows us to relate0394(03BB)
to thesquare of the "volume ratio" of the two lattices
LI
andL2.
For the
eigenvalue
1 wegive
theprecise relationship
between the residue form and the canonical hermitian form in order to use the samestrategy.
This is done
by
Loeser’s Theorem which asserts that the natural hermitian extension of the residue formof [V3]
is the canonical hermitian formof [B1]
for any isolated
singularity
of ahypersurface ([L],
Theorem2).
As an
application
of the theorem in theeigenvalue
1 case, we obtain thefollowing:
COROLLARY. Let Yt be a smooth
hypersurface
inIPn(C) defined
over Q. Denoteby Hn-1pr (H, C)
theprimitive
partof
thecohomology of
H in the middledimension;
denoteby LI
thetopological
0-latticeHpr 1 (e, C)
n Hn-I1 (e@ Q)
and
by L2
the 0-latticegenerated
inHpr
1(H, C) by
the residuesof
mero-morphic differential n forms
onPn(C)
with rationalcoefficients
and withpoles
in e.
Then for
any 0-basisBI
andB2 of LI
andL2, respectively,
we havewhere 1 =
dimc Hn-1pr(H, C).
Section 1 is devoted to the
relationship
between the residue form and the intersection form. The theorem and itscorollary
areproved
in§2.
This paper had been
partially
written when the second author wasvisiting Nancy University
in June 1986. He wants to thank the E. Cartan Institute forhospitality.
§1
We consider the germ of a
holomorphic
function with an isolatedsingularity
at the
origin ofcn+I
andlet f:
X ~ D be a Milnorrepresentative
of it. Thismeans that D is a disc in C and
that f
induces a COOlocally
trivial fibrationof X - f-1 (0) over D*
= D -{0}. We shall use a Scherk compactification
of this situation
[S] (see
also[V3]
for a detaileddescription).
So we have a
projective map f:
Y - D with an open relativeimbedding
X ~ Y over
D,
and Ygives
a smoothpolarized family
ofprojective
manifolds over
D*;
theonly
criticalpoint of lis
theorigin
in X.Fix a base
point so
E D* and letX(so )
andY(so )
denote thecorresponding
fibers of
f and f
Then the Scherkcompactification
has thefollowing properties:
1°)
There is an exact sequencewhere
pn(y(so))
is theprimitive part
of thecohomology* Hn(Y(s0))
withrespect
to thegiven polarization,
where Invpn(y(so))
is themonodromy
invariant
subspace
ofPn(Y(s0))
and where i* is the map inducedby
theinclusion i:
X(s0) ~ Y(so ).
2°)
For any class ain Hn(X(s0))=1
there exists aglobal (n
+1)-holomorphic
form ro on Y such that the
asymptotic expansion
of the section* When the coefficients are not precised, they are in C.
in an horizontal basis of the Gauss-Manin bundle s ~
pn(Y(S))=l
isgiven by
higher
termswhere k e N and
the à,
are horizontal(multivalued)
sections withi*(ã0|Y(s))
= a.Let us remark here for later use in
§2
thatif f is
apolynomial
defined overQ,
it ispossible
to choose a Scherkcompactification
defined over Q suchthat,
if so is fixed in D* nQ,
for any class a inHn(X(s0))=1
inducedby
monomial form
m(dx/df),
we can choose aglobal algebraic (n
+1)-
differential form ro on
Y,
defined overQ,
withproperty 2° )
as before.It will be
important
to notice that the Q-lattice inHn(X(s0))
definedby
classes induced
by
monomialforms,
is invariant underalgebraic change
ofcoordinates in
Cn+1
defined over Q.We now introduce the
monodromy operator
T(resp. T )
onHn(X(s0)) (resp. Pn(Y(s0))).
Denoteby Hn(X(s0))=1 (resp. Pn(Y(s0))=1)
thespectral subspace of Hn(X(s0)) (resp. pn(y(so))) corresponding
to theeigenvalue
1and define
and
Observe that Ker
N is exactly
thesubspace
InvPn(Y(s0)) of monodromy
invariant vectors in
Pn(Y(s0)).
