C OMPOSITIO M ATHEMATICA
A LLEN T ANNENBAUM
On the classical characteristic linear series of plane curves with nodes and cuspidal points : two examples of Beniamino Segre
Compositio Mathematica, tome 51, n
o2 (1984), p. 169-183
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169
ON THE CLASSICAL CHARACTERISTIC LINEAR SERIES OF PLANE CURVES WITH NODES AND CUSPIDAL POINTS:
TWO EXAMPLES OF BENIAMINO SEGRE *
Allen Tannenbaum
© 1984 Martinus Nijhoff Publishers, The Hague. Printed in The Netherlands
Introduction
B.
Segre
in[8]
studies families ofplane
curves withsingularities. (See
alsoZariski
[12]
for an account of some ofSegre’s
work on curves with nodesand
cusps.)
Forexample
if we consider a maximal irreduciblealgebraic (i.e. "complete") family
ofplane
curves ofdegree
d withprecisely
8 nodesand K cusps
(by "cusp"
we mean asingularity analytically isomorphic
toy2+x3),
thenSegre
shows that theexpected (" virtual")
dimension of such afamily
should bed(d
+3)/2 -
8 - 203BA(that
is each nodeimposes
one
independent condition,
and each cusp twoindependent conditions).
If a certain first
cohomology
group vanishes(see
Section 1 below for theprecise definition),
then it follows fromgeneral
deformationtheory
thatthis
family
will benon-singular
of dimensionprecisely d(d
+3)/2 -
8 -2 K. If this
cohomology
group is not zero, then the deformations may be obstructed(" the
characteristic series isincomplete"),
and inpoint
of factJ. Wahl in
[11]
constructsexplicitly
such anexample
of an obstructeddeformation space. It may also occur, that the
cohomology
group is not zero, but that the deformations are nevertheless unobstructed. In otherwords,
that thecomplete algebraic family
isnon-singular,
but of dimen- sionstrictly greater
than theexpected
dimension ofd( d
+3)/2 -
8 - 2 K.Such an
example
is constructedby
B.Segre
in[8]
which we will discuss in Section 3 below.Now in
studying
such deformations ofplane
curves withsingularities (the
deformations we arereferring
to areformally locally trivial,
i.e.they
don’t
formally change
thesingularities;
see Section1),
the firstthing
todo is to
identify
the "characteristic linear series" which isbasically
thelinear
system
cut out on ageneral
curve of thefamily by nearby
curves inthe
family.
In the case ofplane
curves with nodes and cusps we will show* This work was partially done while the author was a guest at the Sonder-
forschungsbereich of the University of Bonn.
that the classical Italian
analysis
of this worksby giving
anexplicit
modern
expression
for the characteristic linear series(see
the details in Section 1below).
However for theformally locally
trivial families ofdeformations of
plane
curves withhigher
ordersingularities,
we will showthat the classical
techniques (as
evidencedby Segre [8])
do notgive
acorrect
description
of the characteristic linear series.(See
alsoSegre [7],
Severi
[9],
and Zariski[12]
for an account of these classical works as wellas an extensive
bibliography.)
Indeed in
[8], Segre
has a secondexample
of acomplete family
ofplane
curves ofdegree
6d withprecisely 6d2 - 2
cusps and onecuspidal triple point analytically isomorphic
toy3
+X4. Segre
claims that thisfamily
is obstructedby computing
the characteristic linear series andshowing
that the dimension isgreater
than the actual dimension of thefamily.
However because of the erroneous classicaldescription
of thecharacteristic linear
series, Segre’s
claim about the obstructedness of hisfamily
isfalse,
and we will show inpoint
of fact that hisfamily
isunobstructed
by using
the correct characteristic linear series(see
Section3).
This work was
partially
done while the author was aguest
at theSonderforschungsbereich
of theUniversity
of Bonn. The author wishes to thank Professor F. Hirzebruch for his invitation to come, and the staff for theirhospitality.
1. Some déformation
theory
We will sketch here some of the relevant deformation
theory
fromHorikawa
[4],
Tannenbaum[10],
and Wahl[11] which
we will need in thesequel.
