C OMPOSITIO M ATHEMATICA
H. C. P INKHAM
Automorphisms of cusps and Inoue- Hirzebruch surfaces
Compositio Mathematica, tome 52, n
o3 (1984), p. 299-313
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299
AUTOMORPHISMS OF CUSPS AND INOUE-HIRZEBRUCH SURFACES
H.C. Pinkham *
© 1984 Martinus Nijhoff Publishers, The Hague. Printed in The Netherlands
Introduction
In
[8]
Inoue constructs afamily
of minimalcompact complex
surfaces Swith no
meromorphic functions,
first Betti numberequal
to 1 and secondBetti number
positive.
These are surfaces oftype VIIo
in Kodaira’sclassification
[9],
and are nowgenerally
called Inoue-Hirzebruch surfaces.The construction which is
explained
in Section 1 but need not concern usyet, depends
on modules in realquadratic
fields.The main purpose of this paper is to determine the full group of
complex automorphisms
of S.By
the same method we obtain an interest-ing
group ofautomorphisms
of"cusp" singularities,
which we nowdescribe.
The
only complex
curves on S arearranged
in 2 connected compo- nentsconsisting
of rational curvesC0,...,Cr-1,
andD0,...,Ds-1,
botharranged
in acycle,
i.e. if r > 1:and if r = 1:
The intersection
matrices 1 Ç - 01 and 1 Di - Djl are negative definite,
so thateach connected
component
can be contracted to a normalsingular point,
* Supported in part by N.S.F. Grant # MCS 8005802, Columbia University.
called a cusp
(Hirzebruch [5], §2).
Call them p and q, and the contracted surface S’. Since each cusp occurs onprecisely
one Inoue-Hirzebruchsurface,
the second cuspappearing
on S’ iswell-defined,
and called the dual of the first. Thisduality
has been studiedby Looijenga [10]
andNakamura
[11]
and is ageneralization
of thestrange duality
of Arnold[1].
A somewhat incidental purpose of this paper is to show that there is alattice theoretic
explanation
for theduality, along
the same lines as theexplanation
of thestrange duality given
in[14],
at least for those cusps that have aninteresting
deformationtheory.
This is done in the last section.(The unicity
statementconjectured
in[14]
can be verifiedusing
the work of Nikulin
[13].)
Theonly
new idea here is to embed twoapparently
unrelated lattices asorthogonal complements
in a unimodularlattice, using
results of[13].
This construction is the lattice theoreticanalog
of ageometric
construction ofLooijenga ([10] Prop. 2.8).
Themain result of this section is used to
study
the deformationtheory
ofcertain cusps in
[18].
This
explanation
of theduality,
and indeed the rest of this paper,depends
on a certain finite abelian groupT,
which we now define.Remove the curves
UC,
andUDJ
from S(or
pand q
fromS’,
if youprefer).
Call theremaining (smooth) variety
S". Inoue([8], §4)
shows thatS" is
homeomorphic
to R X T, where T isan S’ X S
1 bundle overSI.
Then T is the torsion
subgroup
ofH1(, Z).
In the course of the determination of the
automorphism
group of S wewill see that it contains a
subgroup isomorphic
to T which actstrivially
on
H2 ( S, Z).
Thequotient by
anysubgroup
of T isagain
an Inoue-Hirzebruch surface
(Section 2).
Let me concludeby
thefollowing
con-crete
corollary
of myresults,
which wasactually
thestarting point
of thisinvestigation:
COROLLARY: Consider the
hypersurface
cusp :(the
resolutionof
the cusp isgiven, for example,
in[11],
Lemma 2.5 : the dual cusp has three components withself
intersections -(
p -1), - ( q - 1),
-
( r - 1).)
Then T isisomorphic
to the groupG~{03BB, 03BC, 03BD~|03BBp = 03BCq = 03BDr = 03BB03BC03BD} acting by x - Xx,
y - ity, z - vz, and thequotient of
the cuspby
G is the dual cusp.Note that J. Wahl has considered
examples
ofquotients
of cusps in[21],
5.9.4.1. Review of known results
The results in this section come from
[2],
pp.39-53, [5], §2,
and[8].
