Astérisque
M ARIUS V AN DER P UT
Recent work on differential Galois theory
Astérisque, tome 252 (1998), Séminaire Bourbaki, exp. n
o849, p. 341-367
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341
RECENT WORK ON DIFFERENTIAL GALOIS THEORY
by
Marius VAN DER PUT Seminaire BOURBAKI50eme
amnee, 1997-98,
n° 849Juin 1998
1. INTRODUCTION
Linear differential
equations
have a richvariety
ofaspects: asymptotic theory,
differen-tial Galois
theory,
the construction ofalgorithms,
arithmeticproperties,
Grothendieck’sconjecture, rigid
differentialequations
et cetera. We will restrict our attention to recent progress on the inverseproblem
for the differential Galoistheory.
For thehistory
of thisproblem
we refer to the excellent survey paper[S]
and its references. Our purpose is toexplain
andpartly
prove the results obtainedby
J.-P.Ramis,
C. Mitschi and M.F.Singer.
Let us
give
twoexamples
of the results that wehope
toexplain:
(1) Every
connected reductive groups over C can be realized as the differential Galois group of anequation ~ = (Ao
+Aiz)y,
with constant matricesAo, A1.
(2)
There is no linear differentialequation
over the field ofconvergent
Laurent seriesC({z})
with differential Galois groupG~.
In this
presentation
we have taken theliberty
ofchanging proofs, omitting
material andadding
new material withrespect
to theoriginal
papers.2. PICARD-VESSIOT THEORY
A
differential field
K is a fieldequipped
with a differentiation(or derivation) f
Hf’
satisfying
the usual rules:( f
+g)’
=f’ + g’
and( f g)’
=f’g
+f g’.
The field of constantsC is defined
by
C ={a
EKI
a’ =0}.
We will suppose in thesequel
that C is analgebraically
closed field of characteristic zero and thatC ~
K. The derivatives of anelement
f
will be denotedby f’, f", fill, ...
orf (11, f(2) , f (3i,
.... A scalarhomogeneous
linear
differential equation of
order n is anequation
of the formThe solution space
{y
EK~ L(y)
=0}
is a vector space over C of dimension n. In gen- eral the dimension isstrictly
less than n. This leads to the definition of a Picard- Vessiotring
E D K for theequation
L:(i)
TheK-algebra
E isequipped
with a differentiation(also
denotedby ’) extending
the differentiation of K.
(ii)
E hasonly
trivial differential ideals.(iii)
The space V :={a L(a)
=0}
is a vector space over C of dimension n.(iv)
TheK-algebra
E isgenerated by
the elements of V and their derivatives.It can be shown that a Picard-Vessiot
ring
exists and that it isunique
up to differentialisomorphism.
Moreover E has no zero divisors and its field of fractions has C as set of constants. The field of fractions of a(or the)
Picard-Vessiotring
is called a(or the)
Picard-Vessiot field of the
equation
over K. The space V will be called the solution space of L. Let G denote the group of the differentialautomorphisms
ofE/K.
This group actsas a group of C-linear
automorphisms
of V C E. The induced grouphomomorphism
G --~
GL(V)
turns out to beinjective
and itsimage
is analgebraic subgroup
ofGL(V).
The
di ff erential
Galois groupof
theequation
Lover K is defined to be G with its structure of linearalgebraic
groupgiven by
theembedding
G CGL(V).
The group G also coincides with the group of all differentialautomorphisms
of the Picard-Vessiot field over K.The Tannakian
approach
to(linear homogeneous)
differentialequations
over K isgiven
in
[De-M]
and[De].
Thisapproach
can be described as follows. LetDiffK
denote the cat- egory of the differential modules over K. Under thehypothesis
that the field of constantsC of K has characteristic 0 and is
algebraically closed,
one can show that thiscategory
is a neutral Tannakiancategory.
In otherwords,
there is anequivalence
of Tannakiancategories DiffK
~ReprH,
where H is a certain affine group scheme over C andReprH
denotes the Tannakian
category
of the finite dimensionalrepresentations
of H.For a fixed differential module M over K one can consider the full
subcategory {~M}}
of
DiffK generated by
all M ® ~ ~ ~ Q9 M Q9 M* ® ~ ~ ~ Q9 M*. Thissubcategory
is alsoa neutral Tannakian
category
and thus there is anequivalence
of Tannakiancategories
{{M}} ~ ReprG
for some affine group scheme G over C. It turns out that G can be iden- tified with the differential Galois group of M(and
is thus a linearalgebraic group).
