Homology for irregular connections
par SPENCER BLOCH et HÉLÈNE ESNAULT
RÉSUMÉ. Nous définissons sur une courbe
algébrique l’homologie
à valeurs dans une connexion avec des points
singuliers
éventuelle- mentirréguliers, généralisant
ainsil’homologie
à valeurs dans lesystème
local sous-jacent pour une connexion avec points sin-guliers réguliers. L’intégration
définit alors unaccouplement
par- fait entre lacohomologie
de de Rham à valeurs dans la connexionet
l’homologie
à valeurs dans la connexion duale.ABSTRACT.
Homology
with values in a connection withpossibly irregular singular
points on analgebraic
curve isdefined,
gener-alizing homology
with values in theunderlying
local system fora connection with
regular singular
points.Integration
defines aperfect
pairing between de Rhamcohomology
with values in the connection andhomology
with values in the dual connection.0. Introduction
Consider the
following formulas, culled,
one mayimagine,
from a text-book on calculus:
Gamma function Bessel function.
These are a few familiar
examples
ofperiods
associated to connections withirregular singular points
on Riemann surfaces.Curiously, though
ofcourse such
integrals
have been studied for 200 years or so, and math- ematicians in recent years havedeveloped
apowerful duality theory
forholonomic D-modules
(for
dimension1,
which is theonly
case we will con-sider,
cf.~4~,chap. IV,
and~5~),
it is not easy from the literature tointerpret
such
integrals
asperiods arising
from aduality
betweenhomological cycles
and differential forms. A
homological duality
of this sort is well understoodfor differential
equations
withregular singular points,
and forspecial
rank1 differential
equations [2].
Our purpose in this note is todevelop
a similartheory
in theirregular
case. Of course, most of the"heavy lifting"
was doneby Malgrange
op. cit. Wehope,
inreinterpreting
histheory,
to better un-derstand relations between
irregular
connections andwildly
ramified f-asdic sheaves. There arestriking
relations between E-factors for .~-adic sheaveson curves over finite fields and determinants of
irregular periods [8]
whichmerit further
study. Finally,
relations betweenirregular
connections and the arithmetictheory
of motives remainmysterious.
Let X be a
smooth, compact,
connectedalgebraic
curve(Riemann
sur-face)
over C. Let D = C X be anon-empty,
finite set ofpoints (which
we also think of as a reduced effectivedivisor),
and writeU : :=
X D -4
X . Let E be a vector bundle onX,
and supposegiven
aconnection with
meromorphic poles
on DHere w is the sheaf of
holomorphic
1-forms on X and *D refers to mero-morphic poles
on D. Unless otherwiseindicated,
we workthroughout
inthe
analytic topology.
The de Rhamcohomology HDR (X B D; E, V)
is thecohomology
of thecomplex
of sectionsplaced
indegrees
0 and 1. Thesecohomology
groups are finite dimensional~1~, Proposition 6.20, (i).
Let
E’
be the dualbundle,
and letV~
be the dualconnection,
soDefine E =
ker(V),
and£v
=ker(V )
to be thecorresponding
localsystems
of flat sections on U. We want to definehomology
with values in these localsystems,
or moreprecisely
with values in associated cosheaves on X. For~
E X B D, Ex
will denote the stalk of E at x. Define the co-stalk at 0 E Dwhere
x =A
0 is anearby point,
and is the localmonodromy
about 0. Wewrite
Cn - Cn(E, V)
for the group of n-chains with values in £ andrapid decay
near 0. Write On for then-simplex
and b E On for itsbarycenter.
Thus, Cn (E, V)
isspanned by
elements c(9,E with c : On -- X and e E9,(b),
where b E On is the
barycenter.
We assumec-1 (o)
= union of faces C Anand that E has
rapid decay
near D. This is no condition if D nc(,An) = 0.
If 0 E D n
c(On),
we take ei a basis for E near 0 and write E= E f2c*(ei).
