C OMPOSITIO M ATHEMATICA
A. I ARROBINO
J. E MSALEM
Some zero-dimensional generic singularities ; finite algebras having small tangent space
Compositio Mathematica, tome 36, n
o2 (1978), p. 145-188
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145
SOME ZERO-DIMENSIONAL GENERIC
SINGULARITIES;
FINITE ALGEBRAS HAVING SMALL TANGENT SPACE
A. Iarrobino* and J. Emsalem
August,
1976 ParisSummary
We exhibit Artin local
algebras A, quotients
A =R/I
of the power seriesring
R =k[[xl, ..., xr]], having
very small tangent sp,aceHom(I, A),
and hencehaving
as flat deformations(nearby algebras) only
otheralgebras
of the same type, and same kind.Here, by
the type ofA,
we mean the sequence ofintegers
T =to,..., tj,
... where ti =dimk Ai,
the size of the ithhomogeneous piece
of the associatedgraded algebra
A* of A: the type isjust
the Hilbert function orcharacteristic function of A with respect to its maximal ideal. We would like to leave the notion "same kind" vague, to stimulate the
imagination
of thereader,
but for the second half of the paper, itmeans "Gorenstein
algebra".
We
study
also thefamily
of those zero-dimensional Gorensteinalgebras, quotients
ofR, having
a certain maximal typeT,
and show thefamily
is an irreduciblevariety
of which weparametrize
an open dense subset. We show that for some typesT,
these Gorensteinalgebras have,
ingeneral,
no deformations tok[x]1/xn;
for some Tthey
have ingeneral,
no deformations to the trivialalgebra
k
~ ... EB k;
and we indicatewhy
for certainT,
thesealgebras ought
to have déformations
only
to other Gorensteinalgebras
of the same type.When k = C or R, the nontrivializable
algebras correspond
to stablemaps germs
F: (C ", 0) - (C ’, 0), (or (R ", 0)- (R m, 0))
where the localalgebra
A of F is finite oflength
n, but wherenearby
map-germsFt
must have less than n
points
inFt’(0):
there are less than n-sheetsover a
neighborhood
of 0 inCm,
in all map-germsFt
close to F.* Supported 1975-76 by C.N.R.S. exchange fellowship in France.
Sijthoff Publishers-Alphen Rijn
Printed in the Netherlands
Table of Contents
1. Def orming Artin local algebras - introduction 146
1.1. Three problems and three viewpoints 147
1.2. Examples of "generic" Artin algebras 150
1.3. Overview 152
2. Graded algebras with small tangent space 154 2.1. Conditions satisfied by the degree -1 tangents 155 2.2. Example of a length 8 algebra having as deformations only other algebras
of the same type 158
2.3. Ideals generated by vector spaces of degree j forms 161 3. Gorenstein algebras with small tangent space 164 3.1. Gorenstein algebras of type T = 1, r, r, 1 166 3.2. A Gorenstein algebra of type T = 1, 4, 4, 1 having deformations only to
other Gorenstein algebras of the same type 168 3.3. Parametrizing Gorenstein algebras of symmetric, maximal types 171 1 3.4. Some Gorenstein algebras that should be generic - presentation and
tangent space of Gorenstein algebras having symmetric maximal type 179
Appendix: Comparison of two parametrizations of finite length semi-local al-
gebras 182
1.
Deforming
Artin localalgebras -
IntroductionWe suppose R =
k[[xl,. - -, xr]]
is thering
of powerseries,
R’ =k[xl,.
...,Xrl
is thepolynomial ring
in rvariables,
and that thealgebra
A =
R/I
=R’/I’
where(x1,..., x,) D
I’ ~(x1,..., x,)’
is an Artin localalgebra
oflength
n. We can think of A as the localring
of a finite map germ, as analgebra,
or as thering
of a thickpoint - a singular (when
n >
1)
zero-dimensional subschemeSpec
A concentrated at theorigin
of affine r-space
Spec
R’.In §1.1
wegive equivalent topological, algebraic,
andgeometric viewpoints
on the threeproblems,
whether there exist flat defor- mations of A tok (B - - - EB k,
tok[x]lx",
and toalgebras
oftype-kind
different from that of A. We also
give
a shorthistory
of theproblem.