Theequivalence
can be madeexplicit by
N Hker(8, E
Q9KN),
where E is a Picard-Vessiotring
for M over K. The G action on E induces a G action on E Q9K N which commutes with the action of 8 on E ®~ N. Inparticular, ker(8,
E Q9KN)
is a finite dimensional(algebraic) representation
of the linearalgebraic
group G.This more abstract Tannakian
approach
to differential modules has someadvantages.
An easy
application
is thefollowing
useful statement:Suppose
that G is adifferential
Galois group over K and let N C G be a normalalgebraic subgroup.
Then the linearalgebraic
groupG/N
is also adifferential
Galois group over K.Important examples of differential fields:
Let C denote an
algebraically
closed field of characteristic 0.(1)
K =C((z)),
the field of the formal Laurent series in z over C with the derivation~.
(2)
K =C({z}),
the field of theconvergent
Laurent series over the field of thecomplex
numbers with the derivation
~.
(3)
K =C(z),
the field of rational functions over C with the derivationdx.
(4)
K a finite extension ofC(z), equipped
with theunique
derivationextending
thederivation dz
ofC(z).
In otherwords, K
is the function field of a curve(irreducible, smooth, projective, connected)
over C.The theme of this
exposition
is to answer, for the differential fields K in the abovelist,
the
question:
Which linear
algebraic
groups G aredifferential
Galois groups over K ?3. THE THEOREMS
Let G be a linear
algebraic
group(over
the fieldC).
Thesubgroup L(G)
of G is definedas the group
generated by
all(maximal)
torilying
in G. It is clear thatL(G)
is a normalsubgroup
ofG,
contained in thecomponent
of theidentity
GO of G. The groupL(G)
isgenerated by algebraic subgroups
of G and hence is itselfalgebraic.
Thus the factor groupG / L( G)
isagain
a linearalgebraic
group.Theorem 3.1
(Ramis).
The local theorem.- A linearalgebraic
group G is adiffer-
ential Galois group over the
field C({z}) if
andonly if G/L(G)
istopologically (for
theZariski
topology) generated by
one element.Corollary
3.2(Ramis).- Suppose
that G is adifferential
Galois group over thefield C({z}),
thenG/L(G)
istopologically generated by
theimage of
thetopological monodromy.
Explanation
The differential
equation L(y)
= 0 overC ( { z} )
lives in fact as ameromorphic
differ-ential
equation
on aneighbourhood {z
EE}
of z =0,
which hasonly
z = 0 assingularity.
The solution space V can be identified with the solutions of theequation
atthe
point E/2. Analytical
continuation of the solutions ate/2 along
the circle around 0and
through E/2 (with positive orientation)
induces a C-linearautomorphism
of V. Thisautomorphism
can be shown tobelong
to G CGL(V).
The element is called thetopolog-
ical
monodromy.
It isunique
up toconjugation. (See
section 7 for moreinformation.) Examples
3.3 : Order twoAgain K
=C(~z~)
and consider a differentialequation
over K of order two with differential Galois group inSL(2).
The well known classification of thealgebraic subgroups
of
SL(2)
can be used in order to determine thepossible
differential Galois groups. The list(of conjugacy classes)
that one finds is:where B is the Borel
subgroup, Ga
the additive group,Gm
themultiplicative
group andD~
is the infinite dihedral group,i.e.,
thesubgroup
ofSL(2) leaving
the union of two linesLi
UL2
CC2 (through
theorigin)
invariant.Every
group in the above list can be realizedby
a differentialequation
In fact the choices
(m, ao)= (o, z), (o, z2+3z+5/4), (l, o), (o, -z42 ), (o, z-2), (o, - sz-2+
z-1), (0, 4(-1+(n)2)z-2) with §
EQ produce
the above list of differential Galois groups.Some
definitions: regular, regular singular
andirregular
Let
X/C
denote a curve(irreducible, smooth, projective)
of genus g. At thispoint
of the
exposition
it is convenient to define a(linear homogeneous)
differentialequation
over X as a matrix differential
equation y’
=Ay,
where A is a n x n-matrix with coef- ficients inK,
the function field of X. Consider apoint
c E X with local coordinate z~.The field K is embedded in
K~
=C(~z~~),
the field of theconvergent
Laurent series in Ze. Let B EGL(n, Ke).
Put v =By.
Then v satisfies the matrix differentialequation
v’ ==(B-lAB - B-1B’)v.
This newequation
overK~
is calledlocally equivalent
withy’
=Ay.
Theequation y’
=Ay
is calledregular,
resp.regular singular
at c if there is a lo-cally equivalent equation v’
= Dv such that D EM(n,
resp.z~D
EM(n,
Otherwise the
point
c will be called anirregular singularity
ofy’
=Ay.
Theorem 3.4
(Ramis).