Seealso
[17].
Throughout
this paper M denotes acomplete (or full,
in the terminol- ogy of[3])
module in the realquadratic
field K over Q. An excellentaccount of the results we need from number
theory
isgiven
inChapter
2of
[3].
As usual if x EK,
x’ denotes theconjugate
of x. We will consider twoequivalence
relations on modules M :M,
andM2
areequivalent (resp. strictly equivalent)
if there exists an element Y EK, (resp.
y >0, y’
>0),
such thatyMl
=M2.
For any strictequivalence
classrepresented by
M there is aunique
strictequivalence
classrepresented by 8M, 8
> 0 and 8’ 0. This is denoted M*. 1 will often abuselanguage
and use M todenote the
(strict) equivalence
class of M as well as M itself.Let
Um
andU£
be the groups ofpositive
andtotally positive
units ofM, respectively;
e.g.Both groups are infinite
cyclic
and[UM : UM is
either 1 or 2.We consider a
subgroup V
of finite index inUM
and let a denote agenerator
of V.The semi-direct
product G ( M, V)
acts on H X C(and
0-0 XH,
whereH is the upper half
plane) by
The group structure on
G(M, V)
isgiven by:
The action is free and
properly
discontinuous in both cases. LetS"( M, V)
be thequotient
of H Cby
thisaction,
andX’’(M, V)
thatof H H. Both spaces are smooth
complex
spaces, but of course notcompact.
We first need to understand thetopology
ofS"(M, V)
orequivalently X"( M, V).
where x 1, x2, y1, y2 are real coordinates. 0-0 X C is fibered
by
subvarietiesWd
={(z1, z2)~
U-0 XC 1 y, -
y2= d},
invariant underG( M, h).
The quo-tient Td
fibers over{(y1, y2)~R R IYIY2 = d}/V
whichis just S1,
andthe fiber is
{(x1, x2) E
R XR)/M
whichis just SI
XS1. Therefore Td
isan S X SI bundle
overS1.
Since itclearly
does notdepend
ond,
we nowdrop
thesubscript
d. Themonodromy
of T, which is itsonly invariant,
isgiven by
the action of a, thegenerator
ofV,
on M. Therefore from theWang
sequence oneeasily deduces,
as in[8], §4 Eqn. (24)
that the torsionsubgroup
ofH1(, Z)
isM/(03B1-1)M.
We call this groupT(M, V).
Another more direct way of
computing T( M, V)
will be useful later:G ( M, V)
is the fundamental group of T so that ifG’( M, V)
denotes the commutatorsubgroup of G ( M, V) then H1(, Z) = G(M, V)/G’(M, V).
Thus the
following
lemmagives T(M, h):
T( M, V)
is fundamental for the rest of ourinvestigation.
It is of courseisomorphic
toZ/e ~ 1Lif
where e andf
are theelementary
divisors ofa - 1 viewed as an
endomorphism
of M.We have seen that
S"( M, V)
ishomeomorphic
to R X T.We will now
compactify S"(M, V) by adding
twocycles
of rational curves, one at + oo, the other at - oo in therepresentation S"( M, V) ~
R X T. We can of course do each
cycle separately,
so let’s do thecycle
at+ oo first. We can therefore restrict the action to H x H. From this
point
on I will
mainly
use the notation -from Hirzebruch[5],
Section2,
which differs from that of Inoue.The module M is
strictly equivalent
to a moduleM( w ) generated by
1and w, where w E K is
reduced,
i.e. w > 1 > w’ > 0. Since the construction that follows iseasily
seen todepend only
on the strictequivalence
classof
M,
we may as wellreplace
Mby M(w).
w has apurely periodic
modified continued fraction
expansion
w =
[[bo, bl , ... br- d]
where allthe b,
are 2 andsome b,
is 3.(For
basic information on modified continued fraction
expansions
seeHirzebruch
[5], 2.3.)