The type of the
algebra
A is the sequence ofintegers
T =to, ..., t;,
...where ti
=dimk Ai,
the size of the ithhomogeneous piece
of theassociated
graded algebra
A* of A: the type isjust
the Hilbert function or characteristic function of A with respect to its maximal ideal.In §1.2
we sketch our method forshowing
type1, 4, 3, 0 algebras
have in
general
no déformations to anyalgebras
of différent type than A(and
inparticular
none tok[x]lxn
nor tok~ ... (B k);
and wesurvey the results of the paper. Then
in §1.3
wegive
an overviewcomparing
the situation in deformation Artinalgebras
to that knownfor
deforming
Liealgebras,
and we introduce the sectionsfollowing.
1.1. Three
problems
and threeviewpoints
We
give
three almostequivalent viewpoints
on the 3problems
ofdeforming
the finite localalgebra
A oflength n
tok ~ ... EB k (n copies),
tok[xllx",
and toalgebras
of kind or type different than A.Thus, questions 2a,
3a areequivalent,
and when k = R or C, theanswer
"yes"
toquestion
laimplies "yes"
toquestions 2a,
3a. For amore detailed
discussion,
see theAppendix.
1.
Topological
la. There are
nearby
germs with n sheets.Suppose
k = C or R andA is the local
algebra
at theorigin
of the finite stable map germF: (C"’,O)--->(im,O)
or(R",O)~(R’,O).
Are there small deformations of F toFi
such that forUE
a smallenough
ball around0,
there is a ballB8
around 0 inR’ or Cl such
that for t EBs,
theequation Fi
= 0has n distinct solutions in
U,,? Equivalently,
are there map germs near Fhaving n
sheets over a well-chosenneighborhood
of 0 in Cm?(Of
course, there are many stable map
germs F having
A as localalgebra;
we assume one such F has been
chosen.)
lb.
Aligning.
Are there small deformations of F toFt
such that there is onesolution pt
=Fr-1(0)
toFt
= 0 inU,,,
and such that the localalgebra of Ft
at p isisomorphic
tok[x]lxn?
Ic. The type
of
Achanges along
theflat
locus. Are there small déformations of F toFt
such that there is EITHER more than onesolution to
Ft
= 0 inU,,,
but the sum of thelengths
of the localalgebras of Ft
at these solutions remains n, OR there isonly
onesolution pt
toFt
= 0 inU,
the localalgebra
A’ of F at pi haslength
n,but the type or kind of A’ is different from that of A?
The statement la is
purely topological;
we don’t know if the statements lb or lc are.2.
Algebraic
2a. Trivialization. Does the
algebra
A have a flat deformation tok ~ ... EB
k? Here we mean a déformation of the structure constantsgiving
themultiplication
in A.2b.
Deformation
to thesimplest
Artinalgebra.
Does thealgebra
Ahave a
deformation
tok[x]lxn?
2c. The
algebra
is notalmost-generic.
Does A have EITHER adéformation to an
algebra
A’ that is notlocal,
OR a déformation to alocal
algebra
of type or kind different from that of A?3. Geometric
3a.
Smoothing.
Is there a flat deformation of the thickpoint Spec A
in affine r-space Ar to a smooth subschemeSpec At
orAr?
For t~
0, Spec At
would consist of n distinctpoints, p 1(t),
...,pn(t)
each of
multiplicity
one, and thealgebra A,
=(R’/IIm p,t))
where mpi(t) is the maximal ideal ofPie t)
in R’.3b.
Aligning.
Is there a deformation ofSpec
A toSpec
A’=Spec(R’/(xi,
..., xr-i,xr))? (The
thickpoint Spec
A’ consists of theorigin
0 of Ar r with an infinitesimaltangent
line of order n in thexr-direction.
When a functionf
of R’ is evaluated atSpec A’,
one obtains its value and that of its first n - 1partial
derivatives inthe xr direction,
at theorigin.)
3c. The thick
point
is notalmost-generic.