All our schemes will be defined over k a fixedalgebraically
closedfield of characteristic 0. We
begin
with thefollowing
definitions from[11]:
DEFINITIONS
(1.1): (i)
Let V be anon-singular variety,
D c V an effectiveCartier
divisor, ND
the normal sheaf of D in V.Using
the Lichtenbaum-Schlessinger cotangent complex,
define(ii)
Define a functor from thecategory
of finite local artiniank-alge-
bras to the
category
of setsby
H’( A) :
=(subschemes
ofVXSpec k Spec
A flat over Ainducing
D on Vwhich are
locally
trivial deformations of D in the Zariskitopology}.
Then H’ is
pro-representable, H’(k[~]/~2)
=H0(D, N’D)
and smoothness is obstructedby
elements inH1(D, N’D).
(iii)
Let T be analgebraic
k-scheme and X ~ T a flatmorphism
offinite
type.
Then X ~ T is aformally locally trivial family of deformations
if for every closed
point
t E T and every n >0,
in thediagram
Xn
is alocally
trivial deformation ofXl
in the Zariskitopology.
(iv)
Define afunctor J03B4,03BA,d
on thecategory
ofalgebraic
k-schemesby J03B4,03BA,d(S) := {relative
effective Cartier divisorsC P2
X S which as flat families of curves over S areformally locally
trivial at alls E S,
and whosegeometric
fibers areplane
curves ofdegree
d with
precisely
8 nodes and K cusps and no othersingulari- ties}.
Then in
[11],
pages 560-563 it is proventhat J03B4,03BA,d
isrepresentable by
analgebraic
k-schemeVS,tC,d.
REMARKS
(1.2): (i)
Note that if D EV,6,,,,d (by
this we mean that there issome closed
point
inV03B4,03BA,d corresponding
toD),
then the Zariskitangent
spaceof V03B4,03BA,d
at D may be identified withH°( D, N’D),
and ifH1(D, Ni)
= 0,
D is a smoothpoint of VS,tC,d ((1.1)(ii)).
(ii)
In order tocompute
thecohomology
groups ofN’D
we will first relate it to a certain line bundle. We therefore make thefollowing
definition
(see
also Arbarello-Cornalba[1]):
DEFINITION
(1.3):
Let S be anon-singular
irreducibleprojective
surfaceand D ~ S a reduced curve. Let
03C0’: ~ D
be the normalization mor-phism,
and if i : D - S is the inclusion map of Dinto S,
set gr = i o 03C0’:~
S. Let R be the ramification divisorof 17,
i.e. the divisorD
definedby
the zeros of the differential d 77. Then we define a sheafN’03C0 by
theexact sequence
where for a
scheme X, Tx
denotes thetangent
sheaf(the
dual of the sheaf of Kâhlerdifferentials).
REMARK
(1.4):
Note it is clear thatN’03C0
islocally free,
i.e. it is a line bundle. If we defineN03C0 by
then
N’03C0
fits into an exact sequence(see [1],
pages 23-24 fordetails).
We also note that
HO(D, N03C0)
isisomorphic
to the set of infinitesimal deformations of thepair ( D, 03C0) ([4]).
We can now state the
following
result:LEMMA
(1.5) :
LetD c S,
03C0,03C0’, N’03C0
be as in(1.3).
Then(a) 03C0’*N’03C0 ND 0 03C0’*J0
whereND
is the normal bundleof
D inS,
and J is theJacobian ideal
of
D( the first Fitting
idealof
thesheaf of
Kâhlerdifferen- tials ).
Inparticular,
there exists an exact sequencewhere T is a torsion
sheaf,
and(b) If D only
has nodes and(ordinary)
cusps assingularities,
then03C0’*N’03C0 Ni.
Inparticular, Hi(D, N’03C0) H’(D, Ni) for
i =0,1.
PROOF: We prove
(a)
and(b) together.
First note thatby
Piene[6],
page 261 we have that 03C9CO ~ 03C0’*03C9D
where 03C9, OD are thedualizing
sheaves on
D,
Drespectively,
and C is the conductor ideal(i.e.
