C OMPOSITIO M ATHEMATICA
V. B. M EHTA
W ILBERD V AN DER K ALLEN
A simultaneous Frobenius splitting for closures of conjugacy classes of nilpotent matrices
Compositio Mathematica, tome 84, n
o2 (1992), p. 211-221
<http://www.numdam.org/item?id=CM_1992__84_2_211_0>
© Foundation Compositio Mathematica, 1992, tous droits réservés.
L’accès aux archives de la revue « Compositio Mathematica » (http:
//http://www.compositio.nl/) implique l’accord avec les conditions gé- nérales d’utilisation (http://www.numdam.org/conditions). Toute utilisa- tion commerciale ou impression systématique est constitutive d’une in- fraction pénale. Toute copie ou impression de ce fichier doit conte- nir la présente mention de copyright.
Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
http://www.numdam.org/
A simultaneous Frobenius splitting for closures of conjugacy
classes of nilpotent matrices
V. B.
MEHTA1
and WILBERD VAN DERKALLEN2
ISchool of Mathematics, Tata Institute of Fundamental Research, Homi Bhabha Road, Bombay 400005, India, 2Wilberd van der Kallen, Mathematisch Instituut, Budapestlaan 6, P.O. Box 80.010, 3508 TA Utrecht, The Netherlands
Received 7 March 1991; accepted 14 October 1991
©
1. Introduction
We exhibit a nice Frobenius
splitting a
on Gx B b
where b is the Liealgebra
ofthe Borel group B of upper
triangular
matrices in thegeneral
linear group G =Gin.
What is nice aboutit,
is that it descendsalong
familiar maps andspecializes
to familiar subvarieties in a manner that is useful for thestudy
of thesingularities
of closures ofconjugacy
classes ofnilpotent
nby n
matrices. Inparticular,
we show that these closures aresimultaneously
Frobeniussplit,
arenormal,
and have rationalsingularities.
The result on rationalsingularities
isderived from a
general vanishing
theorem that will beproved
in our paper[15].
Note that
normality
hasalready
beenproved by
Donkin in[3].
His method usesa lot of
representation theory
andemploys
resolutions of the closures ofconjugacy
classes inventedby
Kraft and Procesi.An alternative
approach
to thesesingularities
has beengiven by
G.Lusztig.
In[11]
he showed that the samesingularities
occur in Schubert varieties for Kac-Moody
groups of affineWeyl
groups. Now Schubert varieties for such infinite dimensional groups are mastered in Mathieu’s book[12],
where Mathieu showsthey
are normal and have rationalsingularities.
In contrast with
this,
our work remains in finite dimensions. It relies onexplicit
formulas. Indeed the formula for oursplitting
Q isgiven by
aproduct
ofprincipal
minors and thespecialization
of thesplitting
to subvarieties is basedon an
inspection
of whathappens
to the determinants. To descend 03C3 to the Liealgebra
g ofG, (along
the natural map GBb ~
g, cf. Grothendieck’s "simulta-neous resolution"
[2]),
we use a Galois theoreticargument.
We find that above thegeneric point of g
the action of theWeyl
group on a is trivial. Aspreparation
for that
computation
we firstspell
out trivializations of the canonical bundles of Gx B b and G x T t.
The
geometry
ofconjugacy
classes is of coursesimplest
for thegeneral linear
groups. It may be of interest to
try
and extend our method to othersemisimple
groups, but there are some obstructions to this. For
instance,
for thesymplectic
group of rank 2 in characteristic 2 there is no function
analogous
to theproduct
of
principal
minors.(No
function thatyields
asplitting.)
The first author wishes to thank Shrawan Kumar for useful and
stimulating
discussions. The second author wishes to thank Steve Donkin for
pointing
outLusztig’s
paper[11]
and T. A.Springer
forshowing
theimportance
of theWeyl
group action.
2. Orientations
We will need the relation between trivializations of the canonical bundle Co on
three different spaces.
2.1. Notations
We work over an
algebraically
closed field k ofcharacteristic p,
p > 0. Let G be the group of nby n
invertiblematrices,
B itssubgroup
of uppertriangular matrices, B
= T U the usualdecomposition.