Here r does not denote thelength
of theprimitive period
of w, but that of thedegree [U+M : h ] period :
cf. the theorem p. 216 of Hirzebruch.Take an infinite number of
copies of C2,
indexedby k E 1L,
withcoordinates uk and vk . Glue them
together by
Call this space Y. The curve
Ck given by
uk+1= 03C5k = 0
isa Pl
1 withself-intersection - bk .
Thegroup V acts freely
onY,
with asending
thepoint
with coordinates( uk, vk )
in the k-th chart to thepoint
with thesame coordinates in the k + r-th chart.
We have an
isomorphism
defined on the 0-th coordinate chart of Y
by
We now restrict (D
to 03A6-1(H
XH/M(w)).
03A6 iscompatible
with theaction of V on both
sides,
so that we canpatch Y/V
toX"(M(w), V) ~
H
H/G(M(w), V).
Call theresulting
spaceX(M(w), V).
We haveadded to
X"(M(w), V)
acycle
of r rational curvesC,, 0 i r
withself-intersections -b0, -b1,...,-br-1, or - bo + 2
if r = 1. The condi-tion on
the b,
isequivalent
to the intersection matrix(Cl · Cj) being negative definite,
so we can contract the curvesC,
to a normalsingular point
p, which is a cusp(in
dimension2,
a cusp is any isolated normalsingularity having
a resolution withexceptional
divisorconsisting
of acycle
of smooth rational curves, or with an irreducibleexceptional
divisorthat is a rational curve with
a node). By
suitable choiceof w,
henceM,
one can obtain all cusps in this fashion. We call the contracted space
X’(M(w), V).
For later purposes we need to be able to write down a set of generators for thering
ofholomorphic
functions at thesingular point of X’( M( w ), V).
Let M* be the dual lattice of M under trace, i.e.
M* = {v~Q(w)|vm
+ v’m’ ~ Z, m ~ M} .
This use of * does notreally
conflict with ourprevious
definition since oneeasily
sees(Nakamura [12],
Section6)
thatthe dual under trace of M is
strictly equivalent
to our old M*.For m E
M*, m totally positive,
letAccording
to Hirzebruch[5],
Section2, Eqn. (4),
these Fourier seriesgenerate
theconvergent
power seriesring
of the cusp(in [12], §6,
Nakamura shows how to find a minimal set of
generators,
but we will not need hisresult.)
We now return to the surface
S"( M, V) ;
we want to add acycle
ofrational curves at - oo. For this we must look at the action of
G ( M, V)
on H X L
(L
= lower halfplane).
This amounts tolooking
at the action ofG(M*, V)
on H XH,
so that if M*= M(w*),
w* reduced with modified continued fractionexpansion [[c0,...cs-1]],
then we must add on acycle
of rational curves
Do,... D,-, with self-intersections -c0, -c1,...,-cs-
1 or - co + 2 if s = 1. There is asimple algorithm
forgetting
fromthe b,
tothe c,, which first occurs in a paper of
Hirzebruch-Zagier ([6],
p.50)
andlater much studied
by Looijenga [10],
Wahl and Nakamura[12].
The surface obtained
by glueing
on bothcycles
of rational curves toS"( M, V)
is called the Inoue-Hirzebruch surface oftype (M, V)
and isdenoted
S( M, V).
If bothcycles
of curves are contracted topoints p
andq we
get
thesingular
Inoue-Hirzebruchsurface,
denotedS’( M, V).
As mentioned in the introduction the cusp q is called the dual of the cusp p.2. The
automorphism
group of Inoue-Hirzebruch surfacesLet
K, M, V,
etc. be as in Section 1. The module(a - 1)-1M,
which wewrite M
from now
on, isequivalent
to M so we can form the semi-directproduct G(M, UM).
Recall(Section 1)
thatUM
is the group ofpositive
units of M. The
following
lemma is a trivialcomputation.
LEMMA:
G ( M, V) is a
normalsubgroup of G ( M, UM).
