A NNALI DELLA
S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze
M AKOTO N AGATA
A generalization of the sizes of differential equations and its applications to G-function theory
Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 4
esérie, tome 30, n
o2 (2001), p. 465-497
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A Generalization of the Sizes of Differential Equations
and its Applications
toG-Function Theory
MAKOTO NAGATA
Vol. XXX (2001),
Abstract. The aims of this paper are to introduce a generalization of the notion of the sizes and to present its some applications to G-function theory. We define
a new size a(A, B) and estimate it. Furthermore we consider some relations in G-function theory by using our sizes.
Mathematics Subject Classification (2000): 12H25 (primary), 11 S99 (seconda- ry).
Introduction
In
1929,
C. L.Siegel [16]
introduced the notion of G-functions: theoriginal
definition is as follows.
A function
f (x) - aixi
is called a G-function if there exists analgebraic
number field K of finitedegree
and apositive
constant C with thefollowing properties (i)-(iii)
for all i :(i)
ai EK,
(ii)
the absolute valuesof ai
and itsconjugates
do not exceedCi,
(iii)
there is apositive integral
common denominator of which does not exceedCi.
Twenty
years ago A. I. Galochkin[9,
Definition2]
mentioned a relation between a differentialequation
and its G-function solutions. Heproposed
so-called Galochkin’s
condition,
which is anassumption
about the coefficients of the differentialequation.
Under thiscondition,
he obtained bounds of the irrational measures of thespecial
values of G-functions.After some years, E. Bombieri
[3]
defined the notion of arithmetictype,
andsuggested
to theequivalence
between the conditions of Galochkin and those of himself. He also obtained someirrationality
statements aboutspecial
valuesof G-functions which are solutions of differential
equations
of arithmetic type.Pervenuto alla Redazione il 20 marzo 2001.
In
1985,
D. V.Chudnovsky
and G. V.Chudnovsky [6]
showed that:THEOREM A.
If a
solutionof an
irreducibledifferential equation
is aG-function,
then the
differential equation satisfies
the Galochkin condition.In other
words, they
removed the Galochkin condition from the statements aboutirrationality, completing Siegel’s
program.A G-function is an
interesting topic
in itself. Y. Andr6[ 1 J proved
thefollowing
two theorems:THEOREM B. The Galochkin condition and the arithmetic type condition
for
adifferential equation
areequivalent.
THEOREM C.
If a
Fuchsiandifferential equation
withonly
rational exponents at theorigin satisfies
Galochkin’s condition, then the entriesof the
normalizeduniform
part
of
its solution matrix areG-functions.
In
1994,
B.Dwork,
G. Gerotto and F. J. Sullivan[8]
obtained the converseresult to Theorem C
by using
Chudnovskies’ and Andr6’s results:THEOREM D.
If the
entriesof the
normalizeduniform
partof the
solution matrixof
a Fuchsiandifferential equation
withonly
rational exponents at theorigin
areG-functions,
then thedifferential equation satisfies
Galochkin’s condition.Let K be a number field of finite
degree.
We consider the differential
equation:
with A E
Mn (K (x)).
The sizes and the
global
radii of the function y and the coefficient ma-trix A of differential
equation (0.1)
are denoted asa(y), a (A), p(y)
andp (A) respectively (definitions
asbelow).
When one uses thesenotations,
"differential
equation (0. I )
satisfies Galochkin’s condition"is
equivalent
tocr (A)
oo,"differential
equation (0.1)
is of arithmetictype"
isequivalent
top (A)
oo.The above theorems A-D are the statements on the sizes and the
global
radii.So,
our interest concerns the finiteness and the values of the sizes and theglobal
radii.
In this paper we introduce a
generalization
of the notion of the sizes andpresent
someapplications
of it to relations between sizes. This paper isarranged
in two
chapters
as follows:(I)
We consider the differentialequation:
with
A,
B EMn (K (x)).
We attach to
(0.2)
a sizeB)
whichgeneralizes
the usual size(corre- sponding
to the case B =0).
The
following proposition
forB)
holds.THEOREM I. Let
cr (A, B)
:=B)
+cr (B, A)) for A,
B EMn (K (x)).