C: =
AnnOD(03C0’*O/OD)).
Thentaking
thehighest
exterior powers of the exact sequence(1)
of(1.3)
weget
thatBut
again
from[6],
page261,
we have thatCO(-R) = JO.
Henceapplying
theprojection formula,
weget
thatNext from the exact sequence
it is clear that
ND
= J -ND.
From this the existence of the exact sequence asserted in(a)
isimmediate,
and from this exact sequence and the factthat 03C0’ is
affine,
weget
the relations about thecohomology
groups stated in(a).
Finally
if Donly
has nodes and cusps, asimple
calculation([6],
page268)
shows thatfrom which
(b)
follows.Q.E.D.
REMARKS
(1.6): (i) (1.5)
above is ageneralization
ofProposition (1.4)
in[10],
page 110.(ii)
Theproof
of(1.5)
shows thatwhere
K5
is the canonical divisor onD.
Inparticular
if we let g =g()
be the genus of
D,
thenby
Riemann-RochBy
Serreduality
we have thatLet
D
=b,
U ...ub,
where theDi
are the irreduciblecomponents
ofD,
i =
1, ..., s. (We only
assumed that D isreduced;
it may bereducible.)
Ifon each irreducible
component
ofD, Di,
we have thatthen h1(N’03C0) = 0.
Note that our above
arguments
are valid for anarbitrary
reducedcurve D on an
arbitrary non-singular projective
surface S. Wespecialize
now to the case S
= P 2,
and we suppose that D is aplane
curve ofdegree
d with
precisely 5
nodes and K cusps as itsonly singularities. By (1.5)
hi(N’03C0)
=hi(N’D).
Thenh0(N’D) - h1(N’D) is
the " virtual dimension" in thesense of B.
Segre [2]
of the irreduciblecomponent containing
D of theparameter
space((1.2)
ofplane
curves ofdegree d
with 8 nodes and Kcusps. In this case
(2) gives
the well-known classical formula(note
thatKP2 ~ -3l
where 1 is a line and " - " denotes "islinearly
equivalent to").
Finally
the sufficient condition(3)
forH1(N’D) H1(N’03C0)
to vanishreduces in this case to the famous classical criterion that for D irreduci-
ble,
if3d > K,
then the characteristic series iscomplete.
2. The
dependence
of cuspsWe are now
ready
to construct theexample
ofSegre [8]
of an unob-structed deformation space of
plane
curves with cusps but with dimen- sionstrictly greater
than the virtual dimension. We set somenotation,
that we will use
throughout
this section.Let d be an
integer >
1. Letf
be ageneral homogeneous
form ofdegree
2d in the variables x, y, z(the homogeneous
coordinatesof P2),
and let g be a
general homogeneous
form ofdegree
3d.Let Y1 c P 2
bethe curve defined
by f,
and letY2 ~ P2
be the curve definedby
g. Sincef
and g have been chosen
generally, Y, and Y2
will intersecttransversally
in6d2
distinctpoints
Pl, ... ,p6d2· Let Y c P 2 be the curve definedby
theequation f3
+g2
= 0. Then Y hasdegree 6d,
and cuspsprecisely
at thepoints
p1, ...,p6d2 but no othersingular points.
Let 03C0’:Î -
Y be the normalization ofY,
and ’11’ = 03C0’ o i where i :y _ p 2
is the inclusion map, and letN’03C0
be defined as in(1.3).
Then we have thefollowing key
result:PROOF: Blow up the
surface P2
at p1,...,p6d2 and call theresulting
surface S’. Let
e’1, ..., e’6d2
be thecorresponding exceptional
divisors. Let Ili be thepoint
of intersection of the proper transform of Y on S’ with theexceptional divisor el
for eachi=I,...,6d2.
Now blow up S’ at thepoints
ql, ... , q6d2 and call theresulting
surfaceS,
and thecorresponding exceptional
divisors el, ... , e6d2. LetPi
denote the total transformof pi
onS for
i = 1, ..., 6d2.
Then note thatPi·Pj=ei·ej= -03B4ij (03B4ij
is theKronecker
delta), and Pi·ej
= 0 forall i, j = 1,..., 6d2.