We can now state the main theorem of this paper.
THEOREM :
G ( M, UM)/G(M, V) is
thefull (complex) automorphism
groupof S(M, V), S’( M, V)
andS "( M, V). A ny subgroup of G(M, UM)/G(M, V) is of
theform G(N, W)/G(M, V)
and thequotient of S( M, V) (resp. S’, S") by
such asubgroup
is"bimeromorphically"
S( N, W ) ( resp. exactly S’, S").
Note: if W =
UM Um,
thenS( N, W)
denotes thequotient
ofS( N, Um) by
the involution associated to the non-trivial element ofUM/U+M (cf. [8],
Section
6).
The
proof
is in two steps. First we show the group inquestion
is theautomorphism
group ofS"( M, V)
and second we show it extends to S and S’. The secondstep
is easyby general
considerations but wegive
amore
computational proof
in order to exhibit the form of the automor-phisms explicitly.
Step
IIt is clear that any
automorphism
of S or S’ restricts to anautomorphism
of
S",
sinceSBS"
consists of all thecomplex
curves ofS,
andS’BS"
ofthe
only singular points
of S’.So consider any
automorphism f :
S" - S". S" has H C as universal cover, andf
lifts to anautomorphism
F: H C ~ H C which satisfies thefollowing equivariance property
withrespect
toG ( M, V):
where z E H X
C,
g EG(M, V),
h a groupautomorphism
ofG(M, V)
and the action of
G ( M, V)
on U-0 C described in Section 1. Moreexplicitly
write z =( zl, z2), zi e H, z2 ~ C;
g =( v, m), v ~ h, m E M;
h(v,m) = (h1(v, m), h2(v,m))
whereh
1 is a grouphomomorphism
G ( M, V) - V
andh2
a mapG ( M, V) ~ M satisfying
thecocycle
ruleh2(g1g2) = h1(g1)h2(g2) + h2(g1).
Now V is abelian so
h
1 factorsthrough
thequotient by
the commuta-tor
subgroup
G’ ofG(M, V)
whichby
Section 1 consists of(1, m), m~(03B1-1)M.
We will oftenidentify
G’ with( a - 1 ) M. Restricting
toG’ we see that
F(z) = (f1(z), f2(z))
satisfiesfor m E
G’,
whereh 2
is now ahomomorphism
of G’.Thus
~fj/~zl
isperiodic
withrespect
toG’,
so that it has a Fourier seriesexpansion
where * denotes dual under trace, as in Section 1. Now use the
equivari-
ance of F with
respect
to V. Sinceh1(03B1, 0)
=ak
for someinteger k,
so for
example taking the f1
term:so that the coefficients of the Fourier series of
afl/azl satisfy
This series must converge in H
C,
inparticular
when z1~ i~,
andZ2 ~
± ioo.
A standardargument (see
forexample [17],
Section1)
thenimplies
that all the coefficients of the series are 0except perhaps
theconstant term.
Therefore f1(z)
= az+ bz2
+ c, where a,b,
c~C. Sincez2~C and f
ltakes values in
H, b
=0, so fl
is a functionof zl
alone. Recall thatso that
Next set v = 1. Then am =
h2(1, m ) E M,
so that a is a unit of M.Since f
1is a map H ~
H, a
must bepositive. Finally
we haveso(1-v)c~M for all v~ V. Thus c~03B1-1)-1M=M.
A similar
analysis
forf2, using
theexpressions
forh1
andh 2 given
above,
showsthat f2(z)=a’z2 + c’.
Thus the groupG(M, UM )
acts onH X
C,
and its action descends toS"( M, Tl )
with kernelG ( M, V).
Thisestablishes
Step
I.Step
IIIt is trivial to see how the
UM/V part
of theautomorphism group
extendsto S and
S’,
so we willonly
concern ourselves with theM/M
part.(In
fact theU+M /
V part of theautomorphism
group is described in[11], 2.2,
and as
already
mentioned theUMI U:;
part in[8],
Section6.)