Theglobal
theorem.- LetX/C
be a curve(irreducible, smooth, projective ) of genus g
and S ~ X afinite
set withcardinality
m > 1. A linearalgebraic
group G can be realized as thedifferential
Galois groupof
adifferential
equa- tion over X withsingularities
in Sif
andonly if G/L(G)
istopologically generated by 2g
+ m 2014 1 elements.Remark.- The theorem remains valid for S =
0
and2g
+ m -1replaced by 2g.
Corollary
3.5(Ramis).- (1) Suppose
that G is thedifferential
Galois groupfor
adiffer-
ential
equation
on X withsingularities
in thefinite
set S. Then the naturalhomomorphism S, *)
-~G/L(G)
has denseimage for
the Zariskitopology.
(2) Suppose
that the linearalgebraic
group G can be realizedfor
thepair (X, S),
thenG can be realized
by
adifferential equation
with at most oneirregular singular point (to
be chosen
freely
inS)
and the othersingularities, regular singular (and
inS).
Examples
3.6 : Ordertwo,
continued1) {0, oo})
and order two.The list of
possible
groups G CSL(2)
coincides with the list that we have considered in 3.3. The above list is in fact the theoreticalbackground
for thesimplification
of theKovacic
algorithm
for order two differentialequations
with at most twosingular points, presented
in[P2].
2) (P1, t0,1, oo})
and order two.Every algebraic subgroup
ofGL(2)
can be realized for thispair.
Moreprecisely,
everyalgebraic subgroup
G CGL(2)
is the differential Galois group of anequation
where
al(z), a2(z)
EC[z]. (This equation
isregular singular
at0,1
and has anarbitrary singularity
atoo).
Some
definitions :
Thedefect
and the excessof
a connected linearalgebraic
group.C denotes an
algebraically
closed field of characteristic 0. Let G be a connected linearalgebraic
group over C. Theunipotent
radical of G is denotedby Ru.
Let P ~ G bea Levi
factor, i.e.,
a closedsubgroup
such that G is the semi-directproduct
ofRu
and P(see [H],
p184).
The groupRu/(Ru,
where(Ru, Ru)
is the(closed)
commutatorsubgroup,
is a commutativeunipotent
group and soisomorphic
to C". The group P acts onRu by conjugation
and this induces an action onRu).
Therefore wemay write
Ru/(Ru, Ru)
=Ul
1 ® ~ ~ ~ ®Us 8,
where eachUi
is an irreducible P-module. For notationalconvenience,
we suppose thatUi
is the trivial 1-dimensional P-module and 0. Since P isreductive,
one can write P = T .H,
where T is a torus and H is asemi-simple
group. Define mi := nt if the action of Hon Ui
is trivial and mi := ni + 1 if the action of Hon Ui
is not trivial. Define N = 0 if H is trivial and N = 1 otherwise.The
defect d(G)
is defined to be rcl and the excesse(G)
is defined asmax(N,
m2, ...,ms).
Since two Levi factors are
conjugated,
these numbers do notdepend
on the choice of P.Furthermore,
one can show thatd(G)
is the dimension ofRu/(G, Ru).
Theorem 3.7
(Mitschi-Singer).-
Let G be a connected linearalgebraic
group over C.Then G is the
differential
Galois groupof
a matrixdifferential equation
overC(z) of
thewhere
A;,
i =1, ... , d(G)
are constant matrices andA~
is a matrix withpolynomial
entries
of degree
at moste(G).
Inparticular,
thepoints
al, ..., ad(G) are thesingularities of
theequation
in C. Thesesingularities
areregular.
Thepoint
oo ispossibly
anirregular singular point.
Remarks
The
proof
of the result above ispurely algebraic
and moreover constructive. The state- ment is moreprecise
than the one of Ramis’global
theorem and more restricted in thesense that the group G is
supposed
to be connected and that therepresentation
of Gon the space of solutions is not
prescribed. Using
Tannakianarguments
one may alsoprescribe
the faithfulrepresentation
of G on the space of solutions(at
the cost of intro-ducing possibly apparent singularities).
In section 10 we will show thatd(G)
isequal
tothe minimal number of
topological generators
ofG / L( G).
The
special
case of thetheorem,
where the group G issupposed
to be connected andreductive,
is ratherstriking.
It states that G is the differential Galois group of a matrix differentialequation ~ = (A
+Bz)y
with A and B constant matrices. In section 9 wewill
present
anexplicit proof
of this statement in case G is connected andsemi-simple.
4. ABHYANKAR’S CONJECTURE
The base field k is an
algebraically
closed field of characteristic p >0,
e.g.Fp.