Thenletting
" - "denote "is
linearly equivalent to",
ifY
is the proper transform of Y on S(which
is of course thenormalization),
then~ 6dl-03A3l(2Pi+ei).
Fi-nally
let 1 denote a divisor on Ycorresponding
toOS(l)
0O.
Then from(1.6)(ii)
We now
break up
theproof
into severalsteps:
Step (1).
LetY
be any effective divisorlinearly equivalent
to 6dl -03A3i(Pi
+ei).
ThenPROOF: In what follows we
slightly
abuse notationby letting
C - D denotethe intersection number as well as a divisor on C
corresponding
to(9s(D)
0(9,
forC c S
an effective divisor. Then we will first show that3l+K-R ~ . Y.
ButK ~
y. Y+Y-Ks
andKS~ -3l+03A3i(Pi + el).
Asimple computation
then reduces us toshowing
thatBut this follows
immediately
from the fact that eachpoint
of theramification divisor has
multiplicity 1,
and that the intersection numberei·=ei·(-2Pi-ei)=1 for each i = 1, ..., 6d2.
Next consider the exact sequence
Then
using
the abovecomputation
and thelong
exactcohomology
sequence
applied
to(*),
we’llbe
done with theproof
ofStep (1)
once wehave
shown
thath1(OS(- + Y)) = h2((OS(- + Y )) = 0.
But note that-
+ Y ~ 03A3iPi = :
A. We use now thelong
exactcohomology
sequence associated to0 ~ OS ~ OS(A) ~ (f)A(A2)
- 0. Sinceh1(OS)
=h2(OS)
=0,
we
immediately
have thath2(OS(A)) = 0,
and we must prove thath1(OS(A))=h1(OA(A2)) = 0.
But recall that eachP;
issimply
the totaltransform on S of
pi ~ P2 (i = 1, ... , 6d2)
and as such is a reducedreducible curve of arithmetic genus 0 with two irreducible
non-singular
rational
components intersecting
in onepoint.
MoreoverPi·Pj = -03B4ij.
Therefore in order to show that
h1(OA(A2))
=0,
it isenough
tocompute
thath1(OPi(P2i)) = 0,
and this is trivial.Step (2).
Let2
be an effective divisor on Slinearly equivalent
to3dl -
03A3i(Pi
+ei) (recall that Y2 ~ P2 was
definedby
the form g ofdegree
3d).
Then we claim thath1(OS(Y))
=h1(O2(2 · Y )).
PROOF: Consider the exact sequence
Applying
thelong
exactcohomology
sequence to(**)
we mustshow
thath1(OS(-2 + Y)) = h2(OS(- 2 + Y)) = 0.
But notethat -2 +
Y - 3dl.Then the
vanishing
of these groups followseasily
from thelong
exactcohomology
sequence associated tosince
h1(OS) = h2(OS) = 0,
andh1(OS(3dl))
=h1(O3dl((3dl)2))
mayeasily
be
computed
to be0.
Step (3). (f)Y2(Y2 . Y) O2(2 · 2 dl ).
PROOF: Note that
Y-2dl~4dl-03A3(Pl+ei).
But we have that(the
intersection
number) 2 · ( Y - 2 dl )
=12d2 - 12d2
= 0 since(Pl
+el)2
=- 2 for
i = 1, ..., 6d2. Now Y2
and Y - 2 dl may be taken(in
theirrespective
linearsystems)
to beeffective divisors
without any commoncomponents
whichimplies
that(f)Y2(Y2 . (Y - 2dl)) 0
Step (4).
PROOF:
Clearly h°(tPp 2 (d - 3)) = h0(OS(d - 3)l)).
We have the sequenceand a
simple argument
as inStep (2)
shows thath1(OS(2dl)) = h2(OS(2dl))
= 0. Thereforeapplying
thelong
exactcohomology
sequence to(***)
and Serreduality,
we see thatThis
completes
theproof
ofStep (4)
andusing
theprevious
3steps obviously completes
theproof
of the theorem.Q.E.D.