It suffices of course to show the action extends to
X(M, V)
andX’(M, V).
We will doX(M, V)
first. Wereplace
Mby
aM(w)
in thesame strict
equivalence class,
where w isreduced.
By Eqn. (1)
of theprevious
section m E M acts on(zl, z2) E
H X a-0by m:(z1, z2) ~ (z1 + m, z2 + m’).
Thereforeby Eqn. (3),
m acts onY,
in the 0-th coordinatechart, by m : ( uo, v0) ~ (exp(203C0im1)u0, exp(203C0im2)v0)
where m = mlw + m2; MI, m2 ~ Q.We want this action to descend to an action on
Y/V. By iterating Eqn. (2)
we see thatwhere the
p’s
andq’s
are definedby
By
Inoue[8], Eqn. (4)
andProposition
1.2 we haveSo m acts on the r-th coordinate chart
by
Therefore for the action of M to descend to
Y/V, since ur
is identified to uoby a, and vr
to vo, we must haveor
In other
words,
we must have am = m mod M or m E[1/(a - 1)]M,
which is
precisely
ourhypothesis.
NOTE: Here is another way of
expressing
thiscomputation.
The space Yof Section 1 is the toroidal
compactification ([19],
Section15)
of asubspace of C* C*,
so it admits a C* C* actiongiven
in thecoordinates
by
and
What we have done is
simply
to compute what part of the action descends tothe quotient by
V.Note that
MIM
isisomorphic
to the groupT( M, V)
of theprevious
section.
Let’s now turn to
X’( M, V) ( fm
is definedby Eqn. (4)
in§1).
PROPOSITION :
M/M
acts as a groupof
"monomial "automorphisms,
onthe local
ring of
thesingular point of X’( M, V),
with m~ Macting
onfm’
m~M* =
{v~K|tr(vn)~Z, ~n~M}, by
REMARKS:
(1)
aspointed
outby
thereferee,
since X’ is the Steincompletion
ofX",
allautomorphisms
of X" extend to X’. It is useful to knowexplicitly
how
they extend,
however.(2)
if M isisomorphic
to itsconjugate
module M’ thenX’(M, V)
hasan extra
automorphism
of order 2given
on H X Hby ( zl, z2) ~ ( z2, zl ).
As we have seen in
Step I,
this involution does not extend toS"( M, V).
1have not determined what the
quotient
of X’by
this involutionis. t
Theproof
ofStep
II is nowcomplete.
Theremaining
assertions in the statement of thetheorem, concerning
the type of thequotients,
areobvious.
t See note added in proof.
We have the
following
easycorollary
of theproof
of the theorem:COROLLARY:
(1)
The kernelof the
induced actionof G ( M, UM)/G(M, V)
onH2(S(M, V), Z) is G(M, V)/G(M, V) = M/M.
(2)
The induced actionof G(M, UM)/G(M, V)
onHI( T, Z) =
G(M, V)/G’(M, V)
isgiven by (u, m)~ G(M, UM)
sends(v, m)~
G ( M, V) to ( v,
um +(1 - v ) m ). ( It is
easy to see this action descends tothe
quotients ).
Part
(1)
follows fromStep
II of theproof,
oralternatively
from(2)
of thecorollary,
and Part(2)
is atriviality
fromtopology (we
havejust
writtendown
explicitly
the action ofG(M, UM )
onG(M, V) by conjugation)
which we have
given simply
to expressintrinsically
what was done in the lastpart
ofStep
I.EXAMPLE: Take the
hypersurface
cuspx3 + y3 + z5 +
xyz = 0. Its minimal resolution has 2 curves with self intersection - 2 and - 5. So onepossible
choice for w
is
w =[[2,5]]
= 1 +15/5,
a = 4 +/15B the
norm of a - 1 is-
6,
so thatM/M
iscyclic
of order 6. The action ofM/M
on the cusp isgiven explicitly by
where 03B6
is a sixth root ofunity.