One con-siders a curve
X/k (irreducible, smooth, projective)
of genus g and a finite subset S ~ X withcardinality
m > 1.Abhyankar’s conjecture
is concerned with the Galoiscoverings
ofX which are unramified outside S. For a finite group G one denotes
by p(G)
thesubgroup generated by
all thep-Sylow subgroups
of G. In otherwords, p(G)
is the smallest nor-mal
subgroup
such thatG/p(G)
has orderprime
to p. We recall the well known theorems.Theorem 4.1
(Raynaud).-
Thefinite
group G is the Galois groupof
acovering of P1, unramified
outside oo,if
andonly if
G =p(G).
Theorem 4.2
(Harbater).- (1)
Let thepair (X, S)
be as above. Thefinite
group G is aGalois group
of
acovering of X, unramified
outsideS, if
andonly if G/p(G)
isgenerated by 2g
+ m 2014 1 elements.(2) 1 f
G is a Galois groupfor
thepair (X, S),
then the naturalhomomorphism
1 S, *)
--~G/p(G)
issurjective.
(3) Suppose
thatG/p(G)
isgenerated by 2g
+ m -1 elements. Then there is a Galoiscovering of
X with Galois groupG, wildly ramified
in at most one(prescribed) point of S, tamely ramified
at the otherpoints of
Sandunramified
outside S.Remark.- The group
S,* )
denotes theprime
to p,algebraic
fundamental group ofX B
S. This group is known to betopologically generated by 2g
+ m 2014 1 elements anddepends
in factonly
on the number2g
+ m - 1.The translation
During
a dinner at Toulouse(nuit
de lamusique 1993), Raynaud
and Ramis discussed the remarkable relation between the inverseproblem
for differential Galoistheory
andAbhyankar’s conjecture.
Thefollowing
transformation rules seem to link to twosubjects:
Differential Characteristic p > 0
X/C
curve, finite5’ C X, 5’ ~ 0 X/k
curve, finitedifferential
equation equation
with Galoiscovering
of Xsingular point (in S)
ramifiedpoint (in S)
local differential Galois group inertia group
regular singular tamely
ramifiedirregular singular wildly
ramifiedlinear
algebraic
group finite groupL(G) p(G)
7ri(X B S)
-G/L(G)
Zariski dense(X ~ S)
-G jp( G) surjective
In the work of P.
Deligne,
N. Katz and G. Laumon on(rigid)
differentialequations
there is also a
link,
this time moreconcrete,
between differentialequations
and certain sheavesliving
in characteristic p. It would beinteresting
to find a mathematicaltheory explaining
thephilosophical
link observed above.5. FROM LOCAL TO GLOBAL
Proposition
5.1.- Assume that the local theorem 3.1 is valid. Let thefollowing
data begiven:
1) A compact
Riemannsurface
Xof
genus g.2)
Points pi,... pm on X with m > 1.3)
A vector space Vof
dimension n over C.4)
Analgebraic subgroup
G cGL(V),
such thatG/L(G)
istopologically generated by
2g + m -1
elements.Then there exists a
differential equation
overX, singular
at most at thepoints
pl, ..., pm,regular singular
at pl, ..., pm-l,having
a solution space, which isidentified
with V such that G CGL(V) is
thedifferential
Galois group.Proof.-
The function field of X will be denotedby
K. For apoint
p E X we denote the field of themeromorphic
functions at pby Kp.
First one chooses small
disjoint
disks around thepoints
pl, ... , pm. PutXt = X; i , ~ p2 ~ .
InX~
one chooses apoint
c. The fundamental groupc),
whereXo
=X B ~pl, ... ,
isgenerated by
al,bl, ... ,
ag,bg , Ai,..., Am
and has one relationalblallb11
...~1 ~ ~ ~ Am
= 1. The elementAm
is aloop
inX~
around pm and the other~i
areloops
around pl, ... , pm-i . The differential module over X is constructedby glue- ing
certain connectionsMo,..., Mm (with possibly singularities), living
above the spacesXo, ... , Xm.
Let pr : G ~
G / L( G)
denote the canonicalhomomorphism.
One chooses a homomor-phism
p : ~rl(Xo, c)
-~ G cGL(V),
such that thehomomorphism
prp has Zariski denseimage.
Consider thealgebraic
group G’ =prp(Am) »),
where « a » denotesthe
algebraic subgroup generated by
the element a. The group G’ containsL(G)
and soG’/L(G’)
istopologically generated by
theimage of p(Am) . According
to the Ramis’ localtheorem,
G’ is the differential Galois group of a differentialequation
over the fieldKpm.
One can extend this very local
object
to a differential moduleMm, living
aboveXm,
withonly
p~ assingular point.
The solution space at thepoint
c EXm
and the action of G’on this space can be identified with V and G’ C
GL(V).