Then the map
is a
pseudo
distancefunction.
Moreover(II)
We estimatea(A, B)
of differentialequation (0.2).
THEOREM Il- 1. Let u := E
OK [x ]
be a common denominatorof
Aand B such that
u A,
u B E whereOK
denotes theinteger ring of
K.Lets :=
max(deg
u,deg(uA), deg(u B)). Then for
a solution X EGLn (K [[x]]) of differential equation (0.2)
with = I(the identity matrix),
we havem+1 2:vlOO maxi:::m log max(l,
vbeing places of K.
To state an
application
of thistheorem,
we putand
Here A E and T E
GLn(K(x)).
According
to[ 1 ],
there exists such thatand that none of the differences between the
eigenvalues
ofRes(T [A])
is a non-zero
integer. By fixing
such T EGLn (K (x)),
there exists theunique
solutionY E of the differential
equation:
with
Yl,=o =
I. We call thisunique
solution of differentialequation (0.3)
the normalized
uniform
part of solution of differentialequation (0.1). Indeed, T-1 Y xRes(T[A])
is a matrix solution of differentialequation (0.1).
We now state an
application
as thefollowing corollary,
which is aquanti-
tative version of Theorem D without
using
Shidlovskii’s lemma[1, Chapt. VI,
Sect.
2]:
COROLLARY 11-2. Let A E and let Y be the normalized
uniform
part
of
the solutionof differential equation (0.1)
with above T EGLn(K(x)).
Letu
be a common denominator of T [A],
andlets:= max(degu, deg(u T [A])).
Suppose
that9 :=
{eigenvalues of
Then
where
N,,
E ~T is a common denominatorof E.
Notation and
terminology
We fix K as a number field of finite
degree.
For aplace
v of K weput
where d =
[K : Q] [Kv : QJ.
We define a
pseudo
valuation onMnl,n2(K),
the set of nl x n2 -matricesof usual: for M = e ’
For
Yi
E we consider the Laurent series Y = EWe write
log+ a (a
E Andre’ssymbol
in[I], h.,.(.),
is defined
by
DEFINITION
(Cf. [1, Chapt. I]).
We define the size of Y EMnl,n2 (K((x)))
asand the
global
radius of Y aswhere
L:v
means that v runs over allplaces
of K.The
following
definition isequivalent
to the conditions(i), (ii), (iii)
inintroduction in the case of Y E
K[[x]]. (Cf. [1, Chapt. I])
DEFINITION. We say that Y E
Mn¡,n2(K«x»)
is a(matrix of) G-function(s)
if oo.
For
f
=f (x ) = EN 0 f¡xi E K[x]
and for everyplace v
ofK,
the Gaussabsolute value is defined
by I f 1, := maxi=O,...,N If¡ I v.
From here we discuss
only
non-Archimedeanvaluations,
thatis, v f
oo.For every
place
v withv t
oo and forf,
g EK[x]
withg ~ 0,
the Gauss absolute value is extended toK (x) by
We also define a
pseudo
valuation onMn(K(x))
as before: for M =Henceforth D denotes the differential operator
§ .
From[ 1, Chapt. IV,
Subsect.
1.5]
we have . ----for m =
0, 1,
.... Here v is anarbitrary
non-Archimedean valuation of K and M EM,, (K (x)).
For a sequence
{ Fi } i =o,1, ...
CMn ( K (x ) )
and for everyplace v t
oo, we putDEFINITION. We define the size of C
M,,(K(x))
asand the
global
radius ofI Fi I
aswhere
Lvfoo
means that v runs over all finiteplaces
of K.Chapter
1: the sizes of differentialequations
1.1. - Notation
We introduce our
original symbols
and definitions.Let K be a differential extension of K.
Suppose
that3~,
flt, ~ are elementsin
Mn(K).
A sequence{(3~, 2!, ~) ~‘~ }1=0,1,...