So we also have the exact sequenceBut from the exact sequence
(1)
we alsohave, by monodromy
invarianceof i*
Comparison
with(2)
leads to a canonicalisomorphism
v:Hn(X(s0))=1 ~
Im
9 given by v(a) = Ñ(ã)
forany à
EPn(Y(s0))=1
suchi*(â) =
a.By
153
monodromy
invariance of the map i* we haveNow let
k be
the hermitian intersection form onPn(Y(s0))=1 normalized by
thefollowing
formulaLEMMA. For any a, b E
Hn(X(s0))=1
and anyã, b in Pn(Y(s0))=1
such thati*â = a _and
i*b = b,
we haveand this number
depends only
on a and b anddefines
anondegenerate
hermitianform
onHn(X(s0))=1.
We shall denote itby h.
Proof.
First note thatmonodromy
invariance ofk (i.e., k(Tu, tv) k(u, v) ~u, v
EPn(Y(s0))=1) gives k(Nu, v)
=k(u, Ñv)(infinitesimal invari-
ance).
To prove formula(5)
it suffices toput
u = à and v =b.
Let
h(a, b)
denote the number definedby
formula(5); h clearly
defines anhermitian form on
Hn(X(s0))=1
sincek
is hermitian. To establish the non-degeneracy
ofh,
it isenough
to usenondegeneracy
ofk
onpn(Y(SO))=I
which is well-known. So the lemma is
proved.
THEOREM
(Loeser [L]).
The restrictionof
the canonical hermitianform
hintroduced in
[B 1 to Hn(X(SO))=I is equal
toh.
For a direct
definition of
the canonicalhermitian form from asymptotics of integrals f=s~,
~ EC.°° (X) of
type(n, n)
werefer
to[B1].
REMARK l. Because
k
induces the usual intersection form on thesubspace Et)
=Image(Hnc(X(s0))=1 ~ Hn(X(s0))=1),
the theorem iscompatible
withthe relation
REMARK 2. The theorem shows that
k(Ñã, b)
does notdepend
on the choiceof the Scherk’
compactification:
the canonical hermitian form is definedlocally
around thesingular point.
REMARK 3. F. Loeser
pointed
out to us that his paper[L] (or
formula(5)) gives
adefinition,
in terms of themonodromy
andvariation,
of the canoni-cal hermitian form inside the Milnor fiber. This shows that it is a
topological
invariant of the
singularity (see
the final remark in[L]).
REMARK 4. On the rational
cohomology Hn(x(so)’ Q)
of the Milnorfiber,
there is a
nondegenerate
rational formgiven by
intersection foreigenvalues
of the
monodromy
which do notequal 1
andby k(Nâ, b)
for theeigenvalue
1. There are two ways to extend it to
Hn(X(s0), C):
take a C-bilinearextension or a hermitian extension. The first
gives
the residue form(see [V3], namely
formulas(9)
and(14)),
the second the form introduced in[B1].
Proof.
Let a and b be inHn(X(s0))=1. Using property 2°)
of the Scherkcompactification,
we can find m and co" which areglobal holomorphic (n
+l)-form
on Y such that the first terms in theexpansions
of03C9/df and 03C9’/df induce a
andb, respectively,
inHn(X(s0))*.
Let us consider the
asymptotic expansions
in an horizontal basis of the Gauss-Manin bundle associated to s -pn(y(s))
of the sections definedby
oi and ai’ of this bundle
(they
aregiven by
respectively).
The first terms of theseexpansions
aregiven by
where k, k’ ~ N, the âi and 6
are horizontal(multivalued)
sections of the Gauss-Manin bundle s ~Pn(Y(s))=1
and we have the relations(see [V1])
* See property 2° ) of Scherk compactification.
because the first terms must be invariant
by T (ro
and 03C9’ and uniform!).
Then, by
the definition of the canonical hermitian form in[B1],
the valueh(a, b)
is the coefficient ofsksk’ Log |s|2
in theexpansion
at s - 0 of thefunction
But the difference between F and the function
is Cx because of the
transversality
of the fibersof f to
ôX andbecause f has
no critical
point
in Y - X. Soh(a, b)
is also the coefficientof sksk’ Log 1 S 12
in the
expansion
at s = 0 of G. Nowusing (7)
and(8)
we obtainhigher
terms.But for
any s ~ 0,
we havebecause of the
horizontality
of the intersection form.Using
formula(5),
we seeimmediately
that the coefficientof sk sk’ Log |s|2
in the
expansion
of G at s - 0 isBut the choice of ru and 03C9’ is
exactly
such that we haveSo we have shown that h =
h on Hn(X(s0))=1,
and the theorem isproved.