Let z be a local parameter at 0 on A. We
require
that for all N EN,
constants
CN
> 0 exist withCNlzlN
onc-1 (o) .
Note that ifV has
logarithmic poles
in onepoint,
thenrapid decay implies vanishing.
Thus in this case, we deal with the sheaf
itS, where j : X ~
D --~ X .There is a natural
boundary
mapwhere cj are the faces of c. Note if
bj
is thebarycenter
of thej-th
faceand
0,
c determines apath
fromc(b)
to which is canonicalupto
homotopy
on{0~. (As
arepresentative,
one can takec[bj, b~,
theimage
of thestraight
line from b tobj . By assumption, c-1(0)
is a union offaces,
so it does not meet theline.)
Thus E E9,(b)
determines cj ESimilarly
for 0 ED,
ifc(bj)
= 0 there iscorresponding
to E auniqueej
ESo
because we have taken coinvariants. If c : 0’~ - D is a constant
simplex,
there is no
rapid decay
condition.It is
straightforward
tocompute
that 9o9 = 0. Consider c06. Ifc(b)
=0,
where b E
02
is thebarycentre,
thenc(A2)
= 0 and E = Ei = ESo
forall i
and j involved,
thus the condition istrivially
fulfilled. If not, and somec(bi)
=0,
then(ej)j
= E£o
for allj,
and if all0,
then one hasby unique analytic
continuation inc(02)
the relation(Ei)j
=(Ej)i
ESedgeij
for all
i, j,
ifedgeij 0 0,
else in£o.
We define
(The growth
condition means thisdepends
on more thanjust
thetopo- logical
sheaf£V,
so wekeep E~, V’
in thenotation.)
We now define a
pairing
by integrating
over chains in thefollowing
manner. For * =0,
thenHo (X, D; E’, ý7V)
isgenerated by
sections of the dual localsystem 6’
inpoints
E X whileHDR (X B D; E, V)
isgenerated by global
flat sections in~ with moderate
growth.
So one canpair
them. For * =1,
sinceD ~ 0,
then
and since classes c Q9 E
generating
haverapid decay,
theintegral Ie
> isconvergent,
where 0152 eHO(X,wQ9E(*Ð))
and> is the
duality
betweenE~
and E.The rest of the note is devoted to the
proof
of thefollowing
theorem.Theorem 0.1. The process
of integrating forms
over chains iscomPati-
ble withhomological
andcohomological equivalences
anddefines
aperfect
pairing of finite
dimensional vectorcomplex
spacesFIGURE 1. c0
e-tts represents
a class inHl
Example
0.2.(i).
If V hasregular singular points,
there are norapidly decaying
flatsections,
soH* (X B D; ~~ ) . Also, HDR(X B D; E, ~) ~’ H*(U,£) (cf. [1],
Th6or6me6.2),
and the theorem becomes the classicalduality
betweenhomology
andcohomology.
(ii). Suppose
X =p1,
D =f 0,
Let E =Opi
with connectionB7(I)
= for Then .6 CEu = Ou
is the trivial local
system spanned by ett-S,
so£v
CEv
=Ou
isspanned
by e-tts .
We consider thepairing HDR
x C from theorem 0.1. Note first that has dimension1, spanned by
This can either be checkeddirectly
from(0.l), using
or
by showing
the de Rhamcohomology
isisomorphic
to thehypercoho- mology
of thecomplex w ((0) -f- 2(00)),
which iseasily computed.
Tocompute H, (X, D; E’, ~~),
thesingularity
at 0 isregular,
so there are nonon-constant,
rapidly decaying
chains at 0. The sectionE’
:=e-tts
of£v
is
rapidly decaying
on thepositive
real axis near oo, so the chain c infig.
I aboverepresents
a1-cycle.
We havewhich is a variant of Hankel’s formula
(see ~10~,
p.245).
(iii).
LetX, D, E
be as in(ii),
but take= 2 (d(z~cc) - d(~))
for somez E
C B {0}.