Is there EITHER a defor- mation ofSpec
A to a subscheme of Ar not concentrated at asingle point,
or to a subscheme of different type at0,
OR déformations to at least two differentgeneric
subschemesof Ar? (An almost-generic
thick
point Spec
A will have deformationsonly
to other thickpoints
of the same type, and the
point
zparametrizing Spec
A will lie on asingle
component of the Hilbert scheme Hilb"Ar.)
Notice that the
algebra k[x]/xn
has the deformationk[x]/(xn - t)
which isisomorphic
tok E9 ... E9 k
when t #-0,
since then xn - t has n distinct roots. We do not know whetherconversely
the localalgebra
A
being
trivializableimplies
it has a deformation tok[x]lxn"
Thus ananswer
"yes"
toquestions 1b, 2b,
3bimplies "yes"
toquestions la, 2a, 3a, respectively.
Our
viewpoint
isgeometric.
Theproblem
ofdeforming
zerodimensional
singular
subschemes of Ar isinteresting
for two reasons:i. There is a rumor that the
problem
ofdeforming
s-dimensional schemesY’
in X r is related to that ofdeforming
zero-dimensional schemes in an(r - s)
dimensionalvariety:
it isembedding
codimen-sion that indicates the
difficulty.
Work ofSchaps concerning
theCohen-Macaulay
subschemes of codimension2,
theexample
of Mumford of an irreducible reduced curve inP4 having
nononsingular deformation;
and when X r isregular local,
the result of Buchsbaum-’ (Added in proof) Kleppe [27] shows the converse is false: he shows every 3-generator Gorenstein algebra is trivializable; but Theorem 3.35 shows not all these have a
deformation to k[x]/x".
Eisenbud
concerning
the Pfafnan structure ofheight
3 Gorensteinideals,
bear out the rumor.ii. There is a scheme
Hilb" A,,
rparametrizing
thelength n
zero- dimensional subschemes of Air. We use the tangent spaceHom(I, A)
to the
point
z in Hilbn Ar rparametrizing
the subschemeSpec
A =Spec R’Il’,
tostudy
the deformations of A.We now
give
a short account ofprevious
work. For2-generator algebras,
Hartshorne(unpublished),
thenFogarty (1968) [8], Schaps (1970) [21], Briançon-Galligo (1972) [2],
and Laksov(1975) [17]
allgave various
explicit
déformations of A tok ® · · · ® k. Briançon
then showed in 1972
(see thèse, 1976) [1],
that2-generator
localalgebras
A have deformations tok[x]/xn,
when k isalgebraically
closed. J.
Briançon
and J. Damon remark that work of Levine- Eisenbud shows thetopological degree
of themapping, R 2--> R2 given by (xy, x2a _ y2b)
has absolute value2;
and thedegree
of themapping (y, x2a+2b)
is0; hence R[x, y]1(xy, x2a - y 2b )
has no deformation toR[X]I(X2a+2b ). Damon-Galligo
used the trivialization result in 1975 to show that the type of a2-generator algebra
A is aC°
invariant for aC°° stable map germ F
having
discretealgebra type
of which A is the localalgebra. (See
also(Damon [2]
and[4])
where these results areextended.)
For r-generator
algebras, Damon-Galligo
have exhibited certainalgebras
A =RII
where I is a tower-likeideal, having
trivializations(1975).
On the otherhand,
in 1972 larrobino exhibited a nontrivializ- able localalgebra:
theargument
was that the dimension of a certainfamily
ofalgebras (computed
via Hilb"Ar)
islarger
than the dimen- sion rn of the open set U in Hilbn Arparametrizing
trivialalgebras.
For
comparison here,
we summarize thatexample:
suppose r - 3 and consider thefamily
ofalgebras (Av
=R/(V, mj+1)}
where V is a vectorspace of
degree j
formshaving
size dim V =#Rjl2,
half the size ofthe space of all
degree j
forms in R.(We
will usethroughout #S to
denote the vector space dimension of S over
k.)
The dimension of thefamily {Ay} (the
number ofparameters)
is dimGrass(#Rj/2, #Rj) = (#Rjl2)2- = C(jr- 1)2
. Thelength n
of eachalgebra Av
is n =(#Ro + ...
+#Rj-l
+#R;/2)= c’ j r.
