C OMPOSITIO M ATHEMATICA
W. V EYS
Congruences for numerical data of an embedded resolution
Compositio Mathematica, tome 80, n
o2 (1991), p. 151-169
<http://www.numdam.org/item?id=CM_1991__80_2_151_0>
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Congruences for numerical data of
anembedded resolution
W. VEYS
K. U. Leuven, Departement Wiskunde, Celestijnenlaan 200-B, B-3001 Leuven, Belgium
Received 11 November 1990; accepted 21 January 1991
©
Introduction
Let k be an
algebraically
closed field of characteristic zero andf
Ek[xl, ... ,
Xn+1].
Let(X, h)
be an embedded resolution off
= 0 in An+1,
constructed
by
means ofblowing-ups according
to Hironaka’s Main Theorem II[Hi, p. 142].
We denoteby Ei, i E I,
the irreducible components ofh-1(f-1{0}),
and associate to eachEi
apair
of numerical data(Ni, vi),
whereNi
and
vi-1
are themultiplicities
ofEi
in the divisor ofrespectively f 0 h
andh*(dx1
A ... Adxn+1)
on X.In dimension one
(n =1)
someinteresting
relations are known between these data. Fix oneexceptional
curve E with numerical data(N, v),
say E intersects k times another irreducible component and denote these componentsby E1,..., Ek.
Then we haveMoreover we can describe the
quotients (S 1 N;)/N
and(S 1 (vi - 1)
+2)/v
inthe two cases as 1 + p, where p is the number of times that a
point
of E occurs ascenter of some
blowing-up during
the resolution process.When
f(x1,x2)
isabsolutely analytically irreducible, only k =1,
2 or 3occurs. The cases k=1 and k=2 were obtained
by
Strauss[S, Th.1]
andMeuser
[M, Lemma 1],
and the case k=3by Igusa [1, Lemma 2].
Loeser[L,
LemmeIL2] proved
thegeneral
result.If for i =
1,..., k
we set ai = Vi- v Ni,
then we can derive from(*)
theN relation
In
[V]
we haveproved
relations between numerical data forarbitrary
polynomials
in alldimensions, extending
the relation(**).
Now in this paper we will provedivisibility properties
between numerical dataof exceptional varieties, extending
the congruences(*), again
forarbitrary polynomials
in alldimensions,
and describe the
quotients.
Statement
of
the resultWe prove in Theorems
3.3,
4.3 and 4.6essentially
thefollowing.
Fix oneexceptional variety
E with numerical data(N, v).
There are basic congruences(B1
and
B2)
associated to the creation of E in the resolution process,generalizing (*).
And there are additional congruences
(A)
associated to eachblowing-up
of theresolution that
’changes’
E. Moreprecisely (using
the same notations asabove):
The
variety
E in the final resolution X is in fact obtainedby
a finite succession ofblowing-ups
with irreducible
nonsingular
centerCi
c E’ andexceptional variety 03B5i+1
~ Ei+1for
i = 0,..., m -
1. Thevariety
E° is created at some stage of theglobal
resolution process as the
exceptional variety
of ablowing-up
with center D andis
isomorphic
to aprojective
space bundle Il: E0 ~ D over D.For i =
1, ... , m
and for anyvariety V
cEj, 0 j
i, let therepeated
stricttransform of V in E’
(by
ni - 1 0 ... 003C0j)
be denotedby
V(i).There are two kinds of intersections of E with other components of
h-1(f-1{0}).
We have therepeated
strict transforms03B5(m)1,..., 03B5(m)m
in E of theexceptional varieties 03B51,..., 03B5m;
and furthermore we have therepeated
stricttransforms
03B5(m)i
in E of certain varieties03B5i,
i E T,(of
codimensionone)
in E°.For each
i~T~{1,..., m}
thevariety 03B5(m)i
is(an
irreducible componentof)
the intersection of E with
exactly
one other componentof h-1(f-1{0}).
Let thiscomponent have numerical data
(Ni, vi).