The
quotient by
the full groupgives
the dual cuspx2 + y4
+Z7
+ xyz= 0 with resolution
Quotienting by
thesubgroup
of order 3 we get the(hypersurface)
cusp:and
quotienting by
thesubgroup
of order 2 we get its dual:The
involution x ~ y
is theautomorphism
described in Remark(2)
above.
Much more
complicated examples
can becomputed using
the tables in[7].
3.
Quadratic
f orms onT(M, V)
In this section we fix a cusp
D = X’(M, V)
and its dual D’ -X’( M*, V) : T(M, V)
wenow just
callT,
and the smooth Inoue- Hirzebruch surface on which both cusps have resolutions we call S.The
exceptional
divisor of the resolution of D consists of curvesC0,...,Cr-1;
that ofD’, D0,...,Ds-1.
For therelationship
between the numerical invariants of D and D’ see[10], [11],
or[4].
Let L be the lattice
spanned by Co,..., Cr-l
1 inH2(S, Z)
and L’ thatspanned by D0,...,Ds-1.
It follows from[6], §4 (for
more details see[11],
§4)
that we have two exact sequences:( L*
=Hom( L, Z).)
and
so that T inherits 2 finite bilinear forms with values in
Q/Z
that differby
asign,
since oneeasily
sees that L is theorthogonal
of L’ inH2(S, Z).
My general
reference forquadratic
forms will be[13].
Let us now assume that the
configuration
of curvesCo,..., Cr -
ltogether
with theappropriate
intersection matrix(resp.
the curvesD0,...,Ds-1)
lies in a smooth proper rational surfaceV (resp. h’)
as ananti-canonical divisor. The
importance
of this notion isexplained
in[10]
and
[4]. [4]
uses the awkwardterminology
"rational" cusp to describe thisnotion,
but 1prefer
the lessconfusing periphrase "sits
on a rationalsurface". This will
always imply
thatexceptional locus
of resolution of the cusp is an anticanonical divisor of the rational surface. Denoteby R (resp. R’)
theorthogonal complement
inH2(V, Z) (resp. H2(V’, Z))
ofthe lattice
generated by
theC, (resp. D, ),
which of course isisomorphic
toL
(resp. L’).
NOTE: R and R’ are in
general
notunique: [4], §6.
Thenon-unicity
isrelated to the number of
smoothing components
of D’ andD,
respec-tively.
See[4],
6.1.For
simplicity
let us assume bothembeddings L ~ H2(V, Z)
andL’ c
H2(V’, Z)
areprimitive (examples
in[4], §6,
show this is notalways
the
case).
ThenTHEOREM 1:
(1)
R and R’ are even latticesof
rank 10 - r + s and 10 + r - s,respectively,
andsignature (1, -).
(2) R*/R ~ R’*/R’ ~ T,
and the associatedfinite quadratic forms
qR’qR, : T -
Q/2
Zdiffer by
asign.
(3)
There exists aprimitive embedding of
R into -E8
~ -E8
~ H ~ Hwith
orthogonal complement
R’. H is thehyperbolic plane
and -E8
is theunique negative definite
even unmodular latticeof
rank 8[16].
PROOF:
(1)
follows from theadjunction
formulaon V,
since classes in R donot intersect the canonical divisor. The formula for the rank of R follows from the fact that dim.
Pic(V) = 10 - K 2, where - K 2
=multiplicity
ofD =
length
of D’ = s(see [11]
or[4]).
That thesignature
is of the form(l, - )
follows from theHodge
index theorem.(2) R*/R ~
T since L was assumed to beprimitively
embedded. NowR*/R
andR’*/R’
have bilinear forms intoQ/Z
which differby
asign,
since
L*/L
andL’*/L’ do,
so to check that their associatedquadratic
form into
Q/2lL
differby
asign
it suffices([13],
theorem1.11.3)
to checkthat their
signatures
areopposite
mod 8(this
is theArf-invariant).
Signature Signature
so we are done.