Thus the dimension of thefamily
is(C"n2-2/r)
>(rn)
when n > 3 and n islarge;
hence thegeneral algebra
of thefamily
cannot be trivializable since the dimension of Uparametrizing
sets of n distinctpoints in A, is only
m. The existence of such nontrivializablealgebras
with 3 generators alsoimplies
theexistence of
"generic"
localalgebras
with3-generators,
for which theanswer to
questions lc, 2c,
3c is "no": the subschemeparametrized
by
ageneric point
z of acomponent
of Hilbn As r other thanÜ
is afamily
of sets of thickpoints
andpoints;
thealgebra
Acorresponding
to one of the thick
points
will be"generic"
and local(an "elementary component"
of Hilb" Ar in thelanguage
of[14]). However,
till now, there were nospecific examples
known of such "almostgeneric"
orgeneric algebras.
1.2.
Examples
of"generic"
Artinalgebras
We here
give
twospecific examples
of such"generic" algebras - in lengths
8 and10,
and for r =4;
and weindicate, identify,
many more such components, up to a verification of theindependence
of certainlinear conditions that we describe. The
only
method we’ve so far found toverify
theindependence
of the linear conditions is to calculatethem,
and we verified the twosimplest examples (where
onemight
expect the conditions to be mostdegenerate).
Our method is tobound the size of the tangent space
Hom(I, A)
to Hilb" Air at apoint
zof Hilb" Ar
parametrizing
a localgraded Argin algebra
A =R/I;
weshow that for certain types of
algebras
A the tangent space is so small that theonly
deformations of A are otheralgebras
of the sametype.
The two
explicit examples
are1.
Algebras
of type1, 4, 3, 0 generated by
7general enough quadratic
forms in 4 variables.2. Gorenstein
algebras
of type1, 4, 4, 1 generated by
6polynomials
of order 2 in 4 variables.
Precisely speaking,
ageneric algebra B
of type1, 4, 3,
0 is B =k[x,y,z,w](Jaijl)l(gl,...,97),
where(a;j) 1 S 1 S 7, 1 S j S 3)
are 21 variables and gi = ui +ailz2
+ ai2ZW +ai3w2,
with U¡,..., U7= x2,
xy, xz, xw,y2,
yz, ywrespectively.
We prove any deformation B’ of B has in turn B as adeformation;
and B isparametrized by
ageneric point
ofa
component
Z of the Hilbert scheme Hilb" A4parametrizing length
8 zero-dimensionalsubschemes,
of affine4-space;
the component Zparametrizes only
"thickpoints" -
or in otherwords, singular length
8subschemes concentrated at some
point
of A4. ThusSpec
B is a"generic"
0-dimensionalsingular
subscheme of A4. An almostgeneric algebra A
oftype (1, 4, 3, 0)
is for us aquotient
A =k(x,
y, z,w)/I
"close to" a
generic algebra,
in the sense A has deformationsonly
toother
algebras
of the same type and kind. Thepoint parametrizing
Alies on a
single
component Z of Hilb" Ar, and an open subset of Zparametrizes only
"thickpoints"
of the same type asA;
the coefficients of(fI,
...,f7) defining
I are in k. Ageneric point
of thecomponent
Zparametrizes
ageneric algebra B
of type(1, 4, 3, 0),
which is a deformation of A. We will use these words henceforth somewhatloosely;
inparticular
we’llemploy "generic"
with quotes tomean almost
generic.
These
examples
are notrigid,
since there are moduli for theisomorphism
classes of thesealgebras;
we do not know if there existrigid
finite Artinalgebras.
Our methoddepends heavily
on a naturalgradation
of the tangent spaceHom(I, A)
when I isgraded,
describedand used
by
M.Schlessinger
in(Schlessinger,
1973[23]).
We believethat this
dependence
of oursimple
method on thisgraded
structure iswhat prevents our detection
by
it of"generic" algebras
in 3variables, (which
arecertainly
nothomogeneous,
and which willrequire
asomewhat finer
method). However,
there is evidence that over a closedfield,
8 is verylikely
the smallestcolength
in which such"generic"
localalgebras
exist:algebras
oflength
no more than 5 havetrivializations; algebras
oflength
6 and most types do(it
remains to check thetype 1, 3, 1, 1); algebras
oflength
7 and types1, 4, 2
or1, 3,
3(the types
where there are moduli ofisomorphism classes)
alsohave trivializations
(see [7]).