Then we havewhere
di,
iE T,
is thedegree
of the intersectioncycle 03B5j ·
F on F for ageneral
fibreF zé Pn-dim D of II : E0 ~ D over a
point
of D; andin Pic
D/N
Pic D, where k = n + 1 - dim D,03B5ki
is the k th self-intersection ofCi
inE°,
and03B5i=03A0*Bi
whendi=0.
where Ilk, k E
T~{1,..., il
is themultiplicity
of thegeneric point
ofCi
on03B5(i)k.
We have moreover
analogous
congruences for thev-data,
and we can describein each case the
corresponding quotient.
At the end of the paper we
give
someapplications
of these congruencesconcerning
thepoles
of thetopological
zeta function.Terminology
All schemes will be
quasi-projective,
avariety
is an irreducible and reducedscheme,
and subschemes(in particular points)
are assumed to be closed except when stated otherwise. The reduced scheme associated to a scheme X is denotedby Xred.
We make no distinction between a divisor and its divisor
class;
which of both is meant should be clear from the context.Let V be a subscheme of
everywhere
codimension one of anonsingular
scheme X. For all x~X we define the
multiplicity 03BCx(V)
of x on V as themaximal
integer
m, such that the mth power of the maximal ideal of the localring (9xx
of x on X contains the ideal of V in(9xx.
1. Embedded resolution
Let k be an
algebraically
closed field of characteristic zero andf
Ek[xl, ... , x"+ 1 ]
apolynomial
over k. Let Y denote the zero set off
in affine(n
+1)-space An+1 over
k andY,
1~I,
its reduced irreducible components. We exclude the trivial casef~k,
so Y is a subscheme of codimension one of An+1.We fix an embedded resolution
(X, h)
for Y in An+1 in the sense of Hironaka’sMain Theorem II
[Hi,
p.142] by
means of monoidal transformations.Recall that if
g: ~ Z
is a monoidal transformation orblowing-up
of thescheme Z with center a subscheme D of Z, then the
exceptional
divisorE = g - 1 D
iseverywhere
of codimension one onZ,
and the restrictiong|BE: BE ~ ZBD
is anisomorphism.
For any subscheme Vof Z,
the closure ofg-1(VBD)
inZ
is called the stricttransform
of Vby
g. If Z and D arenonsingular varieties,
then the same is true forZ
and E.The embedded resolution
(X, h)
consists of thefollowing
data.Set
Xo = An+1, Y(0) = Y,
andY(0)l = Yl
for all l~I. Fori = 0,...,
r - 1 wehave a finite succession of monoidal transformations
gi:Xi+1 ~ Xi
withirreducible
nonsingular
centerDi
cXi
andexceptional variety E(i+1)i+1
cXi+1
subject
to thefollowing
conditions.Let
E(i+1)j,
Y(i+1) andY(i+1)l dénote
the strict transformof respectively E(i)j,
y(i)and
¥Í(i) by gi for j
=1,...,
i and all l~I. Then(1)
for i =0,...,
r -1 we haveDi
cY(i), codim(Di, Xi) 2,
and themultiplicity
on y(i) of all
x E Di equals
the maximalmultiplicity
on Y(i)(i.e.
03BCx(Y(i)) = maxy~Y(i)03BCy(Y(i))
for allxeD,);
(2) U1jiE(i)j has only
normalcrossings
andonly
normalcrossings
withDi (in
X i) for i = 1,..., r-1;
and(3) (U1jr E(r)j)~(Ul~I Y(r)l) = [(gr-1 ° ··· °g0)-1(Y)]red
hasonly
normal cross-ings
inX r .
Inparticular
all¥Í(r), l~I,
arenonsingular.
A reduced subscheme E of codimension one of a
nonsingular variety
X is saidto have
only
normalcrossings
with a subscheme D ofX,
if for all x E D there exists aregular
system ofparameters
t1, ..., tm in the localring OX,x
of X at xsuch that the ideal in
OX,x
of each irreducible component of Econtaining
x isgenerated by
one of the th and the ideal of D inOX,x
isgenerated by
some of theti. When D = X we say that E has
only
normalcrossings.