Here the connection haspole
order 2 at 0 and oo and ithas trivial
monodromy. Arguing
asabove,
onecomputes dim H1R
=2,
generated by
p EZ,
with relations uPduup-2du.
The GauB-Manin connection on this group is
Assume
Im(z)
> 0. Then the vector space is gen- eratedby
, , , ,
(If 0,
then the secondpath
must bemodified.)
Theintegrals
are
periods
andsatisfy
the Bessel differentialequation
The function
Jn
is entire. To show thatHn
islinearly independent
ofJn,
it will then be sufficient to show that
Hn
is unbounded on thepositive
part of theimaginary
axisRe(z) =
0 as z - 0.Making
the coordinatechange v
=~,
andreplacing
yby ly
one is led to show thatfo exp(-y(v
+v ) ) dv
is unbounded for y >0,
y - 0.Writing En (v) =
f100,
andmaking
thechange
ofvariable v v
in theintegral f01,
oneobtains
For
I,
then thisexpression
is 2:: which isobviously
unbounded. For n =
0,
one haswhere in the last
inequality,
we have assumed that2y
1. This lastintegral is,
up tosomething bounded, equal
g q to 21 dv =
v-2 log(2y) , g( J)
whichis
unbounded,
>0,
y - 0.Usually,
forintegers nEZ,
one considersJn
as one standardsolution,
but not
Hn (see [101, p.371 ) . Finally,
to get Bessel functions fornon-integral
values of n, one may consider the connection
1. Chains
Let D
= ~ x 1, ... ,
be asabove,
and letAi
be a small diskabout x2
for each i.
Let 6j
be theboundary
circle. Define(Note,
for a setlike 8i
which is closed anddisjoint
fromD,
our chainscoincide with the usual
topological
chains with values in the localsystem
S. The groupV)
consists of constant chains c : On 2013~ withvalues in
for some x near x2 as in
(0.3), where pj
is the localmonodromy
aroundxi.)
In the
following theorem, ~(!7,~*)
is the standardhomology
associated to the localsystem
on U= X B
D.Theorem 1.1. With notation as
above,
there is along
exact sequencebe the
complex calculating
be the
subcomplex calculating H* (U, E),
i.e. thesubcomplex
of chainswhose
support
isdisjoint
from D. Of course, one hasC* (U; E, ~) - C* (U; E),
whichjustifies
the notation.Write B =
C* /C* ( U) .
There is an evident map ofcomplexes
which must be shown to be a
quasi-isomorphism.
LetObviously
the map a :EBiB( i)
~ 13 is an inclusion. We claim first that ais a
quasi-isomorphism.
To seethis,
note that all thesecomplexes
admitsubdivision maps subd which are
homotopic
to theidentity.
Given a chainc E
B,
there exists an N such thatsubd~’(c)
ETaking
c withBe =
0,
it follows thatEBH*(B(i)) surjects
ontoH*(13).
Ifa(z)
=ay,
wechoose N such that =
a(z).
Since a isinjective
and commuteswith
subd,
it follows that a isinjective
onhomology
aswell,
so a is aquasi-isomorphism.
It remains to show the
surjective
map ofcomplexes
is a
quasi-isomorphism.
The kernel ofj3
iswhich is
acyclic
asJi
~Ai B
admits an evidenthomotopy
retract.The next
point
is to showThe assertion for
Ho
is easy because anypoint
y in can be attachedto ði by
a radialpath
r notpassing through
xi - Then EE Ey
extendsuniquely
to E on r and8( r 0 E)
= Y 0 E mod chains on6i. Vanishing
in(1.4)
when i = 2 will beproved
in a sequence of lemmas. For conveniencewe
drop
thesubscript
i andreplace zi
with 0.Lemma 1.2. C A be a radial line
meeting J at p.
be the spaceof
sectionsof
the localsystem along f B
withrapid decay
at 0. Then....