Theunipotent
radical of the Borel group B -opposite
to B we call U -. Thus U - consists ofunipotent
lowertriangular
matrices. The Liealgebra
of G is called g and is identified with the vectorspace-viewed
as avariety2013of n by n
matrices.Similarly
b is the Liealgebra of B, u -
is the Liealgebra
ofU -,
t is that of T. TheWeyl
group is W. Allthis is viewed as
being
defined over theprime
field in the usual way.2.2. Volume
forms
A nowhere
vanishing global
section of the canonical bundle on avariety
is calleda volume form.
They
existonly
if the canonical bundle is trivial and thenthey
are
unique
up toglobal
units. In ourexamples
theonly global
units areconstants. We wish to choose volume forms on the three varieties G
x ’ b,
Gx T t
and g. On g this is very easy; one
just
chooses an ordered basis of g andgets
agenerator
of thetop
exterior power039Btop g
and thus aglobal generator v[g]
ofthe canonical bundle
03C9[g].
On Gx Bb
weproceed
as follows. Apoint
p on thisvariety
may berepresented by
apair (g, X) with g
E G and X E b. Given such apair
we map thevariety
U - x b intoG Bb by
the localisomorphism 03C4g,X : (x, Y) ~ (gx, X
+Y).
We fix a volume formv[U-
xb]
of U - x b and takeits
image
in the canonical bundle of Gx ’
b toget
a local section around p of the canonical bundlecv[G Bb].
LEMMA 2.3. This
procedure defines
avolume form
on Gx B b.
Proof.
Think of the canonical bundle as avariety
and think of the desired volume form as amorphism
of varieties. We need to check that the resultspatch
when one varies
(g, X).
For this thekey
is to show that when(gl, X1)
and(g2, X2)
represent
the samepoint
p of GBb,
theresulting
localsections v1
and v2respectively
ofm[G Bb]
agree at p. Put b =g-11 g2.
ThusX1 equals Ad(b)X2.
Identify
U - in the obvious way with aneighborhood
of the’origin’ B
ofG/B.
Thus we
get
an identification of thetangent
space of U - x b at itsorigin (1, 0)
with
g/b
0 b. Consider theautomorphism
ofG/B
x bgiven by (x, Y) ~ (bxb-1, Ad(b) Y).
View it as a birationalautomorphism 03C8
of U - x b. Wehave
03C4g1,X1 03C8 =
7:g2,X2’ so weonly
need to check that thetangent
mapto 03C8
at theorigin (B, 0)
has determinant 1. This determinant is the same as the determinant ofAd(b)
restricted to b times the determinant of the map inducedby Ad(b)
ong/b,
so it issimply
the determinant ofAd(b).
Now theadjoint
action of G isby
linear transformations of determinant 1.
(Recall
that G isgenerated by
its centertogether
with its commutatorsubgroup.)
2.4. Orientation on G
x T
tThe
reasoning
is similar to the case of G x ’ b. Given(g, X) with g
E G and X E twe map the
variety
U - x U x t into Gx T t by
the localisomorphism (x,
y,Y) ~ (gxy, X
+Y).
We fix a volume formv[U-
x U xt]
of U - x U x t and take itsimage
in the canonical bundle of GTt
toget
a local section of03C9[G Bb]. Identify
thetangent
space at(1,1)
of U- x U in the obvious way with thetangent
spaceg/t
ofG/T
at its’origin’
T. Thisgives
an identification of thetangent
space of U - x U x t at itsorigin (1, 1,0)
withg/t
~ t. Theanalogue
of lemma 2.3 holds with a similar
proof
and weget
a volume formv[G x ’ t]
onG
x T t.
2.5.
Comparison of
volumeforms
There is a natural map from G
x T t to G x B b, sending
the class[(g, X)] of (g, X)
to the class
[(g, X)]
of(g, X).
There is also a natural map from Gx T t
to gsending [(g, X)]
toAd(g)X.
We wish to know whathappens
to the volume forms under these maps. Morespecifically,
thepull
back of a volume form is a function times the volume form on the source, and we care about the divisor of that function. This is an exercise incomputing
determinants. Westudy
the map from Gx T t
to g at[(g, X)] by composing
with the map fromU- U t to G Tt,
which was used for
constructing
the volume formv[G x T t].