Now we set
X = Xr
andh = gr-1 °···° g0.
The numerical data of the resolution(X, h)
for Y are defined as follows.For all irreducible components E
of (h-1 Y)red (i.e.
for allE(r)j,
1j
r, and all¥Í(r),
l~I),
let N be themultiplicity
of E in the divisor off
O h on X, and let v -1 be themultiplicity
of E in the divisor ofh*(dx 1
^ ... Adxn+1)
on X. We haveN,
v E
No;
and if Y isreduced,
then all¥Í(r)
have numerical data(N, v)
=(1,1).
From now on we fix
one j~{1,..., r}.
We will describe how the
exceptional variety Ej
and its intersections with otherexceptional
varieties and with the strict transform of Ychange by
theblowing-ups gi, j
i r. So we fix one such gi :Xi+1
~X and
setWhen
Y(i)k, k~I,
orE(’),
1 k i, intersectsE(j),
we set alsoSince E has normal
crossings
with D we have thefollowing important
fact(see e.g. [GH, p. 605]).
PROPOSITION 1.1. The restriction
g IÊ: ~
Eof g
toÊ
is theblowing-up of
Ewith
(nonsingular)
center D n E.Note that D n E can
eventually
be reducible. The totalblow-up
of E withcenter D n E can then be considered as the result of consecutive
blowing-ups
ofE with centers the irreducible components of D n E.
(Because
E has normalcrossings
with D these centers aredisjoint.)
PROPOSITION 1.2. Let E* denote the
exceptional
divisorof the blowing-up gIÈ:
É - E,
andZ
the stricttransform
inE of
any subscheme Zof
Eby g IÈ.
Thenand if codim(D
nE, E) > 2,
we have(For
an eventualproof
see[V, Prop. 3.2].)
The
remaining
situationcodim(D
n E,E)
= 1 occurs if andonly
if D c E anddim D = n - 1. In this case g
IË: ~
E is anisomorphism making
E*correspond
to D. When D is not contained in
respectively ( Yk
nE)rea
andEk
n E,Proposition 1.2(ii)
above is still valid. In the other case we havePROPOSITION 1.3. Let E* denote the
exceptional
divisorof
theblowing-up g|: ~
E.If some
irreducible componentof (Yk
nE)rea
isequal
toD,
then we canhave in a small
enough neighbourhood of
thegeneric point of
E* eitherIf
some irreducible componentof Ek
n E isequal
toD,
then we have in a smallenough neighbourhood of
E*always
Now remember that we have fixed
one j~{1,..., r}.
In Section 2 we constructa
representative
of the self-intersection divisorof Ej (in
the different stages of theresolution
process), involving expressions
in the N-data. We use this result to prove the congruences A in Section 3 and the congruences Bl and B2 in Section 4. In Section 5 we state theanalogous
congruences for v-data. Then in Section 6we
give
someexamples
where the congruences for N-data can be used in thestudy
of thetopological
zeta function.2. The self-intersection divisor on an
exceptional variety
We first fix some notation
concerning
intersections. For anynonsingular variety
V of
dimension m,
letA(V)
denote the Chowring of E
i.e.A(V) = ~mi=0 Ai(V),
where
Ai(V)
denotes the group ofcycles
of codimension i on V modulo rationalequivalence
fori=0,..., m.
LetU·W~Ak+l(V)
denote the intersection of U EAk(V)
and W EA(V). (If
U and W are varieties we can consider U - W also inA’(U)
orAk(W.)
Let also for any inclusion03B3:E
X of codimension one ofnonsingular
varieties E2 = E. E denote the self-intersection divisor of E inX,
considered as an element ofA1(E)(=Pic E).
Remember in this context that inPic E we have
E2 = 03B3*E.
Set
during
this section N =Nj,
and let y :E(r)j
X denote the inclusionof E(r)j
in X.