(3)
follows from[13], Prop. 1.6.1, plus
the standard fact that theonly
even unmodular lattice of rank 20 and
signature (2, 18)
is- E8 ~ -E8
~H~H.For
applications
we need aslight improvement
of this result.THEOREM 2:
Suppose
the cusp D sits on a rationalsurface
V and that theembedding of
L inH2(V, ll)
isprimitive.
Let R be theorthogonal of
L inH2(V, Z).
Then a necessary conditionfor
the dual cusp D’ to sit on arational
surface
V’ is that R admit anembedding
into-
Eg ~ -E8
~ H ~ H.PROOF: Same as that of the
previous proposition,
except that we need thecorrespondence
between overlattices of a lattice andisotropic subgroups
of the finite discriminant form
([13], §1.4).
The
hypothesis
that L embedprimitively
inH2(V, Z)
isobviously
satisfied any time every component
D,,
0 i r - 1 meets anexceptional
curve of the first kind of V. This is the case when r is 5 as can be seen
from
[10],
Theorem 1.1.We conclude
by
anexample
which tiestogether
the methods ofSections 2 and 3. We will need an
explicit description
of the map L* - 1 used above.Consider
X( M, V),
where we assume M is in the formM( w )
with wreduced
(Section 1).
Of course L =H2(X(M, V), Z)
and on L* we willuse the dual basis
C*k, 0 k r - 1, of
the curvesCk .
On M we use thebasis w,
1,
and we write the elements of M as row vectors. It is easy to see(the computation
isessentially
done in[20], Example 2.3)
that theisomorphism L*/L ~ T ~ M/(03B1-1)M
is induced from the 7--liner map g: L* ~ M such that(notation
as in Section2)
EXAMPLE: Let D be the cusp
(5, 11, 2),
i.e. r =3, bo
=5, b1
=11, b2
= 2.Then D’ is
(2, 2, 3, 2...,2, 4),
so s =12,
andby [4], Prop. 4.8,
D’ sites 8on a rational surface V’. The group T is
isomorphic
toZ/3 ED 7L/30 ([15],
Lemma
1),
soby [13]
theembedding
of L’ inH2(V’, Z)
cannot beprimitive,
as theorthogonal complement
of L’ inH2(V’, Z)
is one-dimen-sional.
Infact,
if L’ is theprimitive lattice generated by L’,
thenL’ /L’ = Z/3
and a lift of a generator ofL’/L’
to L’ can be written:Using B
one can construct adegree
3 cover ofV’,_such
that if theresolution
of the cusp D’ is contracted to apoint
onV’,
then the coverZ ~ h’ is unramified outside of the cusp, and
totally
ramified there.By
the results of Section 2 it is clear that Z has a cusp above
D’; using
theexplicit description
of the map L’* ~ Tgiven
above we see it isX’( g( L’), V).
In the case at hand we get the cusp(4, 3, 2, 3, 2, 2, 2) (the
dual of
(2, 3, 4, 6))
which hasmultiplicity
4 and hence is acomplete
intersection.
By [11],
Lemma 2.5 itsequations
can be writtenand a direct
computation
shows that theZ/3 quotient
isgiven by (x,
y, z,w) ~ (x,
wy,03C92z, w),
where w is a cube root ofunity.
Z is arational
surface,
as followsdirectly
fromcomputation
or from ageneral
result of
Mérindol,
with trivial canonicaldivisor,
a cusp(4, 3, 2, 3, 2, 2, 2)
and a
Z/3
group ofautomorphisms.
Furthermore we have a one-parame-ter
family
ofsuch,
since v’ itselfdepends
on one modulus.Deformation theoretic consequences of this
construction,
which ap-plies
to all cusps D such that D’ sitsnon-primitively
on a rationalsurface,
will be dealt with elsewhere.Acknowledgements
1 thank C.T.C. Wall for the
interesting
remark that the group G in thecorollary
above isisomorphic
toTopqr/Tpqr,
as defined in[15];
thereferee,
who
provided
several valuable comments on the first version of this paper;finally
the Centre deMathématiques
of the EcolePolytechnique
for their
hospitality
and financial supportduring
the academic year1982-83,
when this paper was revised.References
[1] V.I. ARNOLD: Critical points of smooth functions. Proc. Intern. Cong. Math. Vancouver (1974) 19-39.