C is definedby
and
recursively
for i =1, 2, ... ,
We write
21, ~) (resp. p (3, 21, ~) )
as an abbreviationfor a (1 (3, 21, ~) ~‘ ~ } ) (resp. p (f (J,
21,~8) (’) 1)) -
DEFINITIONS 1.1.1. For the differential
equation
with A E
M,,, (K (x)),
we0, A) (= a(I, A, 0),
See Subsect. 1.2below)
the size of A
(or
of differentialequation ( 1.1.1.1 ))
andp (1, 0, A ) (= p(I, A, 0))
the
global
radius of A(or
of differentialequation (1.1.1.1»,
where I is theidentity
matrix and 0 is the zero matrix inMn ( K (x ) ) .
The
following
definition coincides with that of Andr6[ 1, Chapt. IV,
Sub-sect.
5.2].
DEFINITION 1.1.2. We say that
(D - A)
is aG-operator
if andonly
ifor(/,0,A)
oo.REMARK l.1.3
(Cf. [I], [3]).
Differentialequation (o.1 )
withp (I, 0, A)
0o is called
of arithmetic
typeby
Bombieri.1.2. -
Properties
of the sizes We define achange of basis
aswhere 3 E and A E One
immediately
obtains:PROPOSITION 1.2.1.
For)1,)2
EGLn(K(x» and for A
EM,, (K (x)),
we haveThe main purpose of this section is to show the
following proposition:
PROPOSITION 1.2.2.
For 3, J2
EGLn (K (x)) and for A, B,
C EM,, (K (x)), the following
statements hold.We shall often write
simply a(A, B)
instead ofcr(7, A, B).
We define afunction on
by
The
following
statements show its characteristicproperties,
andgive
The-orem I in Introduction.
THEOREM 1.2.3. The map
is a
pseudo
distancefunction,
that is, itsatisfies the following
three conditions:and
Moreover we have
and
PROOF. The assertions
(1.2.3.1), (1.2.3.2)
and(1.2.3.3)
are trivialby Propo-
sition 1.2.2. As for the identities
(1.2.3.4),
we use theidentity (1.2.2.3)
inProposition
1.2.2. Then we haveFinally
for theidentity (1.2.3.5),
weapply Proposition
1.2.1 and the identi- ties(1.2.2.2)
inProposition
1.2.2. Then we haveTherefore
8 (A , B)
=J[B]).
0REMARK 1.2.4. One defines an
equivalence
relation A - B inMn(K(x))
as
8(A, B)
=0,
then a metric is induced as usual. However it is not known what thisequivalence
relation A - B means. Forinstance,
even in the caseof A -
0,
we do not know whether therealways
exists 3‘ E suchthat A =
3[0].
Theequality
A =3[0] implies
that all solutions of differentialequation (0.1) belong
toMn(K(x)). (Cf. [1, Chapt. IV,
Subsect.4.2]).
Our
proof
ofProposition
1.2.2requires
somepreparatory propositions,
which are results
concerning
theproperties
of the sequence{ (~, A, B ) ~‘ ~ { .
Weshall use them later
again.
LEMMA 1.2.5. For J E
GLn (K (x)), A,
B EMn (K(x)) and for m
=0, 1, ... ,
we have
PROOF. We show the
identity (1.2.5.1) by
induction on m. For m =0,
both sides of theidentity ( 1.2.5.1 )
are J thus it is true in this case. Assume that theidentity ( 1.2.5.1 )
is true for agiven m >
0. We now prove it for m + 1. We differentiate each side of theidentity (1.2.5.1).
Because =we have
On the other
hand,
Therefore we find that
A similar argument
yields
theidentity ( 1.2.5.2).
0LEMMA 1.2.6.
For sequences {ai
C L
and for
m =0, 1,
...,PROOF. Obvious. 0
LEMMA 1.2.7.
For 3‘1, ’12, J3, A,
B E C EK and for m
=0, 1,...,
we havePROOF. We show the
identity (1.2.7.1) by
induction on m. For m =0,
both sides of theidentity (1.2.7.1)
are:YI3293
thus it is true in this case. Assumethat the
identity ( 1.2.7.1 )
is true for agiven m >
0. We now show it for m + 1.We differentiate the left side of the
identity ( 1.2.7.1 ).