PROPOSITION 2.1. Set E =
E(r)j.
LetEi,
i ET,
be the intersectionsE(r)i
n E orY(r)i
n Eof
E with anotherexceptional variety E(r)i
or with a reduced irreducible componentY(r)i of
Y(r). Then in Pic E we haveProof. By
definition of the N-data we have in Pic Xand thus
Because
(U1irE(r)i) ~ (Ul~I Y(r)l
hasonly
normalcrossings
in X,applying
thepull-back homomorphism y* :
Pic X ~ Pic E to thisequality yields
We shall now describe how the
expression
ofProposition
2.1 for the self-intersection divisor
changes during
the resolution process. Weessentially
use thefollowing.
LEMMA 2.2. Let Z be a
nonsingular variety,
D a propernonsingular subvariety of Z,
and TI:~
Z theblowing-up of Z
with center D andexceptional variety
F.Let C be a
prime
divisorof Z and y
themultiplicity of
thegeneric point of D
on C(so
J.l =1= 0 ~ Dc C).
Let alsoC
denote the stricttransform of
C ini
and the restrictionII |: ~
C. Then in PicC
we haveProof.
Let yand y
denote the inclusionof respectively
C in Z andC
inZ,
andconsider the commutative
diagram
Applying
thepull-back homomorphism y*
to the well-knownequality
II* C =
C PF
inPic Z yields *03A0*C = 2 + 03BC · F in Pic C.
On the other handwe have
*03A0*C=*03B3*C
=fi *C2.
Bothright-hand
sides thenyield
the statedequality.
DFix one
blowing-up gi|E(i+1)j: EY+
1)Ejl
withDi
nE(j)
:0QS,
and one irre-ducible component D of
Di n E(j).
Set E =E(i)j
and let g :~
E be theblowing-
up with center D, which can be considered as a
composition
factor ofgi|E(i+1)j.
(We
suppose g to be the firstblowing-up
in thedecomposition
into suchfactors.)
Let also
Eé
denote theexceptional variety of g
andE’
the strict transformby g
ofany
prime
divisor E’ in E.PROPOSITION 2.3. First case:
codim(D, E)
2.If NÊ2 = 1: aiE;
+aE’e in Pic É,
thenand
where ô = 1
if Di
c E and ô = 0if Di cf.
E; and J-li, 1 i t, is themultiplicity of
the
generic point of
D onE¡.
Second case :
codim(D, E)
= 1.If N2 = ~ti=1 ai’i
+aE’e
in PicE,
thenProof.
First caseFig. 1.
Because
E has normalcrossings
withDi,
Lemma 2.2implies
that2 =g*E2-03B4E’e.
SoSince Pic
E
=g*
Pic E ~ZE’e (where g*
isinjective),
we get the statedequalities.
Second case.
Fig. 2.
In this situation we have D =
Di
c E, so Lemma 2.2 nowimplies
thatÊ2
=g*E2 - Eé.
Sinceg* :
Pic E ~ PicE
is anisomorphism
that makes Dcorrespond
toEé,
we havewhich
implies
statement(iii).
D3.
Congruences
associated to theblowing-ups
of anexceptional variety
To
simplify
notations we nowdrop
thej-indices, i.e.,
we set E(i) =EY)
for alli =
j,...,r and N = Nj.
Fix one
blowing-up gi|E(i+1): E(i+1) ~ E(i)
such thatDi r) E(’):0 Qf
andcodim(Di
nE(’), E(i)) 2,
and one irreducible component D ofDi
~ E(i). We willassociate a congruence between numerical data to the
blowing-up
g of E(’) with center D, which can be considered as acomposition
factor ofgi|E(i+1). (Here
wesuppose g to be the first
blowing-up
in thedecomposition
ofgi|E(i+1),
into suchfactors.)
The
Propositions
1.1-1.3imply
thefollowing.
PROPOSITION 3.1.