Our argument
proving genericity
for the1, 4, 3, 0 algebras
issimple:
suppose I is an ideal
generated by
7quadratic
forms inR,
and that E - F - 1 - 0 is thebeginning
of a free resolution for Iover R ;
then there aregraded
mapsHom(I, A) -
HomF,
A---->
HomE,
A such thatHom(I, A)
is the kernel of 0. The zeropart Homo(I, A)
of the tangentscorrespond
tochoosing
aslightly
different set of 7quadratic forms;
thepositive part
is0;
we showusing
the sequence that if I issufficiently general, Hom-,(I, A)
is4-dimensional, just large enough
for the trivial tangents
corresponding
to the 4independent partial derivatives;
we prove ageneral
lemmashowing
that then alsoHom_2(I, A) =
0. It follows that for linear(tangent)
reasonsonly,
thering
A has deformationsonly
to otherrings
of the sametype.
Thering
A =
R/I,
with I =(f,, ... , f7) = (x2
+z2,
xy +w2,
xw, xz + wz,Y2
+z2,
yw, yz +
W2)
isgeneral enough
to "work" here. We thengeneralize,
but show
something weaker;
if I is the idealgenerated by d
forms ofdegree j
in rvariables,
whered, j
and r are chosenproperly,
then(diMk(Hom-,(E, A))
+r)
>dim(Hom_1(F, A)) :
there areenough conditions, if independent,
to ensure thering
A has deformationsonly
to other
rings
of the sametype.
Our argument for the Gorenstein
1, 4, 4,
1algebras
is similar. Webegin
with agraded 1, 4, 4, 1
Gorensteinalgebra A== RII;
we showthat the zero part
Homo(I, A) corresponds
tochoosing
aslightly
different
graded
Gorensteinalgebra;
thepositive part Homi(I, A)
corresponds
tochoosing
anon-graded
Gorensteinalgebra
A’having
Aas associated
graded algebra,
and we show that if 7 isgeneral enough,
the
negative
partHom-,(I, A)
consistsonly
of the trivial tangents. Thegraded
Gorensteinalgebra
A =R/I,
with I =(fi,..., f6)
=(yz - X2- W2, xz - y2- W2, wz - x2- y2, yw - 2x2 - z2,
xw -2y2 - Z2, xy - 2W2 - Z2)
isgeneral enough
to work here:thus,
it has as def or- mationsonly
other Gorensteinalgebras (not necessarily graded)
ofthe same
type 1, 4, 4, 1.
We then
generalize,
asbefore,
to thelargest
Gorensteinalgebras having symmetric type T,
socle ofdegree j
and r generators.First,
weshow the
family
Gor T C Hilbn R of suchalgebras
isirreducible,
andgenerically rational,
of a dimension we calculate.(Theorem 3.34.)
Toprove
this,
we show the open subset’TT-1(G
GorT) parametrizing
those
algebras quotients
of R whose associatedgraded algebra
isGorenstein,
is in fact alocally
trivial fibration ’TT:’TT -1 G
Gor T--->G Gor T with fibre an affine space, over G Gor
T, parametrizing
thegraded
Gorensteinalgebras
of type T(Lemmas
3.3A and3.3B).
Thevariety
G Gor T is itself an open set in theprojective
spaceP(Rj) (Theorem 3.31).
The dimension calculation shows that for r > 8 and allj,
or for r>4and j>9,
thegeneral
Gorensteinalgebra
of type T isnot smoothable.
(Theorem 3.35.)
We then in section 3.4 extend the argument of section2,
and indicate for which types onemight
expectto prove
genericity using
the method of small tangent spaces.1.3. Overview
Our work shows that there is a
similarity
in the structure ofSLalg(k") parametrizing
semilocal commutativealgebras,
and thestructure of
Lie(kn) parametrizing
Liealgebras
oflength
n, as sum- marized forexample
in the thèse ofMonique Levy-Nahas:
different"kinds" of
algebras
determine thegeneric points
of components of theparameter variety. (See Monique Levy-Nahas [18],
M.Vergne [25].)