Thetopological monodromy corresponding
toAm
can bearranged
to be E G’.The usual solution of the Riemann-Hilbert
problem (in
weakform) provides
a differen-tial module
Mo
aboveXo
such that themonodromy
action isequal
to p.The restrictions of
Mo
toX~
andMm
toX~
are determinedby
their local monodromies.These are both
equal
top(Am)
E G cGL(V).
Thus we have a canonical way toglue Mo
and
Mm
over the open subsetX~.
For eachpoint
can consider the restriction ofMo
toXi .
This restriction is determinedby
its localmonodromy
aroundthe
point
pi.Clearly,
the restriction ofMo
toXi
can be extended to a differential moduleM~
aboveXi
with aregular singular point
at pi.The modules
Mo, Ml,
...,Mm (or
rather thecorresponding analytic
vectorbundles)
are in this way
glued
to a vector bundle M above X. The connections can be writ- ten as V :Mo - S2x
0Mo,
V :Mi -+
®Mi
for i =l, ... ,
m - 1 and V :Mm -
®Mm
for a suitableinteger
d > 0. The connections alsoglue
to a connection V : M -
03A9X(p1
+... + + ® M. LetM*
denote the set of allmeromorphic
sections of M. ThenM*
is a vector space over K of dimension n witha connection V :
M* - OK/C 0 M*.
Thus we have found a differential module over K with the correctsingularities.
K has a naturalembedding
in the fieldKc.
The differential module is trivial overKc
and its Picard-Vessiot field PV over K can be seen as a subfieldof
Kc.
The solution space is V C PV CKc.
Finally
we have to show that the differential Galois group H CGL(V)
isactually
G.By
construction G’ cHand also theimage
of p lies in H. Thisimplies
that G C H.In order to conclude that G = H we can use the Galois
correspondence.
Thus we havefinally
to prove that an elementf
E PV CKc,
which is invariant underG, belongs
to K.Since G’ is
by
construction the differential Galois group ofMm
aboveXm,
we con-clude from the invariance of
f
under G’ thatf
extends to ameromorphic
solution of thedifferential
equation
aboveXm.
The invariance off
under theimage
of pimplies
thatf
extends to ameromorphic
solution of the differentialequation
aboveXo
UXm.
Thepoints
pl, ... , areregular singular
and any solution of the differentialequation
aboveX;, i =1, ... , m -1
extendsmeromorphically
toXi.
Thusf
ismeromorphic
on X andbelongs
to K.Remark.- For the case of X =
P~
and pm = oo, it ispossible
to refine the above reason-ing
to prove thefollowing
statement.Corollary
5.2.- Let G CGL(n, C)
be analgebraic
group such thatG/L(G)
istopolog- ically generated by
m -1 elements. Then there are constant matricesA1,
..., andthere is a matrix
A~
withpolynomial coefficients (all
matricesof
order n xn)
such thatthe matrix
differential equation
has
differential
Galois group G cGL(n, C).
This result is close to the one of
Mitschi-Singer.
We note however that there seems to be no bound on thedegrees
of the coefficients of the matrixAoo.
6. THE FORMAL THEORY
In this section the differential field is
k
:=C((z)).
The classification of differentialequations over K
is well known(Birkhoff, Turrittin, Malgrange, Levelt,
etal.).
We willpresent
this classification in a somewhat differentform,
which clarifies the connection with the differential Galois group. For this purpose we need a universaldifferential
extensionR of k
which can be defined as follows:(i)
The7~-algebra ~
has a differentiationextending
the one ofk.
(ii) Every
differential idealof R
istrivial, i.e.,
0 orR.
(iii) Every homogeneous
linear differentialequation
of order nover K
has a solution space inR,
which is a C-vector space of dimension n.(iv) R
is minimal in the sense thatR
isgenerated over k by
all the solutions and theirderivatives of all
homogeneous
linearequations
overK.
For any differential field one can show that there exists an universal differential extension
(as above).
Moreover one can show that this extension isunique
up to differential iso-morphism.
Theinteresting thing
is that one can write down this extensionexplicitly
inthe case of
K.
We introduce first some notations: 6 is the derivation
z1;.
We will writef’
forz1;I.
Put Q
= TheK-algebra R
isrepresented by generators
and rela-tions as follows.
R
={e(q)}qEQ, lJ
and the relations are:za+b = e(ql
+q2)
=e(q1)e(q2)
and za = za EK
for a E Z.The
differentiation
onR
isgiven by:
(za)’ = e(q)’ =
~’ = l.The intuitive
interpretation of is:
za is the function l is the function
log(z)
ande(q)
is the functionIn sectors at the
point z
= 0 thisinterpretation
makes sense and can be combined with thelifting
of certain formal Laurent series inK
to actualmeromorphic
functions on asector.