(i)
LetEi,
k ET,
be the reduced irreducible componentsof
intersections
of
E(’) with otherexceptional
varietiesE(i)t,
1 t i, or withcomponents
Y(i)l,
1 E1, of
the stricttransform Y(’) of Y
Therepeated
stricttransform of Ek
in E(r)by
the consecutivegl|E(i+1):
E(l+1) ~E(l),
i 1 r, isequal
to someirreducible component
of
the intersectionof
E(r) with another componentof (h-1 Y)red’
say withE(r)k
orYic(r).
(ii)
LetEé
denote theexceptional variety of
theblowing-up
g. Also therepeated
strict
transform of Eé
in E(r)by
the otherfactors of gi IE(i+ 1)
and the consecutivegl|E(l+
1): E(l + 1) ~E(l),
i + 1 1 r, is an irreducible componentof
the intersectionof
E(r) with some otherexceptional variety,
say withE(r)e.
REMARK 3.2. In the
proposition
aboveE(r)k
is different from thecorresponding E(r)t and/or 1
if andonly
if the center of somegl|E(l+1):
E(l+1) ~E(l),
i l r,contains the
repeated
strict transform ofEk
in E(’). The same remark holds forEfr)
andE(r)i+1.
THEOREM 3.3.
Using
the same notations as inProposition
3.1 we have thefollowing
relation between the numerical dataof E(r), E(r)e,
andE(r)k
orY(r)k,
k E T. Let,uk, k E T, be the
multiplicity of
thegeneric point of
D onE’k.
ThenMore
precisely,
suppose that therepeated
stricttransforms of E’e
andEi, k
eT,
occur in the next steps
of
the resolution processrespectively
me and mk times as centerof blowing-ups gl|E(l+1):
E(l+1) ~E(l),
i + 1 1 r. Thenwhere b = 1
if Di
c E(i) and 03B4 = 0if Di cf.
E(i).Proof. Starting
with theexpression
ofProposition
2.1 for N times the self-intersection of
E(r),
weconsecutively apply Proposition 2.3(i)
or2.3(iii)
to allcomposition
factors of thegl|E(l+1), r
> l i + 1 and to all factors ofgi|E(i+1)
except g(in
the inverseorder).
We obtainwhere
É is
theblowing-up
of E(i)by g
andÉk, k
e T, is the strict transformof E’k by
g. Then
by Proposition 2.3(ii)
we havewhich is
equivalent
to the stated relation. DREMARK 3.4. All
N,, corresponding
to intersections onEj arising
after thecreation of
Ej
asexceptional variety,
can thus be written as linearexpressions (with integer coefficients)
in N and theNk, corresponding
to the intersections at its creation.4.
Congruences
associated to the création of anexceptional variety
In this section we set
E = E(j)j, D = Dj-1, 03A0=gj-1|:E ~ D,
and alsok =
codim(D, Xj-1).
Let be the ideal sheaf of D in
Xj-1.
Then[Ha, II,
Th.8.24]
we know that Ewith the
projection
map n isisomorphic
to theprojective
space bundleP(03B5)
over
D,
associated to thelocally
freesheaf 03B5 = f f2
of rank k on D. We denoteby
C the divisor
corresponding
to the invertible sheafO(1).
in for
example [F,
Th.3.3]
we findPROPOSITION 4.1.
(i)
Thehomomorphism
03A0*:A(D) ~ A(E)
makesA(E)
into afree A(D)-module generated by 1, C, e2,..., Ck-1.
1 n
particular
we have(ii)
Pic E = 03A0* Pic D q)ZC,
where II* isinjective.
So for any
prime
divisor E’ on E, we can write E’ in Pic E as E’ = II* B +dC,
where B E Pic D and d~N. The number d is thedegree
of the intersectioncycle
E’ · F on F, where F ~ Pk-1 is a
general
fibre of II : E ~ D over apoint
of D.(When
E isisomorphic
toPn,
d isjust
thedegree
ofE’.)
Moreprecisely,
F can inthis determination of d be any fibre of IT that does not
satisfy
F 9 E’(only occurring
if d =0).