Proof of
lemrraa. LetC* (£)
be thecomplex
of chainscalculating
this homol- ogy, and letC* (£ ) {0})
CC* (P)
be thesubcomplex
of chains notmeeting
0.Then
C,, (f B ~0~)
iscontractible,
andwhere
C*
denotes classicaltopological
chains. The result follows. 0 One knows from thetheory
ofirregular
connections in dim 1[4]
thatA B ~0~
can be coveredby
open sectorsV C A
such than(1.5)
where
Li
is rank I andMi
has aregular singular point.
Let W C VU ~ 0 ~
be a smaller closed sector with outer
boundary 6w
= 6 n W and radial sides£1, £2.
Recall the Stokes lines are radial lines where the horizontal sections of theLi
shift fromrapid decay
torapid growth.
We assumeW contains at most one Stokes
line,
and that£1, £2
are not Stokes lines.Writing
W =Wi
UW2,
whereWi
are even smallersectors,
each of whichcontaining
the Stokes line if there is one, one may think of thefollowing
lemma as a
Mayer-Vietoris
sequence.Lemma 1.3. With notation as
above,
let w be abasepoint
in the interiorof W .
ThenProof of
lemma. One hasand of course the assertion of the lemma is that this coincides with e3
,Et2
-~££1 +’Ef2 .
To checkthis, by (1.5)
one is reduced to the case E = where L has rank 1 and M hasregular singular points.
If W does not contain a Stokes line for L then
Efl =’Et2
=+’Ef2,
andthe
argument
isexactly
as in lemma 1.2.Suppose
W contains a Stokes line for L. Then(say) = Sw
and.6,2 = (0).
LetC* (W )
be thecomplex
of chainscalculating
the desiredhomology,
and letC* (W ) (0))
cC* ( W )
be the chains notmeeting
0. Asin the
previous lemma, C* (W B {0})
isacyclic.
We claim the mapis a
quasi-isomorphism.
If we choose anangular
coordinate 0 such thatthen rotation
re(1-t)i8 provides
ahomotopy
contraction of the in- clusion of.~1
C W. Thishomotopy
contraction preserves the condition ofrapid decay, proving
the lemma. DLet 7rd : A 2013~ A be the ramified cover of
degree
d obtainedby taking
thed-th root of a
parameter
at 0.By
thetheory
of formal connections[4],
onehas,
for suitabled,
adecomposition
as in(1.5)
for the formalcompletion
of the
pullback 7r*E
0Mi.
Let m2 be thedegree
of thepole
of theconnection on
Li
when weidentify Lj -£ 8,
i.e. =gi (z)dz
for a localparameter z,
and mi is the order ofpole
of gi . Lemma 1.4. We haveProof of
lemma. Assume first that we have adecomposition
of thetype
(1.5)
on Eitself,
i.e. that nopullback 7r~
is necessary. We write A as aunion of closed sectors
Wo, ... ,
whereWi
has radialboundary
linesti
andRi+1.
We assume eachWi
has at most one Stokes line.Using
excisiontogether
with theprevious
lemmas weget
By
lemma1.3,
the map v above isgiven by
An element in the kernel of v is thus a section e which has
rapid decay along
each£i .
Since eachWi
contains at most one Stokesline,
suchan e would
necessarily
haverapid decay
on every sector and thus would be trivial. This provesvanishing
forH2 (A, 8; E, V). Finally,
to compute the dimension ofHl,
note that ifLi
has a connection withpole
of order m2, then it has a horizontal section of the formef ,
wheref
has apole
of order1.
(The
connection is 1 ~df .) Suppose f = az1-mi
+ .... Stokeslines for this factor are radial lines where
azl-mi
is pureimaginary. Thus,
there are
2(mi - 1)
Stokes lines for this factor. Consider one of the Stokeslines,
and suppose it lies inWk.
If the realpart
ofchanges
fromnegative
topositive
as we rotate clockwisethrough
thisline,
say we are incase +, otherwise we are in case -. We have
since the two cases
alternate,
weget
a contribution of(mi - 1 ) dim(Mi ) .