* Since ax is transversal to all fibers of f, up to a Coo function of s, this is the same as
where Q E C~c(X), Q = 1 near 0.
156
COROLLARY. For a, b in
Hn(X(s0), Z)=1
we haveThe
corollary
is an obvious consequence of theproof
of the theorem.REMARK: It is not
possible
ingeneral
toreplace Q by
Z in the conclusion because thelogarithm
of aunipotent
is not defined over Z.But,
of course,one can use the fact that
Nk
= 0 forsome k n
to be moreprecise
aboutthe denominators of these rational numbers!
The fact that
(2in)n-I h
is real onHn(x(so)’ R)
wasalready proved by
F. Loeser
(see [L], corollary
1 of Theorem2).
§2
Consider a
quasi-homogeneous polynomial
P with isolatedsingularity
andassume that P is defined over Q
(i.e.,
P has rationalcoefficients).
Let be an
eigenvalue
of themonodromy acting
on thecohomology
ofthe Milnor fiber of P. Set k =
Q(03BB)
and K = C. Denoteby El
theeigen-
space of the
monodromy corresponding
to theeigenvalue  (E03BB
is definedover
k)
and letLet
L2
be the k lattice in V =LI ~k C generated by
all monomial differential formsm(dx/dP)
whoseweights correspond
to theeigenvalues
03BBand 03BB
of themonodromy (these weights satisfy e-2i03C0w = 03BB
ore-2i03C0w = 03BB).
First assume
that 03BB ~ 03BB
and choose a monomial basis ofLet et, oc +
1,
... , et+ k
be theweights
of the monomials in this basissatisfying e-2i03C0w
= Â and letfi, fi
+1, ... , fi
+ 1 thosesatisfying e-2i03C0w = 03BB.
Let
Hrx, H,+ 1,
... ,H,+k
andH03B2, H03B2+1,..., H03B2+l
denote thecorrespond- ing k-subspaces of L2 generated by
thecohomology
classes inducedby
thèsemonomials
(a
monomial m inducesm(dx/dP) by definition).
* Of course, since h coincides on Hn(X(s0))~1 with the intersection form, we have (2i03C0)nh(a, b) ~ Z for a, b ~ Hn(X(s0), Z)~1.
157 Then we have the
following orthogonality
relations for the k-bilinear intersection form onL2 (see [V3])
For monomials à and which induce classes a and b in
H03B1+i
andH03B2+j respectively
with(03B1
+i )
+(f3 + j )
= n we have from[V3]
formula(9)
where
Cn+1
is an universal(explicitly given)
constantdepending only
on n(see [V3],
p.35).
We shall
only
use the fact that(2i03C0)-nCn+1
~ Q.So the restriction of the intersection form to
L2
isgiven by
thefollowing picture,
where it is known that k = 1 and a+ 03B2
+ k = n and where wehave 0 in the upper left side and where the "skew
diagonal"
blocks are filledin with the
help
of formula(10).
Now,
for the monomials à andb,
the numbersResp,0 (â dx, b dx)
arerational: for instance the residue can be defined as the value at 0 of the trace
of the
form âb
dx via the finite map, defined overQ, given by aP/aXo , ... , êplaxn -
So the entries of the "skew
diagonal"
blocks are inCn+1 · Q;
that is to say in(2in)n.
Q. The determinant of the C-bilinear extension of the intersection form in this basisB2
ofL2
is in(2in)nl _
Q where d =dim(E.
+E03BB).
Now let
B,
be a real k =Q(03BB)
basis ofLI
and denoteby
C the matrix ofthe intersection form in
BI.
Then1 ° )
C has coefficients inQ(03BB)
m R and the matrix D* CD of the C-bilinear intersection form in the basisB2 (here
D =G1d(C)
isunknown)
satisfies2°)
det(D* CD)
E(2in)nd.
Q.If we look now at the matrices of the hermitian intersection form
(normalised by l/(2i7r)" oc u 03B2)
in thebases B1 and B2 they
areand
Fig.
Because the determinant of an hermitian form is real and C has real coefficients we
get (2in)nl
ER;
that is to say nd is even(this
is trivial in ourcase 03BB ~ 03BB
because d = 2dim E.
iseven).
So we deduce from
2° )
that(det D)2
E R andso det DI2
= ±(det D)2.
So we
get 0394(03BB) = det DI2
det(1/(2i03C0)n C)
E Qby 2°).
This proves the result in this case.