The
Propositions
1.1-1.3imply
PROPOSITION 4.2. Let
E’i,
i ET,
be the reduced irreducible componentsof
intersections
of E
with otherexceptional
varieties or with the stricttransform of Y
The strict
transform of E’i
in E(r)by
the consecutivegl|E(l+1):
E(l+1) ~E(l), j
1 r,is
equal
to some irreducible componentof
the intersectionof
E(r) with anothercomponent
of (h-1Y)red,
say withE(r)i
orY(r)i.
THEOREM 4.3.
Using
the same notations as inProposition 4.2,
we have thefollowing
relations between the numerical dataof
E(r) andE(r)i
orY(r)i,
i E T. LetE’i
=03A0*Bi
+diC
in Pic Efor
i E T. Then(Congruence Bl)
and
(Congruence B2’)
More
precisely,
suppose that therepeated
stricttransforms of E’i,
i ET,
occur in thenext steps
of
the resolution process mi times as centerof blowing-ups gl|E(l+1):
E(l+ 1) -E(l), j
1 r. Then we have(Relation Bl)
and
(Relation B2’)
Proof. Starting
with theexpression
ofProposition
2.1 for N times the self-intersection of
E(r), repeated applications
ofProposition 2.3(i)
or2.3(iii)
to allcomposition
factors of thegl|E(l+1), r
>l j, yield
in Pic E. Since E2 = - C
(see [Ha, II,
Th.8.24c])
this isequivalent
toNow
by Proposition 4.1(ii)
we obtain the stated relations. 0 REMARK 4.4. When Pic D istrivial,
e.g. when D is apoint,
relation B2’ is ofcourse inexistent.
EXAMPLE 4.5. When Y is a curve
(n = 1), only blowing-ups
with apoint
ascenter occur in the resolution process. We have E ~ P1
and,
since allE’i
arepoints
onE, di
= 1 for i E T. So we obtain the familiar relationFor those
E’i
withdi ~ 0,
the divisorBi
has notreally
a"geometrical meaning".
We will now rewrite relation B2’ in terms of the k th self-intersectionsE’ki
EAk(E)
of thecycles E’i
in E.THEOREM 4.6.
Using
the same notations as inProposition 4.2,
we have thefollowing
relation between the numerical dataof
E(r) andE t or Y(r)i,
i~T. LetE’i
=I-I *Bi + diC
in Pic Efor
i E T. Then(Congruence B2)
More
precisely,
suppose that therepeated
stricttransforms of E’i,
i ET,
occur in thenext
steps of
the resolution process mi times as centerof blowing-ups gl|El+1:
E(l+1) ~E(l), j
l r. Then we have(Relation B2)
in Pic D, where e is the
first
Chern classof
thesheaf
9.Note.
By
theequality (*)
in theproof
below theexpression 03A0*(E’ki) dk-1l
in thetheorem can indeed be considered as an element of Pic D.
Proof.
Fix i E Twith di ~
0. We can writeE’ki
inAk(E)
aswhere
Ok-2
containsonly
terms inCl,
0 l k - 2. Nowby
the definition of Chern classes oflocally
free sheaves we havewhere also
19i-2
containsonly
terms inCl,
0 1 K k - 2. SoFor all l 2 we have dimek-l > dim D and thus
03A0*(Ck-l)
=0;
theprojection
formula
(see
e.g. Ha[p. 426])
thenimplies
thatSince
03A0*(Ck-1)
=D,
we obtainWe now substitute the equalities kBi=03A0*(E’ki) dk-1i
-
dle, i~T and di~ 0,
in(k times)
relation B2/. Thisyields
Using
relation Bl in the termsinvolving
e, we getOne can prove
by
localcomputations
that theE’i t with di
= 0 neverbelong
to thestrict transform yU) of Y in XU) and that
consequently
their associated number mi is zero.Considering
this fact we obtain the stated relation. 0 EXAMPLE 4.7. When Y is a surface(n = 2),
weonly
needblowing-ups
with apoint
or anonsingular
curve as center in the resolution process.(When
D is apoint,
relation B2 is of courseinexistent.)