Recall weidentify
the
tangent
space of U - x U x t at itsorigin (1, 1,0)
withg/t ED
t which in its turn may be identified with g itself. Theupshot
is that we have tocompute
the determinant of the map from g to g which sends Y + Z toAd(g)([ Y, X]
+Z)
forY ~ u- (D u and Z E t. That determinant does not
depend
on g butonly
on X.One may view it as the
product
of the rootsapplied
to X. The divisor of thefunction on G
x T
t which arises as the coefficient of the volume form is thus twice the divisor of the reducedsubvariety
G x Ttirr,
wheretirr
is thesubvariety consisting
of the elementshaving
fewer than n distincteigenvalues.
So this is theanswer when we
pull
back from g. Next let uspull
back from Gx B b.
Thedeterminant to consider is now the determinant of the
endomorphism
ofu- ~ u ~ t = u- ~ b sending (Y-, Y+, Z)
to(Y-, [Y+, X ] + Z).
Thereforenow the divisor
is just
once Gx T t;rr .
2.6. The action
of
WAn element w of the
Weyl
group acts on Gx T t through [(g, X)]
H[(gw-1, Ad(w)X)],
with aslight
abuse of notation.LEMMA 2.7. The
Weyl
group actsthrough
thesign representation
on the linearspan
of
thepull
back to Gx T t of the
volumeform of
Gx B
b.Proof:
The map from Gx T
t to g isequivariant
forW,
when W actstrivially
on g, so the
pull
back of the volume form ofg is
invariant. We have to divide thispull
backby
the functiondefining
Gx T t;rr,
on which W indeed actsthrough
thesign representation.
3. Frobenius
splittings
3.1. A
partial
orderIn order to describe our
computations,
we need tosingle
out aparticular
class ofB invariant ideals of b. To this end we
put
apartial
order on the setP = [1, n] [1, n]
which indexes the coordinates on g. We declare thatIf S is an ideal for this
partial order,
i.e. if(i,j) (r, s)
and(r, s)
E Simply (i,j)
ES,
then we define
b[S]
to be thesubspace
of bconsisting
of the matrices X withXij
= 0 for(i, j ) ~ S.
Oneeasily
sees that such asubspace
is a B invariant ideal.Let us agree to use the notation
b[S] only
when S is an ideal for thepartial
order. We will find a Frobenius
splitting
for all Gx B b[S] simultaneously.
3.2. Subdeterminants
If
M ~ g
is amatrix,
let us indicateby
a notation likeMr,s
the submatrixconsisting
of the entries whose row number is at most r and whose columnnumber is at least s.
LEMMA 3.3.
Let g be a unipotent
lowertriangular
matrix and let M E g be such thatMr,n-r = 0 for
someinteger
r between 1 and n. Then3.4. The choice
of
uWe choose a very
particular
section 03C3 of the anti-canonical bundle of GBb.
Namely,
if wemultiply
03C3by
our volume formv[G Bb],
which we take to bedefined over the
prime field,
then werequire
theresulting
function to be theproduct
over allintegers
r between 1 and n of thepull
back from g of thesubdeterminant function
det(Xr,r).
The power03C3p-1
of u definesby [13]
atwisted linear
endomorphism 4J (1
of the structure sheaf of Gx B 6.
Here twisted linear means that it is amorphism
of sheafs of abelian groupssatisfying
the ruleIf this
endomorphism
preserves the constant function1,
then it is in fact aFrobenius
splitting. (This
is indeed what willhappen.)
3.5.
Specializing
to asubspace
Let S be an ideal of the
partially
ordered set P of3.1,
and(s, t)
a maximalelement of
S,
so that S’ = S -{(s, t)l
is also an ideal. Assume s t so that thecorresponding
coordinate does not vanish on b. Ifu[S’]
is aglobal
section of theanti-canonical bundle of G
Bb[S’],
which vanishes on GBb[S],
we wish todefine a residue res
a[S’]
ofa[S’]
such that the twisted linearendomorphism
~03C3[S’]
of the structure sheaf(!) G
Bb[S’] of Gx B b[S’],
definedby the p -
1-st power ofu[S’],
induces on the structure sheaf of the codimension 1subspace
Gx B b[S]
the twisted linear
endomorphism ~03C3[S]
definedby
the p - 1-st power of03C3[S’]
: = resu[S’].
To this end we consider onG/B
an open set V which is smallenough
to ensure that the line bundle Gx B (b[S’]/b[S])
trivializes over ESay f
is a nowhere
vanishing
section over V of the dual line bundle. We chooseres 03C3[S]
so thatfor a local
section il
of the canonical bundle of GBb[S],
withhopefully
selfexplanatory
notation. One checks that this isindependent
of theprecise
choiceof
f,
and thereforepatches
as we vary V. One also checks the desiredcorrespondence
with twistedendomorphisms, using
theexplicit
local formulasof [13].