For 03BB = -1 the fact that det
(1 /(2i7,)n C)
is real shows that nd is even andwe can argue
along
the same lines.The case 03BB = 1 is
slightly
different.First of all C is no
longer
real because of thecorollary
of Loeser’s Theorem in§1.
But of course det(1/(2i03C0)n C)
is stillreal,
and so, if we know thatD*[1/(2i03C0)n]
CD has a determinant in Q we canagain
conclude that(det D)2
e R andso det DI2
= ±(det D)2
and soA(l)
e Q.So for the case 03BB = 1 we can
again
choose adecomposition L2 = (D 0’ H,, + "
icorresponding
tointegral weights
in ourbasis,
but we have tochange
thepolynomial
P* to have a nice Scherkcompactification (as
in§1)
in order touse results of
[V3]
in the case of adegenerate
intersection form(§3).
Ofcourse this can be dône
algebraically
over Q** and so we can concludeagain
that the determinant of the C-bilinear intersection form in our basis
B2 belongs
to(2i03C0)nd ·
Q where d =dimo El.
Now we can finish the
proof
in this case as beforeif,
instead of[Bl]
Theorem
3,
we use the Theoremof §1
and[V3], §3.
This
completes
theproof
of the Theorem.REMARK 1. Let
f
be anypolynomial having
an isolatedsingularity
at0 E Cn+1 and defined over Q. For fixed define the
integral lattice L1 = Ea + E03BB
and letL2
be the lattice definedby
thecohomology
classes inducedby spectral projections
onLI Ok C
ofpolynomial (n
+1)-forms
withrational coefficients. Then it is
possible
to proveagain
that vol(B2/B1)2 ~ Q(À)
for anyQ(03BB)
basis ofLI
andL2.
Justreplace
thepicture
we have usedto
compute
the determinant in our monomial basis ofL2, by
thepicture given
in[V3], §4,
no. 6. But of course, it is morecomplicated
to define0394(03BB) (the
determinant of the canonical hermitian form in a basis ofL2 )
in sucha case, because its
expression
in terms ofasymptotics
ofintegrals
on thefibers
of f is
much more involved.REMARK 2. Let P E 0
[Xo,
...,Xn, 03BE1,
... ,03BEp]
afamily
ofquasi-
homogeneous polynomial (parametrized by 03BE) with
an isolatedsingularity
atthe
origin.
Assume that the Milnor number03BC(03BE)
is constantfor 03BE
near 0(in Cp).
Thenworking
over the fieldQ(03BE)
leads to ananalogous
theorem. Infact,
theonly point where 03BE
appears(because
monomials are defined over0)
is in the residue.
Computing
trace via the mapleads to coefficients in
C(03BE).
Then the use ofconjugation
leads to0394(03BB)2
eQ(03BE, Z).
* By an algebraic change of coordinates defined over Q.
** As noticed before, this preserves the L2 lattice.
160
EXAMPLE
(see [B3]).
LetP03BE(X, Y, Z) = X3 + y3
+Z3
+303BEXYZ
andlook at À = 1.
Then L2
isgenerated by
monomials 1 and XYZ. The remark above saysconcretely
thefollowing:
Let Q) = Xd Y 039B dZ + YdZ 039B dX + ZdX A dY and
for e
EC~c(C3)
such
that Q =-
1 near 0 we have thefollowing asymptotics
when s - 0Then the square of
is in
Q(03BE, Z) (the
rationals functionon 03BE and Z
with coefficients inQ).
The function c,,,
(ç)
isgiven
in[B3]:
where
A(03BE)
is the area of the fundamentalparallelogram
of theelliptic
curveX3 + Y3
+Z3
+303BEXYZ
= 0 inP2 (C).
The coefficientsCI,2(Ç),
C2,1(ç)
andC2,2(03BE)
can be deduced from c,,,(ç) by
thefollowing
remark:We have
d03C9/d03BE = 2013
3XYZro on thefamily P, =
s(s fixed).
Thisgives
and and so
As one can
clearly
see in theprevious example
the matrix of the canonical hermitian form in a basis of theholomorphic
latticeL2
is not "skewtriangular"
and hashighly
transcendantal entries. This comes from theconjuguation
map which does not preserve theL2
lattice.Proof of
thecorollary.
Denoteby (Xo,
...,Xn, t) homogeneous
coordi-nates on
Pn+1(C)
andidentify Pn(C)
with thehyperplane {t
=0}
inPn+1.