It’sjust
a matter offinding
theright
"kinds" toaccurately
describe thecomponents. Perhaps
this search will suggest new ways ofdivying
up the finite commutativealgebras,
into kinds other than"type T",
or "Gorenstein oftype
T". Our work also indicates that there are twoelementary components
ofHilbl°
As, hence that the number ofcomponents
of Hilb" As growsexponentially
with n.(See [14].)
We should like to thank B.
Teissier,
B.Bennett,
M.Schlessinger,
D.
Trotman,
and J. Mather for discussions and encouragement, D.Laksov for a critical
reading,
M.Levy-N ahas
forinspiration through
herresults on Lie
algebras,
andpeople
of theLê-A’Campo
seminar for whom weprepared
a first version. The first author wassupported by
a CNRSexchange fellowship
in Franceduring
this work.We now outline the sections. In section 2.1 we
give
our mainargument
on smallness of the tangent space for the case A =R/I,
where I is
generated by
the elements of a d-dimensional vector space ofquadratic
forms. We then calculate thepairs (d, r)
where theargument
should work. Wegive
theexample
in section 2.2 - a cal- culation of theindependence
of the 24 conditions in 28 unknownsarising
in thesimplest
case ofalgebras
oftype 1, 4, 3, 0.
In section 2.3we
generalize
the discussion of§2.1
to vector spaces ofdegree j forms,
when r islarge compared
toj.
We also show that ifHom-i(7, A)
has dimension r, and I isgeneral enough,
then all thenegative part Hom_(I, A)
vanishes(Lemma 2.31).
In section 3.1 we
give
ourargument
for the Gorensteinalgebras
oftype 1, r, r, 1
when r>4. In section 3.2 wegive
the calculation ofindependence
in thesimplest algebra
we found that works for r = 4.Verifying
theexample
involvesfinding
the somewhatcomplicated
relations between the 6 generators of a
graded
type1, 4, 4,
1 Goren- stein idealI,
thenshowing
thenonsingularity
of theappropriate
20 x 20 matrix: the
key
is to choose an ideal Isymmetric enough
sothat the relations can be
hand-calculated,
butgeneral enough
so thatthe conditions we use are
independent.
Then in section 3.3 we discussthe Gorenstein ideals of thin
symmetric type T, showing
their exis-tence
(Theorem 3.31), parametrizing
them(Lemmas
3.33A and3.33B,
Theorem3.34),
andshowing
theirnonsmoothability
forlarge
r(Theorem 3.35).
We then in section 3.4study
theirtangent
space,comparing
the sizes ofHom(F, A)
andHom(E, A)
in Theorem 3.36.In these more
complicated algebras,
we need to use more of thepresentation,
to estimate thetangent
space. Section 3.4 isconjectural, depending
on anassumption concerning
thepresentation
of thegeneral
Gorensteinalgebra
oftype
T.Finally,
in anappendix,
wegive
the relation between dimAlg
T and dim HilbT,
the dimensions of theparametrizations by
structureconstants and
by
theGrassmanian,
of Artin localalgebras
of type T.We do this
mainly
toclarify
the relation between these twoparametrizations.
Oneapplication
of theappendix
is that the knownbounds on dim
Hilb" A,
r(See [14]), [12])
determine bounds ondim
SLalg,(kn).
2. Graded
algebras
with smalltangent
spaceWe consider
rings
A =R/I
where I is the idealgenerated by
asufficiently general
d-dimensional vector space V ofquadratic
formsin the power series
ring
R =k[[xl, ..., xr]]
of dimension r > 2. Wegive
aplan
of argumentshowing
that if d is well chosen for r, theserings
A have norigid
deformation(and
inparticular they
have nosmooth
deformation).
Theonly
deformation of suchrings A,
in cases where the argument can be carried out, will bealgebras
A’ =R/I’
where I’ is
generated by
another d-dimensional vector space ofquadratic
forms in R. If E --> F --> I ~ 0 is thebeginning
of a minimalfree resolution of I
over R,
we mayassign degrees
to the basiselements of F and E such that the maps have
degree
0. We also cangrade Hom(F, A), Hom(E, A),
andHom(I, A):
we say t EHoms(F, A)
if
degree t(f) = degree f + s
whenf
is"homogeneous".