If D is anonsingular projective
curve, then relation B2 becomes a numerical relationby taking degrees
in Pic D. Lete =
deg
eand xi
=deg E’2i,
iE T,
the self-intersection number ofE’
in E. Weobtain
(When E’i
=TI* Bi
we must havedeg Bi
= 1 sinceE’i
isirreducible.)
REMARK 4.8. In
[V, Prop.
7.1 and Ex.7.2]
we showed how to compute the divisors03A0*(E’ki)
of Theorem 4.6 in terms of concrete intersectioncycles.
5.
Congruences
between v-dataCombining
the relations between N-data and the relationsproved
in[V],
wecan
immediately
derive relations between v-data. Moreprecisely,
a combinationof respectively
Theorem 3.3 and[V,
Th.4.4],
Theorem 4.3 and[V,
Th.6.2],
andTheorem 4.6 and
[V,
Th.6.5] yields
thefollowing
theorems.THEOREM 5.1.
Using
the same notations as inProposition
3.1 we have thefollowing
relation between the numerical dataof E(r), E(r)e, and Er)
or1k(r), k
e T. LetIlk,
k E T,
be themultiplicity of the generic point of D
onEi.
Then(Congruence A)
where d =
codim(D, E(i).
THEOREM 5.2.
Using
the same notations as inProposition 4.2,
we have thefollowing
relations between the numerical dataof
E(r) andE,
orY(r)i,
i E T. LetE’i
=TI*Bi
+diC
in Pic Efor
i E T. Thenwhere k =
codim(D, Xj-1);
andin Pic
D/v
Pic D, whereKD is
the canonical divisor on D.Moreover we can
fully
write out thecorresponding
relations with the same’quotients’
as theanalogous
N-relations.6.
Application
to thetopological
zêta functionLet K be a number field and R its
ring
ofalgebraic integers.
For any maximal ideal p ofR,
letRp
andKp
denote thecompletion
ofrespectively
R and K with respect to thep-adic
absolute value.Let Ixl
denote this absolute value forXE Kp,
and
let q
be thecardinality
of the residue fieldRp/pRp.
Let
now §
be a character ofRxp
of orderd,
and letf(x)~K[x],
x =
(x 1, ... , xn+1).
To these data one associatesIgusa’s
local zeta functionA
where
|dx| denotes
the Haar measure so normalized thatRn+1p
has measure one.One can compute
Z03C8(s) using
an embedded resolution forf
= 0 in An+1. Let(X, h)
be such aresolution, using
now all notations of Section 2. We also set S= {1,..., r} ~
I andE(r)l
=Y(r)l
for 1 e I.Denef [D,
Th.2.2] proved
thefollowing
formula.
THEOREM 6.1.
Let §
be a characterof Rxp
which is trivial on 1 +pRp . Then for
almost all p
(i.e. for
all except afinite number)
we havewhere
CI,03C8(~C) depends on 03C8
and thepoints of i~I E(r)i.
Now to d and
f
we can also associate thetopological
zeta functionwhere
ÉI = (~i~IE(r)iBUj~SBIE(r)j)
Here for any scheme V of finite type over Kwe denote
by X(V)
the Euler-Poincaré characteristic ofV(C)
with respect tosingular cohomology.
This zeta function can be constructed as a limitof Igusa’s
local zeta functions and does not
depend
on the choice of the resolution(X, h) for f [DL,
Th.2.1.2].
If the
monodromy conjecture [D, Conj. 4.3]
is true, we expect thefollowing.
Fix j~ {1,..., rl.
IfEr)
is ’ingeneral position’
with respect to its numericaldata,
i.e. there is no
E(r)i i~SB{j}, intersecting E(jr)
withvi N Ni
=vj Ni and
ifx((j)
=0,
then the contribution of
E(jr)
to the residue of thecandidate-pole - vj
forZd,top(s)
is zero. We willgive
someexamples
of thissituation, using
thecongruences of this paper.