Let P e Q[Xo, ..., Xn]
be an irreduciblehomogeneous polynomial of degree ô
such that{P
=01
nPn =
Je. ThenC(Jf’) = {P
=01
is thecone over XI in
Pn+1,
We shall consider the smooth
hypersurface V
ofPn+1 defined by P(X) = t03B4.
Then for m ~ C
[Xo,
... ,Xn]
a monomial ofdegree
kô -(n
+1) (k
eN*),
themeromorphic
differential form(defined
overQ)
onPn+l
1with
poles
in{P
=0},
satisfiesThen we have the commutative
diagram
of restrictions and residues(see Leray [2])
since
As is known
(see [G],
Theorem8.3),
theimage
of the residue mapResPnH
is the
primitive part Hpnr 1(H, C),
so the latticeL2
isgenerated (as
a Q vector162
space) by
elements of thefollowing type
for m e Q
[Xo,
... ,X,, monomial
ofdegree
k03B4 2013(n
+1).
Now it is clear that the map 2in
ResvH (which
is defined over Q as theadjoint
of the tube mapHn-1(H, Q) ~ Hn+1(V - 9V, Q))
sends the twolattices of the
monodromy
invariantpart
of thecohomology
of the Milnor fiber V - e of the affinehypersurface {P
=01
inCn+1,
to the latticesL,
and
2i03C0L2
of the groupH;r-I (:Yf, C). So,
as aby product
of theproof
of thetheorem,
we obtainwhere 1 =
dimCHn-1pr(H, C),
for any Q-basisBI and B2
ofL, and L2
respectively.
REMARK. This
implies
of course, that the determinant in any basisB2
of
L2
of the hermitian intersection form onHn-1pr(H, C)
normalizedby
1/(2i03C0)n-1 Hu
tB D is rational.EXAMPLE. For an
elliptic
curve inP2(C)
defined over Q(Y2 Z
= 4X3 -g2XZ2 - g3Z3
with g2, g3 EQ)
we have n =2,
1 = 2 andL2
isgenerated
by (Z/Y)d(X/Z) and(X/Y)d(X/Z).
The matrix of this basis in the
toplogical
basiscoming
from the standardparametrisation
where cv, , ro2 are the
periods
and ~1, 112 thecoperiods;
the classicalLegendre equation
iswhich is
compatible
with the statement of thecorollary; namely ((~203C91 -
111
ro2))2
E(2in)2
Q.References
[B.0] D. Barlet: Développements asymptotiques des fonctions obtenues par intégration dans
les fibres. Inv. Math. 68 (1982) 129-174.
[B.1] D. Barlet: La forme hermitienne canonique sur la cohomologie de la fibre de Milnor d’une hypersurface à singularité isolée. Inv. Math. 81 (1985) 115-153.
[B.2] D. Barlet: le Calcul de la forme hermitienne canonique pour Xa + Yb + Zc. In Lecture Note n° 1198, pp. 35-46, Séminaire Dolbeault/Lelong/Skoda (1983/1984).
[B.3] D. Barlet: Le calcul de la forme hermitienne canonique pour un polynôme homogène
à singularité isolée. Journal de Crelles 362, (1985) 179-196.
[G] P. Griffiths: On the periods of certain rational integrals I. Ann. Math. 90 (1969) 460-495.
[L] J. Leray: Le calcul différentiel et intégral sur une variété analytique complexe (problème
de Cauchy III). Bull. Soc. Math. France 87 (1959).
[L] F. Loeser: A propos de la forme hermitienne canonique d’une singularité isolée d’hyper-
surface. Bull. Soc. Math. France 114 (1986) 385-392.
[S] J. Scherk: On the monodromy theorem for isolated hypersurface singularities. Inv.
Math. 58 (1980).
[V.1] A.N. Varchenko: Gauss-Manin connection of isolated singular point and Bernstein
polynomial. Bull. Sci. math. (2) 104, (1980) 205-223.
[V.2] A.N. Varchenko: The complex singularity index does not change along the stratum
03BC = const. Funk. Anal. i Prilozken 16(a) (1982) 1-12.
[V.3] A.N. Varchenko: On the local residue and the intersection form on the vanishing coho- mology. Math. USSR Izvestiya, 26(1) (1986) 31-52, translated from ~~~ Akaq Hayk
CCCP Cep. Matem. Tom. 45, n° 1 (1985).