Some
differential automorphisms of R/K:
The
formal monodromy ,
is the differentialautomorphism
of/
definedby:
,~,(za)
=e27ria za
and - ~ -~-27ri,
in
particular
the actionof q
on thealgebraic
closure ofK
andon Q
is defined.=
The
exponential
torusHom(Q, C*)
acts as a group of differentialautomorphisms
ofFor an element c of this group, one defines the differential
automorphism
cby
cza =
za,
cl =l, ce(q)
=c(q)e(q).
It is
possible
to write down all the differentialautomorphisms
ofR/K.
This has the struc-ture of an affine group scheme over C. The
subgroup generated by
the formalmonodromy
and the
exponential
torus is a densesubgroup
in a certain sense. For our purposes the formalmonodromy
and theexponential
torus will suffice.The
triple (V,
associated to adifferential equation
overK.
Let
L(y)
= 0 be ahomogeneous
differentialequation
of order n overK.
Put V :={r
ERI L(r)
=0},
the solution space of L inR.
Then V is a vector space over C of dimensionn. The set V is invariant under the actions of the formal
monodromy
and theexponential
torus. Let ’v denote the restriction
of 7
to V.Put Vq
:= V ~ K[{za}a~C,l]e(q). Then for almost all qE Q
the vectorspace Vq
= 0. One has further V =~q~QVq
and =%q
for
all q
EQ.
This defines thetriple (V,
associated to the differentialequation
over
K.
The
important
observation is:The
differential equation
overk
isequivalent
to the associatedtriple (V, {Vq}, w).
We will make this statement more
precise by considering
thecategory Gri,
whose ob-jects
are thetriples (V, {Vq}, satisfying:
(i)
V is a finite dimensional vector space overC, (ii)
is afamily
ofsubspaces
such that V =®Vq.
(iii)
~y~ is a C-linearautomorphism
of V such that =Vyq
for all q EQ.
One can
give Gri (in
an obviousway)
the structure of a(neutral)
Tannakiancategory.
Let
Diff
denote the Tannakiancategory
of the differential modules overk.
Proposition
6.1.- The above construction is anequivalence
between the Tannakian cat-egories Diff
andGr1.
Corollary
6.2.- Let thetriple (V, {Vq},
be associated to thedifferential equation L(y)
= 0 overk.
Then thedifferential
Galois group Gof
L can beidentified
with the al-gebraic subgroup of GL(V) generated by
~yy and the actionof
theexponential
torus on V.Examples
6.3 : TheAiry equation
The
Airy equation y"
= zy has asingular point
at z = oo. Thetriple
associated to theequation
is V =Vz3/2 ® V_z3/2.
The two spacesVz3/2, V_z3/2
have both dimension l.After a suitable choice of bases for the two spaces the formal
monodromy
has the matrix0 }
and theexponential
torus has the form~ I t E C*~.
The differ- ential Galois group is therefore the infinite Dihedral groupDoo
CSL(2).
The information in this section on the formal differential Galois group suffices to
give
a
proof
of the"easy
halves" of the theorems.Proposition
6.4. The easyimplications
for the local and theglobal
theorem.-(1)
LetG be the
differential
Galois groupof
anequation
over thefield C({z}).
ThenG/L(G)
istopologically generated by
one element.(2)
Let X be acompact
Riemannsurface of
genus g, S ~ X afinite
subset withcardinality
m > 0 and G thedifferential
Galois groupof
adifferential equation
over Xwith
singularities
in S. Then the naturalhomomorphism S, *)
-~G/L(G)
hasdense
image.
Proof.- (1)
The groupG’/L(G’)
isaccording
to section 2 also the differential Galois group of someequation y’ = Ay
overC({z}).
The differential Galois group H of thisequation
over
C((z))
is asubgroup
ofG/L(G).
The latter group has a trivial maximal torusand thus the
exponential
torus is notpresent
in H. Therefore the differentialequation
is
regular singular
and isequivalent
tozy’ - By
where B is a constant matrix. It is well known that the differential Galois group(either
overC({z})
or overC((z)) )
is thealgebraic subgroup
ofGL(n) generated by e2"iB.
(2)
Let K denote the function field of X. The groupG/L(G)
is the differential Galois group of a matrixequation y’
=Ay
over X which has itssingularities
in the set S. As in(1),
it follows that theequation
hasonly regular singularities.
Take apoint
c E XB
Sandlet V be the space of the local solutions of the
equation.
The Picard-Vessiot field L can be identified with the subfield ofK~ generated by
K and(the
coordinates of the elementsof)
V. The
monodromy of y’
=Ay
onX ~ S
induces ahomomorphism S, c)
-~GL(V).