REMARK 3.6. In 3.5 it is
actually
not essential thatf
is a section of a line bundle. The "residue" in 3.5 is dual to a Poincaré residue(cf. [6])
restricted to thesubvariety,
and thus exists ingreater generality.
3.7. Formulas
for
thespecializations
If S is as
above,
and r is aninteger
between 1 and n, let03B4r[S]
denote the matrix with a one at eachentry (1, j) e S
with i + n= j
+ r and zeroes elsewhere. The open subset U- xb[S]
of GBb[S]
isisomorphic
to a linear affine space, so ithas-up
to a constantmultiple-a
natural choice of volume form.(The
fullspace G
x B b[S] usually
has no volumeform.) Multiplying 6[S] by
such avolume form we claim to
get
a functionsending (g, X)
E U- xb[S]
to a constanttimes the
product
over allintegers
r between 1 and n of the subdeterminantsdct((g(X
+03B4r[S])g-1)r,r).
THEOREM 3.8. For each ideal S
of P
there is a sequenceof specializations (cf. 3.5) starting
with uof 3.4
andending
witha[S]
as in in 3.7. The p - 1-st powerof a[S] defines
a Frobeniussplitting
on G x Bb[S].
Thissplitting
is also inducedby
the
splitting ~03C3 of G x B b.
3.9. Start
of proof
We argue
by
induction on the size of S to show thatspecialization
leads to theformulas indicated in
3.7,
but we will go in the other direction to prove that one has Frobeniussplittings.
The formula for6[S]
isby
definition correct whenb[S]
equals
b.(Note
that in this case i> j
for(fj)
E S so that03B4r[S]
vanishes for rn.)
Therefore let us now assume S contains a maximal element
(s, t) with s
t. Weassume the formulas true for S’ = S -
{(s, t)l.
Put r = s + n - t. For(g, X) E
U - xb[S’]
thehypotheses
of Lemma 3.3apply
with M = X +03B4r[S’].
Moreover
Mr,>-r
is a block matrixwith determinant
det(a)X,, det(03B2).
We may useXst
as thef
of3.5,
at least overthe open subset U - of
G/B.
As U - xb[S]
is dense in GBb[S],
thehypotheses
for the residue construction are satisfied and we
only
need to check that itreplaces
the factordet((X
+03B4r[S’]),>n-r)
in theproduct
foru[S’] by
the factordet((X
+03B4r[S])r,>n-r)·
Indeed one mustput Xst equal
to zero in theregular
function
det(Mr,>n-r)/Xst
=det(03B1) det(03B2).
And thisgives
the same asputting Xst equal
to zero indet((X
+03B4r[S])r,>n-r).
3.10. The
splitting of G/B
We take S = P and
investigate Q[S].
It is a section of the anti-canonical bundleof G B0 = G/B.
Its p - 1-st power defines a twistedendomorphism ~03C3[S]
of thestructure
sheaf,
which is a Frobeniussplitting
if~03C3[s](1)
= 1. AsG/B
iscomplete,
we may
try
the criterion in terms of local coordinates around aspecial point, given
inProposition
6 of[13].
Asspecial point
we take theorigin B,
and werestrict to its
neighborhood
U - =U - B/B.
But for the coordinatesof g E U - we
take the matrix coefficients
Yij
with i> j
of the inverse matrix. Theproduct
ofu[S]
with the volume form of U - isgiven by
theproduct
of the subdeterminantsdet((g-1)>n-r, r).
For r = 1this gives Yn,1. Putting
that coordinateequal
to zeroone
gets Yn-1,1 Yn,2
as subdeterminant for r = 2.Putting
those two coordinatesequal
to zero too, onegets Yn-2,1 Yn-1,2 Yn,3
as the subdeterminant for r = 3.Proceeding
in this manner, one sees that the p - 1-st power of theproduct
of thesubdeterminants has 1 as the coefficient of the monomial
03A0i>j Yp-1ij.
This showsthat we have a
splitting. (As
ithappens,
thenormalizing
constant is auto-matically
correct because we started withsomething
defined over theprime
fieldand then took a p - 1-st power. Otherwise we would have had to rescale
~03C3.)