Then0:
Hom(F, A) ---> Hom(E, A)
is agraded
map with kernelHom(I,A),
and the first order deformationsT’(A)
arejust Hom(I, A)/A(a/axl, ..., al ax,).
The argument issimply
that if V is nottoo
special
the linear conditions0(t) = 0 determining
thedegree -1
partT’-,(A)
of the first orderdeformations, ought
to be irredundant.If so, and if the dimension d of V is well
chosen,
the -1 part ofHom(I, A)
containsonly
the trivial tangents, the -2 andpositive
partsvanish,
and thedegree
0 part comes from deformations of the generators of I to other generators of the samedegree. Hom(I, A)
is the tangent space to thepoint
zparametrizing
I on the Hilbertscheme
parametrizing
ideals ink[xi,...,xr];
we canexplicitly
describe there all the deformations
producing degree
0 elements ofHom(I, A)
orproducing
the trivialdegree -1 elements;
and there isno room in the tangent space for extra deformations. Thus the
algebra
A will be
"generic".
Thequotients
of R that are deformations ofA,
will be describedby
an open U in the GrassmannianGrass(d, R2) parametrizing
all d-dimensional V inR2.
Thecomponent
ofHilb" A,,
rincluding
apoint
zparametrizing A,
will contain the open set U x Ar, and will be smooth and reduced at itsgeneric point.
Of the coor-dinates in
U,
there are(r2 - 1)
parameters ofPgl(r - 1) acting
onGrass(d, R2),
and the rest(d(cod V) - (r2 - 1»
are the moduli ofisomorphism
classes ofalgebras
A’ of the same type near A. The closure U x Ar in Hilb" Pur will be anexample
of anelementary
component of Hilb" Pr - oneparametrizing only
irreducible 0-dimen- sional subschemes of Pr r(see [13]). (Here
thecolength n
is 1 + r +cod
V.)
The dimensions d that workought
to be all those betweenabout 3
the size ofR2 (13
the dimension of the space ofquadratic
forms),
and(#R2 - 3). However,
we have not found thekey,
theproof
that the linear conditions
0(t)
= 0 that we find areusually irredundant,
save in the
simplest
case T =1, 4, 3, 0.
So at the moment the method ismainly
ascouting
tool forfinding elementary components
of Hilb" Pr.Any particular
values of interest can beput
into a computer and checked. The number of conditions is aboutrd,
which ranges from aboutr3/6
to(r3/2
+r2/2).
In section 2.1 we
give
in more detail thegeneral argument
and describe which d shouldwork;
in section 2.2 weverify
that it worksin the
simplest case - giving
acolength
8elementary "generic singularity",
thequotient
ofk[[x,
y, z,w]] by
the idealgenerated by
7general quadratic
forms. To prove theexample,
wesimply
solve the24x24 system of linear conditions
defining T ’-,(A)
when I =(fI, ..., f7) = (x2 + Z2,
xy +w2,
xw, xz + wz,Y2
+z2,
yw, yz +w2).
Insection 2.3 we comment on
higher degree
extensions of the sameintuition.