The
image
of thishomomorphism
lies inG/L(G).
Letf
E L be invariant under thisimage.
Thenf
extends to ameromorphic
function on XB
S. Since thesingularities
ofy’
=Ay
areregular singular, f
extends to ameromorphic
function on all of X. Thereforef
E K. From the Galoiscorrespondence
we draw the conclusion that theimage
ofS, c)
inG/L(G)
is Zariski dense.7. THE ANALYTIC LOCAL THEORY
In this section the differential field K is
C({z}).
For notational convenience we take the derivation 6 to beb( f )
=f’
= For thedescription
of the differential modules over K we introduce a secondcategory Gr2.
First we will need some notation. Let d E R and 0. Then d(or
rathereid)
is considered as a direction at thepoint z
= 0.The
front o f q,
in notationFr (q),
consists of the d’s such that the function h :=eJ
has maximal decrease in the direction d. In other words has maximal decrease whenr > 0 tends to zero. For the
example
q =z-1
one finds = and the frontFr(z-l)
is thus 7r + 27rZ. For any q EQ,
one denotes theprojection (along
theother
by
prq.Using
thisterminology
we can define anobject (V, StV,d)
ofGr2
as follows:(1) (V, {Vq}, qv)
is anobject
ofGrl.
(2)
Forevery d
E R there isgiven
anautomorphism StV,d
of V of the formwhere
Nq2,Ql
is a C-linear mapV ~~2 Vq2 -~ Vql
C V.(3)
TheStV,d
shouldsatisfy
the relation = The are seen to beunipotent
maps.If
(V, {Vq~,
is fixed then there are modulo 2~ronly finitely
many d’s such that there exists q2, ql with d EFr(q2 - ql)
andVq2 ~ 0,
0. Thepossibilities
for theStV,d
form thus a finite dimensional vector space over C.
Morphisms
between twoobjects
are C-linear mapspreserving
all the data. The tensorproduct
of twoobjects
V =(V, {Vq},
qv,Stv,d)
and W =(W, {Wq},
qw,StW,d)
is definedas the vector space V 0 W with the data:
(v
0W)q
=Wq2.
= iv ® ’Yw and
=
StV,d
®Stw,d.
One can show that
Gr2
is a neutral Tannakiancategory
over C. LetDiffK
denote theTannakian
category
of the differential modules over K =C({z}).
The main results of Martinet and Ramis on multisummation can now bephrased
as:Theorem 7.1.- The multisummation
operator provides
anequivalence
between the Tan- nakiancategories DiffK
andGr2.
Corollary
7.2.- Let L be a linearhomogeneous differential equation
over K and let(V, {Vq},
yy,Sty,d)
denote theobject of Gr2
associated to L. Then thedifferential
Galoisgroup
of
L can beidentified
with the Zariski closureof
thesubgroup of GL(V) generated by:
(1)
Theformal monodromy
~yv.(2)
Theexponential
torus.(3)
The collection{Stv,d},
called the Stokes matricesof
L.Remark.- It must be stressed that the theorem and the
corollary
are at the heart of thetheory
of multisummation and form moreover the essentialpart
of theproof
of Ramis’local theorem.
The
category Gr3
The
categories Grl
andGr2
were introduced in[PI]
in order to obtain a nice andcompact
formulation of the work of Martinet and Ramis. A furtherreformulation,
dueto
Ramis,
willsimplify
theproof
of the local theorem even further. Thecategory Gr3
isdefined
by:
the
objects
aretuples (V, {Vq},
qv,stv,d)
with(1) (V,
is anobject
ofGrl.
(2)
For every d E R there isgiven
astv,d
E(3)
Thestv,d
shouldsatisfy 03B3-1V stV,d03B3V
=We
identify,
asbefore,
with a linearsubspace
ofEnd(V).
A mor-phism f : (V, {Vq}, stv,d)
~(W, {Wq},
qw,stw,d)
is a linear map V -3 Wsatisfy- ing f(Vq)
CWq,
= ~yw of, f
ostv,d
=stw,d
of.
The tensorproduct
of twoobjects (V, {Vq}, (W, {Wq}, stw,d)
is the vector space V ® W with the data(v®W )q
- =’Yv®’Yw and =stV,d~idW+idV~stW,d.
It is
easily
seen thatGr3
isagain
a neutral Tannakiancategory.
Infact,
the Tannakiancategories Gr2
andGr3
areisomorphic.
Lemma 7.3.-
(1)
Theexponential
map induces anequivalence of
Tannakiancategories Exp : Gr3 --~ Gr2.
(2)
Let theobject (V, {~}, stv,d) be
associated to adifferential equation
overC({z~).