PROOF: This follows
immediately
from the fact thath0(N’03C0) - h1(N’03C0) =
6d(6d
+3)/2 - 12d2 (see (1.6)(ii»
and from(2.1)
above.Q.E.D.
COROLLARY
(2.3):
LetV6d
be the irreducible componentcontaining
Yof
the parameter scheme
of plane
curvesof degree
6d withprecisely 6d2
cusps and no othersingular points ((1.1)).
Then dimV6d2 = (13d
+2)(d
+1),
and
V6d2
isnon-singular
at Y.PROOF: From
(2.2)
we see that dimV6d2 (13d
+2)(d
+1). Clearly
thedimension of the
family
ofplane
curves{C|C
is theplane
curve definedby 3
+g2
= 0where f
is ahomogeneous
form in x, y, z ofdegree 2d,
and
g
is ahomogeneous
form in x, y, z ofdegree 3d}
isFrom this
(2.3)
followsimmediately. Q.E.D.
COROLLARY
(2.4) : If d > 2,
then dimV6d2 > 6d(6d + 3)/2 - 12d2 ( the
virtual
dimension).
PROOF: In this case from
(2.1), h1(N’03C0)
> 0.Q.E.D.
3. The classical characteristic linear series
As we mentioned in the
Introduction,
in his paper[8],
page35, Segre gives
a secondexample
which he claims defines an obstructedfamily
ofintegral plane singular
curves withordinary
cusps and onehigher cuspidal point.
We will show inpoint
of fact thatSegre’s family
is not obstructedand will show that his error
(and apparently
the classical Italian geome- ters’ error[7,8,9])
is a sometimes incorrect identification of the character- istic linear series for such kinds of deformations.Segre
associates his characteristic linear series toH0(N’03C0)
instead ofH0(N’D) (see
also Wahl[11],
Mumford[5],
and Mumford’sappendix
toChapter
V of Zariski[12]
for discussions of the characteristic linear series for
curves).
In the case offormally locally
trivial deformations ofplane
curves whoseonly singular-
ities are nodes and cusps, we have shown in
(1.6)
thatHi(N’03C0) Hi(N’D),
i =
0, 1,
so in this case there is noproblem.
But for theformally locally
trivial deformations of
higher
ordersingularities
one nolonger
has suchan identification.
We now
completely analyze
theSegre example
from a modernpoint
of view. Let g be a
homogeneous
form in x, y, z ofdegree
3d such thatthe
curve Y2 c P 2
definedby
g has a node at somepoint
p and no othersingularities.
We will assume(as
is done in[8],
page35)
that d > 2.Let f
be a
homogeneous
form in x, y, z ofdegree
2 d such that the curveYl ~ P2
definedby f
isnon-singular
and passesthrough
p so that thecurve
Y, U Y2
has anordinary triple point (i.e.
with distincttangents)
atp. Let Y be defined
by f3 + g2
= 0. Then Y has6d2 -
2ordinary
cusps(defined by
thepoints
of intersectionof Y1 and Y2
outsideof p)
and acuspidal triple point analytically isomorphic to y 3 + x 4 at p. (To
seethis,
note that if we
represent Y2 locally
aroundp as x2 + y2 = 0,
andY,
asy =
0,
weget
thatlocally around p,
Y isisomorphic to (x2+y2)2+y3=0.
One can now either make a rather
long
messy calculation that(x2 + y2)2 + y 3
isanalytically equivalent to y 3
+x4,
or asmercifully pointed
out tous
by
G. Barthel and C. Gibson one can use the results of Arnold[2],
page
33.)
DefineN;
as before. Then:THEOREM
(3.1): h1(N’03C0) = (d - 1)(d - 2)/2.
PROOF: The
proof
is almost identical to that of(2.1)
sowe just
sketch thesteps.