We now suppose n =
2,
we fix oneEr)
’ingeneral position’
such thatdl Ni
andwe set
(as
inSection 4) E = EY), D = Dj-1, 03A0=gj-1|E ~ D,
and(N, v)=(Nj, vj).
LetRd
denote the contribution ofEr)
to the residue of thecandidate-pole - v
forZd,top(s).
EXAMPLE 6.2.
Suppose
D ~P1,
card T = k3, di
=d2
=1, E’ n E’
=0.
and d.
= 0 for i =3,..., k (Fig. 3).
Sox({j})
= 0.Suppose
also thatE(r)j ~
E.Fig. 3.
Let
(Ni, vi)
be associated toE’i
as inProposition
4.2 and set (03B1i = Vi- v Ni
fori=1,...,k.
When d = 1 we have
Now
by [V,
Th.6.2]
there is the relation(03B11+03B12 = 0
between numericaldata, implying
thatRd
= 0.But if for
example
we should haved|N1
andd N2,
thenand there is no relation between numerical data available to make this
expression
zero. Now because of Theorem 4.3 this situation isimpossible
sincecongruence Bl states that
implying that d |N1 ~ d |N2.
EXAMPLE 6.3.
Suppose
D &épl,
card T =4, dl = d2
=d3
=1, d4
=0,
and thecurves
E’, ... , E’4
intersect asgiven by Fig.
4. Sox({j})
= 0.Suppose
also thatEr)
is obtained from Eby
oneblowing-up
with center P andexceptional
curveE’ (Fig. 5).
Fig. 4. Fig. 5.
Let
(Ni, vi)
be associated toE’i
as inProposition
4.2 or 3.1 and set 03B1i = Vi-v V Ni
Nfor i = 1,..., 5.
When d = 1 we have
There are the relations
implying
thatSo
Rd=0.
Now if for
example dN1, dAN 2’
andd Ni
for i =3, 4, 5;
then we haveand we cannot make
Rd
zeroby using
the available relations. We will show that thissituation,
and moregenerally
any’problem situation’,
cannot occur.By using [V,
Ex.7.2]
we can compute the self-intersection numberK1 = 2
andk2 = k3 = 0.
SoExample
4.7gives
the relationNow set
E’1
= C +b1 f
in Pic E = ZC~ Zf,
wheref
is any fibre of II and Ccorresponds
to the invertible sheafO(1)
on E. Thenk1(=degE’21)=e+2b1,
which
implies
that e is even. We can thus derive the congruenceMoreover
by
congruence A of Theorem 3.3 we haveBecause of
(i)
and(ii)
we now see thatimplying
thatRd
= 0 for all d.References
[D] J. Denef, Local Zeta Functions and Euler Characteristics, Duke Math. J. (to
appear).
[DL] J. Denef and F. Loeser, Caractéristiques d’Euler-Poincaré, Fonctions Zeta locales, et modifications analytiques (to appear).
[F] W. Fulton, Intersection Theory, Springer-Verlag, 1984.
[GH] P. Griffiths and J. Harris, Principles of Algebraic Geometry, John Wiley and Sons, 1978.
[Ha] R. Hartshorne, Algebraic Geometry, Springer-Verlag, 1977.
[Hi] H. Hironaka, Resolution of singularities of an algebraic variety over a field of characteristic zero, Ann. Math. 79 (1964), 109-326.
[I] J. Igusa, Complex powers of irreducible algebroid curves, in Geometry today, Roma 1984, Progress in Mathematics 60, Birkhaüser (1985), 207-230.
[L] F. Loeser, Fonctions d’Igusa p-adiques et polynômes de Bernstein, Amer. J. Math. 110 (1988),
1-21.
[M] D. Meuser, On the poles of a local zeta function for curves, Inv. Math. 73 (1983), 445-465.
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[V] W. Veys, Relations between numerical data of an embedded resolution, Amer. J. Math. (to appear).