3.11. End
of proof of
3.8We now know that
~03C3
induces asplitting
on GB0,
socP(1(I)
restricts to 1 onG
B0.
It remains to show that it is 1 on all of Gx B b.
Now if c is a nonzeroconstant, we
get
anautomorphism hc
of Gx B b given by [(g, X)]
H[(g, cX)].
Under this
automorphism
the section 03C3 goes to a nonzero constantmultiple
ofitself,
because determinants are multilinear. Thisimplies
that the zero set of~03C3(1)
is invariant under
hc,
for all nonzero c. As~03C3(1)
is 1 on the zero section of the vector bundle Gx B b
overG/B,
the result follows.Alternatively,
one may show that 03C3 extends to acomplete variety, by embedding
b as an open subset of theprojective
spaceP(b
Ef)k)
... ~4.
Conjugacy
classes ofnilpotent
matrices4.1. Partitions
Given the
conjugacy
classC(N)
of anilpotent
element N of g, one may associate to it twopartitions
of n. Thefirst,
say03C0(N) = (n[N]
1,...,n[N]r),
consists of the sizes of the Jordanblocks,
indescending
order. The second is the dualpartition 03C0’[N].
It may also be read off the dimensions of the kernels of the powers ofN,
inan easy way. Let F be the
partial flag
in k nwhose i-thpart
isspanned by
the first03C0’[N]1
+ ... +03C0’[N]i standard
basis vectors,(0
i03C0[N]1),
and letP[N]
bethe stabilizer of the
flag
F. ThenP[N]
is aparabolic subgroup
and the sizes of the blocks in its Levisubgroup
areexactly given by n’[N].
Letr[N]
be the Liealgebra
of theunipotent
radicalR(P[N])
ofP[N]
It has an openorbit,
calledr[N]reg,
under the actionof P[N].
This orbit is the open dense subsetconsisting
of the elements whose powers have maximal
rank,
i.e. such that the i-th powerhas rank
03C0’[N]i+1
+ ... +03C0’[N]S,
where s =n[N]
1 is also the number ofsimple
factors of the Levi group. The
regular
orbit is also the intersection of the G orbit of N withr[N].
An element X of the Liealgebra r[N]
doesnot just
preserve theflag;
itactually
satisfiesX(Fi)
ceFi-1
and thus induces mapsFi/Fi-1 ~ Fi-l/Fi-2.
One checks that itbelongs
to theregular
orbit if andonly
if all these maps are
injective.
4.2. Resolution
Let p
denote the map from GBb
to ggiven by [(g, X)] - Ad(g)(X).
We want totake a "direct
image"
of thesplitting ~03C3 along
p.THEOREM 4.3. The twisted
endomorphism of 03C1*(OG Bb)
inducedby ~03C3
leavesinvariant the
subsheaf Og,
and thusyields
a Frobeniussplitting 0 of
g. For eachnilpotent
matrix N in g thissplitting
iscompatible
with the closureof the conjugacy
class
of
N.Proof.
Letf
be aregular function,
defined on some open subset V of g. As p is proper,h(03C1-1(v), (9G Bb)
is finite overr( V, (9.). Moreover,
g is a normalvariety,
so to prove that
cP(1(f)
EF(V, Og),
it suffices to show that it is in the function fieldk(g)
of g. Now the function field of Gx ’
b is the same as the function field of G Bbreg
= G x Ttreg,
and the latter function field is a Galois extension withgroup W of k(g),
see[2].
Thus what we need to show is that~03C3(f)
is W invariant.As
f
is Winvariant,
this will follow if the restriction of the Frobeniussplitting
~03C3
to G x Ttreg
is invariant. It is indeed invariant because of Lemma 2.7 and the construction of~03C3. (The p -
1-st power of thesign representation
is the trivialrepresentation,
and functions that arepulled
back from g areinvariant.)
Toprove the last sentence of the
theorem,
we use thatr[N]
is one of theb[S] of 3.1,
because the
parts
ofx’[N]
are orderedby descending
size. Thusby
theorem 3.8~03C3
leaves invariant the ideal sheaf of Gx B r[N]
andthus 0
leaves invariant theideal sheaf of
p(G Br[N]),
which is indeed the closure of theconjugacy
classof N.
NOTATION 4.4.