Ifmi 1 there are no
rapidly decaying sections,
so that case can beignored.
Summing
over i with 2gives
the desired result.Finally,
we must consider thegeneral
case when thedecomposition ( 1.5)
is
only
available on7r*E
for some d > 2.By
a traceargument, vanishing
of the
homology upstairs,
i.e. for7r*E,
indegrees
1implies vanishing
downstairs. Since
A B f 01 --+ A ) (0)
isunramified,
an Euler charac- teristicargument (or,
moreconcretely, just cutting
into small sectors overwhich the
covering splits)
shows that the Euler characteristicmultiplies by
d under
pullback, proving
the lemma. DIn
particular,
we have nowcompleted
theproof
of theorem l.l. D 2. de RhamCohomology
In this
section, using
differentialforms,
we construct the dual sequence to thehomology
sequence from theorem 1.1.(More precisely,
we continue towork with
E, V,
so the sequence we construct will be dual to thehomology
sequence with coefficients in
E~, V~).
Consider thediagram
ofcomplexes
A result
of Malgrange [6]
is thatB7 an/mero
issurjective.
Define N :=e3iNi
=ker(Van/mero) -
* Since none of these sheaves hashigher cohomology (by
as-sumption D ~ 0)
weget
a 5-term exact sequenceby taking global
sectionsand
applying
theserpent
lemma:Theorem 2.1.
Integration of forms
over chainsdefines
aperfect pairing
between the exact sequence
(2.2)
and the exact sequencefrom
theorem 1.1:-1 1 / -1 1 1 i /
Proof.
To establish the existence of apairing,
note that if c 0Ev
is arapidly decaying
chain and 7y is a form of the samedegree
with mod-erate
growth,
thenelementary
estimates show is well defined.Suppose
c : On - X and write On -limt-o A’
whereA’
denotesOn B
tubularneighborhood
of radius t around Let ct = and sup- pose q = dT where T has moderategrowth
also. ThenNote 8c may include
simplices mapping
to D. Our definition(0.5)
offactors these chains out.
Thus,
we doget
apairing
ofcomplexes.
Of course, chains away from D
integrate
with forms withpossible
essen-tial
singularities
on D. Tocomplete
thedescription
of thepairing,
we mustindicate a
pairing
To
simplify
notation we willdrop
thesubscript
i andtake xi
= 0. Anelement in
Hl
can berepresented
in the formE’
® c where c is a radialpath.
Let c n i ={p}.
Given n EN,
choose a sector Wcontaining
c onwhich E has a basis
By assumption,
we canrepresent
rc witha2
analytic
on the open sector, such thatwhere ei from a basis of E in a
neighborhood
of 0and qj
aremeromorphic
1-forms at 0. then
by
definitionThe
pairing
is taken to be trivial on chains which do not contain 0. If s isa 2-chain
bounding
two radialsegments
c and c’ and apath along 6
fromp to
p’.
ThenCauchy’s
theorem(together
with alimiting argument
at0) gives
Similar
arguments
show thepairing independent
of the choice of the radiusof the disk.
Also,
if¿ aiEi with bi meromorphic
at0,
thenIt follows that the
pairing
is well defined.Lemma 2.2. The
diagrams
and
commute.
Proof of
lemma. Consider the top square. Thetop
arrow isexcision,
re-placing
a chain with the part of itlying
in the disksAi.
The bottom arrowmaps an n as above in some
Ni
toE
ej 0 77j 0daj . Along
c outsidethe disks
E ej
is exact; itsintegral along
the chain is a sum of terms ofthe form
(pi)
where pi E c f1Ji.
For thepart
of the chain inside theAi
of course we must take(E v, ,ej)i7j. Combining
these terms withappropriate signs yields
the desiredcompatibility.