Blowup P2
at po : = p, p1,..., p6d2-2 and denote theresulting
surface
by
S". Lete"i
be thecorresponding exceptional
divisors( i =
0, ..., 6d2-2),
andlet q;
be thepoint
of intersection ofe"l
with theproper transform of Y on S" for each i. Next blow up S" at the
points
qo, ql, ... , q6d2-2 and denote the
resulting
surfaceby
S’ and the excep- tional curvecorresponding
to qoby
e’. Blow up S" at thepoint
ofintersection of the proper transform of Y on S" with
e’,
and call this(final)
blown up surface S and theresulting exceptional
vivisor e.Let P,
be the total transform of Pi on
S,
andsimilarly Q,
the total transform of q, on S for each i =0,..., 6d2 -
2. Note thatfor all
i, j
=0,..., 6d2 -
2. The proper transform of Y onS, (which
isof course the
normalization),
islinearly equivalent
to the divisorwhere 1 is the total transform of a line
in P2.
Let l denote a divisor oncorresponding
toOS(l)
~O. Then j ust
as in(2.1)
we have :Step (1).
Let Y be any effective divisorlinearly equivalent
to 6dl -(2Po + Q0
+e) - 03A36d2-2i=1(Pi
+Qi).
Thenh1(O(3l+K - R)) =
h1(OS(Y)).
PROOF:
Again
we show that3l + K - R ~ y. Y.
We note thatKs - -
31+ 03A36d2-2i=0(Pi+Qi)+e,
and thenusing
theadjunction formula,
we arereduced to
showing
thatNote that the
point
in R whoseimage is p
hasmultiplicity 2,
while theother ramification
points
havemultiplicity
1. But we have that(the intersection numbers) ·(Q0+e)=-(Q0+e)2=2, and ·Qi=1
fori=1,...,6d2-2.
N ext following
theargument
ofStep (1)
of(2.1)
we see that if we set- + Y~03A3Pl=:A,
we must show thath1(OA(A2))=0.
Butagain
as in
(2.1)
this is trivial(note
in this casePo
is areduced,
reducible curveof arithmetic genus 0 with three irreducible
non-singular
rational compo- nents, whilePi,... P6d2-2
have the samedescription
as in(2.1)).
Step (2).
Let Y’ be an effective divisor on Slinearly equivalent
to
3dl-03A3(Pl+Ql)-e.
Then we claim thathl«(f)s(1T» =
h1(Oy,(Y’·Y)).
PROOF: Note that - Y’ +
Y~3dl-P0=:C.
Note that we may assumethat C is an irreducible smooth curve
(it
islinearly equivalent
to theproper transform of a curve of
degree
3din P2 passing through P0),
andfollowing Step (2)
of(2.1)
we must show thath1(OC(C2))
= 0. But this isimmediate.
PROOF: We have that
Y-2dl~4dl-(2P0+Q0+e)-03A3(Pl+Ql)
and it is
easily
seen that Y - 2dl islinearly equivalent
toan effective
divisor with no common
components
of Y’. Then the fact that(Y - 2dl ) -
Y’ = 0
completes
theproof.
PROOF: Identical to that of
Step (4)
of(2.1).
Thiscompletes
theproof
of(3.1). Q.E.D.
PROOF:
(i)
is immediate from(1.6)(ii), equation (2),
and(ii)
follows from(i)
and(3.1). Q.E.D.
Now on this basis
Segre ([8],
page35)
concludes that he has anexample
of an obstructed deformation ofdeficiency w
= 1(the "de- ficiency"
is the difference between the dimension of the Zariskitangent
space and actual dimension of thespace).
Indeed hisargument
runs as follows: Consider thealgebraic family
of curves(d >
2 asalways
in thissection)
V : =
{C|C
is a curve definedby 3 + 2 = 0
whereg
is a form ofdegree
3 d such that the
curve { = 0)
has a nodeand f is
a form ofdegree
2 d such that
( = 0)
passesthrough
thisnode}.
On an open subset of V we
get
afamily
ofplane
curves with6d 2 - 2
cusps and one
triple point
oftype y3 + X4.
The dimension of V caneasily
be
computed
to be(13d2 + 15d - 2). Segre
claims V is acomplete family
and indeed we will prove this(see (3.3)
and(3.5) below).
Thensince
h0(N’03C0)
>(13d2
+15d - 2)
=dim V, Segre
concludes thefamily
isobstructed
(and h0(N’03C0) -
dim V = w =1).