If N ~ g is a nilpotent
element and S is such thatr[N]
=b[S],
we write
a-[N]
forQ[S], b[N]
forb[S], 03B4r[N]
forbr [S]. By p[N]
we denote therestriction
of p to G x B r[N]
with astarget
the closure of theconjugacy
class ofN.
PROPOSITION 4.5.
If
N E g isnilpotent,
there is aprincipal effective
divisor Dwhich contains the
exceptional
locusof p [N] :
G x Br[N] ~ C(N)
and on which03C3[N]
vanishes.Proof.
Let us show first thatu[N]
vanishes on theexceptional locus.
Thislocus is the
complement
of GBr[N]reg.
As its intersection with the open set U - xr[N]
isdense,
we may restrict attention to that open set. Let us consider(g, X ) E
U - xr[N]
such that6[N]
does not vanish at[(g, X)].
We have to showthat
X ~ r[N]reg.
The mapFi/Fi-l 1~ Fi-1/Fi-2
inducedby
X isgiven by
asubmatrix a of X with
03C0’[N]i columns
and03C0’[N]i-1
rows.(2
i03C0[N]1).
Letfl
be the submatrix of aconsisting
of the bottom7r’[N]j
rows. Choose r such thatfi
is one of the blocksalong
thediagonal
in(X
+03B4r[S])r, >n-r·
Then thehypotheses
of Lemma 3.3apply
with jB1 = X +03B4r[S],
sodet(Mr,>n-r)
does notvanish. But
M r,
>n-r is a block matrix of the formso
fi
has full rank and the mapFi/Fi-1 ~ Fi-l/Fi-2 is injective.
It follows thatX E r[N]reg.
Tofinish,
check that the map(g, X) H det(03B2)
defines aregular
function on G
x B r[N].
THEOREM 4.6.
If N E g
isnilpotent,
thenC(N)
is normal and has rationalsingularities.
4.7. Start
of proof
By 4.3, C(N)
is Frobeniussplit,
sonormality
will follow from[14]
if we find any normalvariety mapping
ontoC(N)
with connected fibres. One may use a map from[10],
but weprefer
to use thefollowing
theorem.THEOREM 4.8
(Spaltenstein).
Thefibres of p[N] :
GBr[N] ~ C(N)
areconnected.
Proof
LetM E r[N]
and let F be thepartial flag corresponding
withP[N].
Note that X ~
r[N]
if andonly
ifX(Fi)
cFi-l
for all i. Theconjugacy
classes ofnilpotents
that intersectr[N]
are those that are contained in theimage C(N)
of03C1[N]. By
section 1 of[4]
the criterion for X tobelong
to such a class is thatdim(ker Xi) dim(ker Ni)
for all i 1. In otherwords,
the condition is thatx[X] K 03C0[N]
in the "closureordering"
ofpartitions,
called "dominance" order in[5].
The fiber03C1[N]-1(M)
of M isparametrized by
which maps onto a set of
partial flags
through
a map g Hg(F),
which is a proper map with connected fibres. To provethe theorem it thus suffices to show that,97 is connected. Now P maps onto a set V of linear
subspaces
ofker(M) by
the mapf
whichassigns
to apartial flag
itsfirst
part. By
an inductionhypothesis
we may assume the fibres off
to beconnected,
asthey
are of the same nature asP,
but for smaller n. It thus remainsto understand
why 1/’
is connected.By
the remarks above Y consists of the03C0’[N]1
dimensionalsubspaces
Lof ker(M)
for which themap X
=ML
inducedby
M onk"IL
satisfiesdim(ker Xi) dim(ker N’) - dim(L)
for i 1. Now onecan be
quite explicit
about the way the Jordantype
ofML 2013 or
theYoung/Ferrers diagram
of itspartition depends
on the choice of L.(We
maynow
forget
aboutN.) Let ei,j
be a Jordan basis of kn forM,
witheij ~ ei,j-1~ ··· ei1 ~ 0.
One may think of this basis as indexed
by
the boxes of theYoung diagram
ofrc =
03C0[M].
For asubspace
L of ker M =span(el
i,...,els)
we define apivot
to bean
integer
i such that L intersects e 1 +span(e11,..., e 1, i -1 ). Taking
vectors thatrealize the
respective pivots gives
a basis of L and the Jordantype
ofML
isobtained from that of M
by making
the i-th block one smaller if i is apivot.