[2] A. ASH, D. MUMFORD, M. RAPOPORT and Y. TAI: Smooth compactification of locally symmetric varieties. Brookline, Mass: Math. Sci. Press (1975).
[3] Z.I. BOREVICH and I.R. SHAFAREVICH: Number Theory. New York: Academic Press (1966).
[4] R. FRIEDMAN and R. MIRANDA: Smoothing cusp singularities of small length. Math.
Annalen 263 (1983) 185-212.
[5] F. HIRZEBRUCH: Hilbert modular surfaces. Enseignement Math. 19 (1973) 183-282.
[6] F. HIRZEBRUCH and D. ZAGIER: Classification of Hilbert modular surfaces. In: W.L.
Baily and T. Shioda (eds.), Complex Analysis and Algebraic Geometry. Cambridge University Press (1977).
[7] E.L. INCE: Cycles of reduced ideals in quadratic fields. British Assoc. Advancement science, Math. tables, Volume IV, London (1934).
[8] M. INOUE: New surfaces with no meromorphic functions II. In: W.L. Baily and T.
Shioda (eds.), Complex Analysis and Algebraic Geometry. Cambridge University Press (1977).
[9] K. KODAIRA: On the structure of compact complex analytic surfaces, I and II. Amer. J.
Math. 86 (1964) 751-798 and 88 (1966) 682-721.
[10] E. LOOIJENGA: Rational surfaces with an anticanonical cycle. Ann. Math. 114 (1981) 267-322.
[11] I. NAKAMURA: Inoue-Hirzebruch surfaces and a duality of hyperbolic unimodular singularities. Math. Ann. 252 (1980) 221-235.
[12] I. NAKAMURA: Duality of cusp singularities in: Complex Analysis of Singularities (R.I.M.S. Symposium, K. Aomoto, organizer) Kyoto (1981).
[13] V.V. NIKULIN: Integral symmetric bilinear forms and some of their applications. Math.
USSR Izvestija 14 (1980) 103-167.
[14] H. PINKHAM: Singularités exceptionnelles, la dualité etrange d’Arnold et les surfaces K-3. C.R. Acad. Sc. Paris, Série A, 284 (1977) 615-618.
[15] H. PINKHAM: Smoothings of the
Dpqr
singularities, p + q + r = 22. Appendix to Looijenga’s paper: the smoothing components of a triangle singularity. Proceedings ofthe Arcata conference on singularities (1981). Proc. Symp. Pure Math. 40 (1983) Part 2, 373-377.
[16] J.-P. SERRE: Cours d’arithmétique. Paris: P.U.F. (1970).
[17] K. BEHNKE: Infinitesimal deformations of cusp singularities. Math. Ann. 265 (1983)
407-422.
[18] R. FRIEDMAN and H. PINKHAM: Smoothings of cusp singularities via triangle singulari-
ties. To appear in Comp. Math.
[19] T. ODA: On torus embeddings and its applications. TATA Institute Lecture Notes, Bombay (1978).
[20] P. WAGREICH: Singularities of complex surfaces with solvable local fundamental group. Topology 11 (1972) 51-72.
[21] J. WAHL: Smoothings of normal surface singularities. Topology 20 (1981) 219-246.
(Oblatum 23-VII-1982 & 28-111-1983) Department of Mathematics Columbia University
New York, NY 10027 USA
Note added in
proof
(1)
As J. Wahl haspointed
out, the "extraautomorphism"
considered in Section2,
Remark 2 hasalready
been studiedby
U.Karras,
Math. Ann.215
(1975) 117-129,
Section 3.(2)
Lattice theoreticconsiderations,
somewhat similar to those in Section3;
have been usedby
Wahl andLooijenga
tostudy smoothings
ofall Gorenstein surface