For the bottom square, the
top
arrow associates to a relative chain onAi
itsboundary on 61
C U. The bottom arrow associates to a horizontalsection E on U the
corresponding
element in N. Note here the aj will be constant so in thepairing
with Nonly
the term -~(E~, ej)aj(p)
survives.The assertion of the lemma follows. 0
Returning
to theproof
of thetheorem,
we see it reduces to apurely
localstatement for a connection on a disk. In the
following lemma,
wemodify notation, writing
N to denote thecorresponding
group for a connection on a disk A with ameromorphic singularity
at 0.Lemma 2.3. The
pairing
is
nondegenerate
on theleft,
i. e.( E V 0 c, n)
= 0for
all relative1-cycles implies n
= 0.Proof of
lemrraa. We work in a sector and we suppose the basis Ei taken in the usual waycompatible (in
thesector)
with thedecomposition
intoa direct sum of rank 1
irregular
connections tensorregular singular point
connections. Let
Ev
be the dual basis.Fix an i and suppose first Ei and
Ey
both have moderategrowth.
Weclaim ai
has moderategrowth.
For this it suffices to showdai
has moderategrowth.
ButThis has moderate
growth because,
ej, all do.Now assume 0
c, n) =
0 for allE v
Q9 c eHl.
Fix an i and assumeEZ
israpidly decreasing
in our sector. Let c be a radius in the sector withendpoint
p. We can find(cf. [4], chap. IV, p.53-56)
abasis t2
of E on thesector with moderate
growth
and suchthat ti
=so t’(
=We are interested in the
growth
of aiEialong
c. We have/... - - ’-
Asymptotically, taking y
theparameter along
c, as~/ 2013~ 0 for some k > 0 and some N > l. We need to know the
integral
has moderate
growth
as p - 0.Changing variables,
so x= y-1, q
=p-1, U
= x - q, this becomeswhere
f
is a sum of monomials in q and u withpositive
coefhcients.Clearly
this has at worst
polynomial growth
as q --~ oo as desired.Finally, assumeey
israpidly increasing
and Ei israpidly decreasing.
Wehave as above
- - -- -
In
particular,
has moderategrowth.
Thisimplies
a2 EZ =has moderate
growth
as well.Indeed, changing notation,
this amounts tothe assertion that
if g
israpidly decreasing
andg d
has moderategrowth,
then
g f
has moderategrowth.
Fix apoint
po with 0 p po. the meanvalue theorem says there exists an r with
p
r po such thatSuppose I i
Weget
proving
moderategrowth.
We conclude that our
representation
for n has moderategrowth,
andhence it is zero in N. It follows that the
pairing
N xHl --~
C isnondegen-
erate on the left. D
Returning
to theglobal situation,
we have nowand to finish the
proof
of thetheorem,
it will suffices to show these dimen-sions are
equal.
Lemma 2.4. With notation as
above, dim Ni
=dim Hi(Aj, 6i; EV, pv .
Proof of
lemma. It will sufhce tocompute
the difference of the two Euler characteristicsIt is
straightforward
to show this difference is invariant if U isreplaced by
a smaller Zariski open set, and that the Euler characteristics are mul-tiplied by
thedegree
in a finite etalecovering
V - U.Using
lemma1.4,
we reduce to the case whereformally locally
ateach x2
E D we haveE ®
Mij
withLij
rank 1 andMij
at worstregular singular.
(Here KXi
is the Laurent power series field atx2).
Let mij be thedegree
ofthe
pole
for the connection on Then one can find coherent sheavessuch that
It follows
that, writing g
=genus(X),
Since
(which
is provenalgebraically
asabove, replacing V by
theregular
connec-tion associated
to E)
it follows that"J
Referring
to lemma1.4,
we see that this is the desired formula. D Thiscompletes
theproof
of the theorem. DReferences
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Spencer BLOCH Dept. of Mathematics
University of Chicago Chicago, IL 60637, USA
E-mail : [email protected]
H616ne ESNAULT Mathematik Universitat Essen
FB6, Mathematik 45117 Essen, Germany
E-mail : esnaultCduni-essen. de