We will now show that this
family
is unobstructedby analyzing
thecorrect characteristic linear series. We first prove the
following:
THEOREM
(3.3):
Let r ~Y be
such that03C0’(r)
= p(the triple point of Y).
Th en
h1(N’03C0(- 4r))
=h1(N’03C0)=(d- 1)(d - 2)/2.
PROOF : The same method used in
(2.1)
and(3.1)
worksagain.
To see thiswe outline the four
steps
one last timeusing
the same notation as in theproof
of(3.1). =
Step (1).
Let Y be any effective divisorlinearly équivalent
to 6dl -4Po
-
03A3(Pi
+Qi) (which
islinearly equivalent
toY - 2 Po
+Qo
+ e inthe notation of
Step (1)
of(3.1)).
ThenPROOF:
As usual we show that3l+ K-
R - 4r - 1 . Y. But3l+K - R
-
· Y (from (3.1))
and sinceY ~ Y - 2Po
+Qo
+ e we needonly
showthat
·(-2P0+Q0+e)~ -4r (on Y )
and this is immediate.Following
theargument
ofStep (1)
of(2.1)
we mustnow
showthat
h1(OS(-+Y))=h2(OS(-+Y))=0. Since -+Y~ -P0 +
Qo
+ e this isquite
obvious. Indeedusing
the exact sequenceand the facts that
h1(OP0(Q0+e))=h2(OS(Q0+e))=0
weget
thath2(OS(-P0+Q0+e))=0. Moreover,
it is easy to see thath1(OS(Q0 + e))=h0(OS(-P0+Q0+e)=0,
andh0(OS(Q0 + e)) - h0(QP0(Q0 + e))
= 1. Therefore from the exact sequence
we have that
h1(OS(-P0
+60
+e))
= 0.Step (2). h1(OS(Y))
=h1(OY’(Y’· Y))
where Y’ is as inStep (2)
of(3.1).
PROOF: - Y’ +
Y ~
3dl -3Po
+60
+ e which isclearly linearly equiva-
lent to a reduced effective divisor C’. As before we must show that
h1(OC’((C’)2))= 0, and
this is obvious.Step (3). OY’(Y’· Y) r2y,(Y’ . 2dl ).
PROOF :
Y-2dl~4dl-4P0-03A3(Pi+Qi).
From the
representation
and the
assumption d> 2,
weget
that Y - 2dl islinearly équivalent
to aneffective divisor with no common
components
of Y’. Since Y’ . Y - 2dl =0,
we are done.Using Step (4)
of(1.3)
we cancomplete
theproof
of the theorem.Q.E.D.
COROLLARY
(3.4) : h0(N’Y)
= dim V =(13d2
+15d - 2).
Inparticular, V
is
non-singular at
Y( i . e.
thedeformations
are unobstructed atY )
and thelamily V is complete.
PROOF: Recall the exact sequence
from
(1.5)(a),
where T is a torsion sheafsupported
at p. We claim that dimTp=1.
Indeed we have thatN’YJNY, and 03C0’*N’03C0(03C0’*JO)NY.
Now Piene
[6],
page268, computes
thatp (t8, t9)k[[t3, t4]],
and(03C0’*JO)p
=t8k[[t]].
Note then thatJp
consists of all formal power series of theform {a0t8 + a1t9
+03A3i0biti+11},
i.e. these power series are mis-sing
the termt10,
while(03C0’*JO)p
consists of all formal power series of the form{03A3i0biti+8}.
From this it is immediate thatdim Tp = 1.
Moreover from this
description
ofJ,
it is clear that03C0’*N’03C0(-4r)
isnaturally
contained inN’Y (recall
that03C0’(r) = p ),
and so we have an exactsequence
for some torsion sheaf
T. Applying
thelong
exactcohomology
sequence to(2),
we conclude thath1(N’03C0(-4r)) h1(N’Y),
and therefore from(3.3), h’(N’03C0) h1(N’Y).
But from the exact sequence(1)
we have thath0(N’Y) h1(N’03C0),
and so we conclude thath1(N’Y)
=hl(N,).