2.1. C onditions satisfied
by
thedegree
-1tangents
We view A =
R/I
as thering
of the subscheme X =Spec A
concentrated at the
origin
0 of Ar =Spec k[xl,..., xr] ;
the affine space Ar is embedded in Pr; Hilb" Pr = Hparametrizes
thelength n
dimen- sion 0 subschemes of Pur. If z e Hilb" Pr rparametrizes X,
thenNX
=Hom(I, A)
is the tangent space to H at z; theisomorphism
classes ofthe first order deformations
Tlx = T1(A)
is definedby
the exactsequence
The
map 0
takes the vectorfield X
= Efi alaxi
to~X
which mapsf
E Ito the class
of 1 fi alaxi mod I;
theimage
is the trivial first orderdeformations, arising
from the Hilbert scheme Hby merely changing
the
point
in Pr r where thesingularity
is defined from theorigin
to anearby point
in Pr, andacting by
an element of Aut R. All thedegree
0tangents - mapping
thegenerators
of I toA2 = R2/ V -
occurby changing
V =(fI,
...,fd)
to anearby
vector space V’ =(fi,
...,fd)
inR2;
there are no nonzeropositive degree
tangents,provided I ~ m 3 (which
will hold in ourexamples);
if we can showHom-,(I, A)
isjust
the trivial tangents and
Hom_2(I, A)
=0,
then the Hilbert scheme Hnear z is
just
U x Ar, with U an open in the Grassmannian G.Suppose
I isgraded
and the sequence E ---> F ---> I ---> 0begins
aminimal
graded
free resolution ofI,
and thatEo
denotes the sub- module of trivialrelations;
then there is an exact sequenceThe
degree -1
tangents, those inHom-1(I, A)
arise fromHom(F, AI)
whereAl
1=R is
the linear part of A. Ourgoal
is to show these lie in theimage
of0,
for V well-chosen. We count: there are rd elements ofHom(F, AI).
The relations inE/Eo
are thedegree
3 relations(L BiFi == 0
withBi E RI),
and are the kernel ofmultiplication
map:(E/Eo)3
=Ker(R1 Q9 V) ~M R3.
Thus if M issurjective
Now 0 maps
(Hom F, Al)
toHom(E/Eo, A2):
If t EHom(F, Al)
takesfi to ei
EAI
and e E E’ is thedegree
3 relation 1BJi
=0,
then0(t)(e) = E Biti
EA2.
That0(t)
= 0 isequivalent
to thevanishing
of slinear conditions whose variables are the rd coefficients of t. Here
s =
#(Hom(E3, A2)
= dimE3 .
dimA, - (rd - (r32)(cod V).
We know there is at least the solution space0(alax,,..., alax,)
which is r-dimensional if V is
sufficiently general.
If V is chosengeneral enough,
the s linear conditionswill,
we expect, be asindependent
aspossible,
and weexpect
dimT’-,(A)
= dimHom-,(F, A) - (dim RI Q9
V-dimR3)(cod V) -
r(or
zero when thequantity
is nega-tive).
In other words we expectWe now
show, assuming
char k # 2LEMMA 2.1 :
If (with
the notationabove)
dim V >2,
andT ’-,(A) =
0,
then alsoT’2(A)
= 0.PROOF:
Suppose
t E ker 0:Hom(F, AO) ---> Hom(E’, A 1).
We choosethe basis
ffil
of V such thatt(fl)
=1, t(f2)
= 0. Then(X1t, ..., xrt)
CHom(F, Al)
is an r-dimensionalsubspace (the images
of
f being independent) coming
fromHom(I, A),
so must be the samesubspace
as$(ôlôxi, ..., alaxr)
sinceT’-,(A)
= 0. This wouldimply
all the
partials
are 0 onf2. :z># 0 (See
also Lemma2.31)
Wegive
here a table of solutions ofWe have shown that when d =
(#R2 - 2),
thealgebra
A =R/( V)
hassmooth
deformations,
so that value of d is omitted from the table.Table
of
Solutions toKey Inequality : h (r, d) 0,
and d #(#R2 - 2)
r = # variables d = dimension n =
colength
When r >
5,
and d satisfiesthen h
(r, d) ~
0. When r is verylarge,
the constant 2 on the left of(2.1.3)
can be reduced to
1,
then toslightly
over2.
In other
words,
we expect that if one chooses any number between about#R2/3 (see (3)
forprecise limits)
and(#R2 - 3)
ofgeneral enough quadratic
forms inR,
the ideal I in Rthey
generate has no deformations other than ideals I’similarly
formed.Of course, when
completed,
this is a first order argument: there could be more values of dyielding "generic singularities". (The skeptic
would say there could beless!) Incidentally,
thisstyle
argumentgives
noexamples
in 3 variables: at the time ofwriting, although
we know there aregeneric singularities
ofcolength
no morethan 102 in 3 variables
(probably
incolengths
muchless),
we have noexplicit examples
ofembedding
codimension 3.The line of argument
suggested
can be used to limit the size ofHom(I, A),
even when it doesn’t showT1(A)
is 0. Emsalem remarksthat in certain cases this