Then the
differential
Galois group G CGL(V)
is the smallestalgebraic subgroup
such that:(a)
Theexponential
torus and TVbelong to
G.(b)
AllstV,d belong to
the Liealgebra of G.
-Proof.-
Theexponential
map associates to(V, ~Vq~, stV,d)
theobject (V, ~Vq}, Stv,d)
with
Stv,d
=exp(stv,d).
It iseasily
seen that this results into anequivalence
of Tannakiancategories.
The secondpart
of the lemma is a reformulation of 7.2.Multisummation and the Stokes matrices
Consider a differential
equation L(y)
= g over K andwith g
E K. Letf E k
be aformal solution of the
equation.
The main theoremo f
theasymptotic theory o f differen-
tial
equations
states that for a sector S at 0 with smallenough opening,
there exists ameromorphic
functionf
on S withasymptotic expansion f
and stillsatisfying L(/)
= g.In
general
thisf
is notunique.
Multisummationproduces
aunique
choice for thef
above.For d E R one considers the direction
eid
at 0. There are, modulo27rZ, finitely
manysingular
directions d for the differentialequation L(y)
= g. For a directiond,
which isnot
singular,
there is a multisummationoperator Sd
which maps a formal solutionf
to asolution of the
equation,
which lives on a certain sector with bisector d and hasf
asasymptotic expansion.
Ingeneral depends
on the choice of d. This isusually
calledthe Stokes
phenomenon.
HoweverSd( f )
does notdepend
on d E(a, b)
if this interval does not contain anysingular
direction.Let d be a
singular
direction. Then we defineSd+ ( f )
andSd- (/)
as andfor E > 0 and small
enough.
The difference betweenSd+ ( f )
and is measuredby
the Stokes matrix
StV,d.
We will make this moreprecise.
Let M be a differential module over K =
C({z~).
The solution space V is definedas V =
ker(a, R
Q9KM).
Thering R
isgiven
a basisover K
=C((z)),
e.g.zalne(q)
with a E C and 0
Re(a)
0and q
EQ.
Further M can begiven
a basis over K.
Combining
this one obtains a basis ofR
Q9K M overK.
The elements v E V can be written as finitesums £
with/~
i EK.
Thef
are formalsolutions of a set of
(inhomogeneous)
linear differentialequations
over K. For a directiond,
which is notsingular,
one definesSd(V)
as whereintd(Bi)
is the in-terpretation
ofB~ (this
involves za and thelogarithm)
in the direction d. There resultsa C-linear
bijection Sd :
V -Sold,
whereSold
is the vector space of the solutions ofM on a suitable sector
containing
the direction d. For any directiond,
there are twoisomorphisms Sd+ , Sd- :
V -~Sold.
One definesStv,d
= EGL(V). Clearly
is the
identity
if d is not asingular
direction. It is not difficult to prove that theobject (V, ~Vq~, belongs
to thecategory Gr2,
and that multisummationproduces
infact a functor
F2 : DiffK
-Gr2
of Tannakiancategories.
Theproof
of7.1, i.e., proving
that
F2
is anequivalence
ofcategories,
is rather involved(see [P3]
and[R2]).
The relation between the formal and the
topological monodromy
Let the differential module M over K be
given
withF2 (M) = (V, ~Vq~, Sty,d).
Let0
di d2
...dm
27r denote thesingular
directions(in
fact for the differential moduleHom(M, M)) lying
in[0, 2~r).
Thetopological monodromy
~yM of M iseasily
seento
satisfy (up
toconjugation)
the formulaExamples
7.4 : TheAiry equation,
continuedWe consider
again
theAiry equation y"
= zy. There are twosingular
directions d =0,
~rmodulo 27rZ. The
topological monodromy
is trivial and the formalmonodromy
is not triv-ial. The formula for the
topological monodromy implies
that both Stokes matricesStv,o
and are different from 1. The two matrices have the
form O1 1 * j and
with
respect
to thedecomposition
V =Vz3/2 ® V_z3/2.
It follows from 7.2 that the differ- ential Galois group of theAiry equation
overC(z)
isSL(2).
The same
argument
shows that the differential Galois group of anyequation y"
= ry with r GC(z~
apolynomial
of odddegree
isSL(2).
8. THE PROOF OF THE LOCAL THEOREM
The
following
lemma will bea.guide
for the construction of a suitableobject
in thecategory Gr3.
The data
V is a finite dimensional vector space over C and G c
GL(V)
is analgebraic subgroup.
T denotes a maximal torus and
g, t
cEnd(V)
are the Liealgebras
of G and T.The action of T on V
yields
adecomposition
V = where the X~ are distinct characters of T and the non-trivial spacesVx;
are defined as{v
EVI tv
=Xi(t)V
for allFor each