Thus from(1)
weget
an exact sequence
from which we see that
From this we conclude that
h0(N’Y) = dim V,
so that V is acomplete family
of curvesnon-singular
atY,
and thus the characteristic linearseries is
complete. Q.E.D.
REMARKS
(3.5): (i)
There is still thequestion
ofproving
the existence of auniversal
family
ofplane
curves of 8nodes,
K cusps, and Àcuspidal points
oftype y3 + X4
as was done for nodes and cusps in[11].
We don’tdoubt that the methods of
[11]
would work in this case as well butactually
here this is unnecessary. Indeed let us use the notation of(1.1).
So
again
we have a functor H’ from thecategory
of artiniank-algebras
tosets defined
by
H’(A) := {subschemes of P3xSpec k Spec
A flat over Ainducing
Yon P2
which are
locally
trivial deformations of Y in the Zariskitopology. .
Then H’ is
pro-representable,
sayby
thecomplete ring
R. Butby
theabove R is
smooth,
i.e. is acomplete
power seriesring
and hence we canapply
the criterion of Artin[3]
to conclude that R isalgebraisable,
so thatthere exists a " universal"
algebraic
k-scheme Xparametrizing formally locally
trivial deformations of Y such thatX,x R
where x E X corre-sponds
to Y. Moreover it is clear that X must beisomorphic
to V in aneighborhood
ofY,
and this isenough
for our purposes.(ii)
Note that we have proven the existence of an exact sequenceMoreover one has an exact sequence
(see (1.4))
and since these are vector spaces, we may
identify H0(N’03C0)
as a subvectorspace of
HO(N,).
Now sections ofH0(N03C0) correspond
to infinitesimal deformations of thepair ( Y, 03C0).
Theargument
above then shows that there exist infinitesimal deformations of( Y, 03C0) corresponding
to sectionsof
H0(N’03C0)
which do not induceformally locally
trivial deformations of Y. But of course in no way does thisimply
that such deformations of Yare obstructed.
References
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Helvetici 56 (1981) 1-38.
[2] V.I. ARNOLD: Normal forms of functions in neighborhoods of degenerate critical points. Russian Math. Surveys 29 (1974) 10-50.
[3] M. ARTIN: Algebraization of formal moduli. Global Analysis (papers in honor of K.
Kodaira; edited by D. Spencer and S. Iyanaga), University of Tokyo Press, 21-71
(1969).
[4] E. HORIKAWA: On deformations of holomorphic maps I. J. Math. Soc. Japan 25 (1978)
372-396.
[5] D. MUMFORD: Lectures on Curves on an Algebraic Surface. Princeton University Press, Princeton, N.J. (1966).
[6] R. PIENE: Polar classes of singular varieties. Ann. Scient. Ec. Norm. Sup. Ser. 4 Vol. II
(1978) 247-276.
[7] B. SEGRE: Dei sistemi lineari tangenti ad un qualunque sistema di forme. Atti Acad.
naz. Lincei Rendiconti serie 5 Vol. 33 (1924) 182-185.
[8] B. SEGRE: Esistenza e dimensione di sistemi continui di curve piane algebriche con dati
caraterri. Atti Acad. naz. Lincei Rendiconti serie 6 Vol. 10 (1929) 31-38.
[9] F. SEVERI: Osservazioni sui sistemi continui di curve appartenenti ad una superficie algebrica. Atti Acad. Sci. Torino Vol. 39 (1904) 376-392.
[10] A. TANNENBAUM. Families of algebraic curves with nodes. Conip. Math. 41 (1980)
107-126.
[11] J. WAHL: Deformations of plane curves with nodes and cusps. Amer. J. Math. 96 (1974) 529-577.
[12] O. ZARISKI: Algebraic Surfaces. 2nd supplemented edition, Springer, Berlin/New York (1971).
(Oblatum 15-11-1982)
Department of Theoretical Mathematics The Weizmann Institute of Science Rehovot 76100
Israel
Department of Mathematics 201 Walker Hall
University of Florida Gainesville, FL 32611 U.S.A.