(Exercise.)
In termsof n[M],
one should subtract 1 fromn[M]i
when i is apivot,
and then reorder the
parts again by size, if necessary.
If L has i as apivot,
but noti -
1,
then one maymodify
thecorresponding
basis vector, and thus alsoL,
to lower thepivot by
one.Doing this,
the otherpivots
remain the same anddim(ker(ML)i)
canonly increase,
as one seesby looking
at thepartitions.
So onedoes not leave Y’ this way. It is easy to realize such a
lowering
of apivot
in a oneparameter family
ofsubspaces
in which thegeneral
element has theoriginal
setof
pivots
and thespecial
element has the "lower" set. Thisfamily
thus lies inside V. The process may berepeated
until the set ofpivots is {1,..., dim(L)},
inwhich case L =
span(e11,
... ,el ,dim(L»).
All of r is thus in the same connectedcomponent
as thisparticular subspace.
4.9. End
of proof of
4.6The map
p[N]
factorsthrough
the birational map GP[N]r[N] ~ C(N)
and thehigher
directimages
of(9G x B,,[N] in G P[N]r[N]
vanish because GBr[N] ~
GP[N]r[N]
is a fibration with fibreP[N]/B
to whichKempf’s vanishing
theoremapplies.
Further thesplitting
of G x Br[N]
iscompatible
withthe zero set
of 03C3[N]
and its subdivisor D from 4.5(see [13]
Remark on page34;
observe that the scheme
03C3[N]
= 0 cannot contain a divisor withmultiplicity
> 1 because that would make thesplitting
wrong in localcoordinates).
Soby [ 15]
itfollows from 4.5 that the
higher
directimages
inC(N)
of the structure sheaf ofG
x B r[N]
vanish.By
theLeray spectral
sequence thehigher
directimages
inC(N)
of the structure sheaf of G x P[N]r[N]
also vanish. And that structure sheafis also
isomorphic
with the canonical bundle. We have thus checked the conditions statedby Kempf
on page 51 of[8].
DReferences
[1] W. Borho und H. Kraft, Über Bahnen und deren Deformationen bei linearen Aktionen reduktiver Gruppen, Comm. Math. Helv. 54 (1979), 61-104.
[2] E. Brieskorn, Singular elements of semi-simple algebraic groups, Actes du Congrès Inter-
national des Mathématiciens 1970, tome 2, 279-284 Gauthiers-Villars, Paris (1971).
[3] S. Donkin, The normality of closures of conjugacy classes of matrices, Invent. Math. 101 (1990),
717-736.
[4] M. Gerstenhaber, On nilagebras and linear varieties of nilpotent matrices, III, Annals of Math.
70 (1959), 167-205.
[5] M. Gerstenhaber, On dominance and varieties of commuting matrices, Annals of Math. 73 (1961), 324-348.
[6] P. Griffiths and J. Harris, Principles of algebraic geometry, Wiley & Sons, New York (1978).
[7] W. Hesselink, The normality of closures of orbits in a Lie algebra, Comm. Math. Helv. 54, (1979), 105-110.
[8] G. Kempf et al., Toroidal embeddings, Lecture Notes in Math. 339, Springer 1973.
[9] H. Kraft, Parametrisierung von Konjugationsklassen in sIn, Math. Annalen 234 (1978), 209- 220.
[10] H. Kraft and C. Procesi, Closures of conjugacy classes are normal, Inv. Math. 53 (1979), 227- 247.
[11] G. Lusztig, Green polynomials and singularities of unipotent classes, Adv. in Math. 42 (1981),
169-178.
[12] O. Mathieu, Formules de caractères pour les algèbres de Kac-Moody générales, Astérisque 159-160 (1988).
[13] V. B. Mehta and A. Ramanathan, Frobenius splitting and cohomology vanishing for Schubert varieties, Annals of Math. 122 (1985), 27-40.
[14] V. B. Mehta and V. Srinivas, Normality of Schubert varieties, American J. of Math. 109 (1987), 987-989.
[15] V. B. Mehta and W. van der Kallen, On a Grauert-Riemenschneider vanishing theorem for Frobenius split varieties in characteristic p, to appear in Inventiones Math.
[16] A. Ramanathan, Equations defining Schubert varieties and Frobenius splitting of diagonals,
Publ. Math. IHES 65 (1987), 61-90.