We haveWhere
((3‘2, A, B)(1), A, B) (i)
=(i
-I-1)(J2, A,
can be shownby
induc-tion.
On the other
hand,
the differentiatedright
side of theidentity ( 1.2.7.1 )
isTherefore we obtain that
by
Lemma 1.2.6. 0LEMMA 1.2.8.
For 31, 32, A, B,
C Eand for
m =0, 1,
...,PROOF. We show the
identity (1.2.8.1) by
induction on m. For m =0,
bothsides of the
identity ( 1.2.8.1 )
areJiJ2
hence it is true in this case. Assume that theidentity ( 1.2.8.1 )
is true for agiven
m > 0. We now prove it for m -E-1.We differentiate the
right
side of theidentity ( 1.2.8.1 ).
Then we haveThe last
expression
isequal
to the differentiated left side of theidentity ( 1.2.8.1 ),
Therefore
We now prove
Proposition
1.2.2.PROOF OF PROPOSITION 1.2.2. First we show the
identity (1.2.2.1).
It isclear that
Therefore
or(/, A, A)
= 0.For the
proof
of(1.2.2.2),
assume that thefollowing
identities hold:and
We
substitute J[B]
for B in theidentity (1.2.9.1)
and3-1 [A]
for A in theidentity (1.2.9.2).
Thenusing Proposition 1.2.1,
we obtain thatand
hence we conclude the identities
(1.2.2.2).
It suffices to show the identi- ties(1.2.9.1)
and(1.2.9.2).
We prove theidentity (1.2.9.1). Using
the iden-tity (1.2.5.1)
in Lemma1.2.5,
we findfor every
place v with v t
oo. HenceThe number of
places
v with vfi
oo such thatI:Jlv :0
1 is finite and it followsthat -
It
yields
On the other
hand, by
theidentity ( 1.2.5.1 )
in Lemma1.2.5,
we also findfor every
place v with v f
co. Hence we have as aboveConsequently
we obtain theidentity ( 1.2.9.1 )
from theinequalities (1.2.9.6)
and
(1.2.9.8).
As for theidentity (1.2.9.2),
one finds it in a similar way.Next we show the
identity (1.2.2.3).
Because of theidentity ( 1.2.7.1 )
forc =
0, ~3
= I and B = 0 in Lemma1.2.7,
we havefor every
place v
withv f
00. ThusIt follows
The number of
places
v with v~’
oo suchthat
finite and itfollows that -
Therefore we obtain
We also have
Consequently
we deduce theidentity (1.2.2.3)
from(1.2.9.11)
and(1.2.9.12).
We conclude this
proof by showing
theinequality (1.2.2.4). By
Lemma1.2.8,
one has
Then we obtain
The statements for the
global
radii instead of the sizes inProposition
1.2.2and Theorem 1.2.3 hold
similarly.
PROPOSITION 1.2.10.
For ’1, :y2
EGLn (K (x)) and for A, B,
CE Mn (K (x)), the following
statements hold.THEOREM 1.2.11. Let
Then the map
is a
pseudo
distancefunction.
Moreover we haveand
Chapter
2: estimations of the sizesIn this
chapter
we consider a relation of differentialequation (0.2)
and itssolution.
2.1. -
Diophantine approximations
We assume that X E
GLn(K[[x]])
with = I is a solution of differ- entialequation (0.2).
Hence forA,
B EMn ( K (x ) )
Moreover we write
for q
EK[x]
and P E R :=qX -
P EIn this
section,
we show someproperties
of simultaneousapproximations
of the solution X.
The
following
lemma isfundamental.
PROOF. We show the
identity (2.1.1.1 ) by
induction on m. For m =0,
both sides of theidentity (2.1.1.1 )
are P and it is true in this case. Assume that theidentity (2.1.1.1 )
is true for agiven m >
0. We now prove it for m + 1. One hasSince
(X, A, B ) ~ 1 ~
= DX - A X + X B =0,
we obtainNOTATIONS 2.1.2.
Throughout
this section and the next, we denoteby N,
Larbitrary integers
such thatand
Moreover for
A, B
EMn ( K (x ) ),
we write u Eas
a common denominator of A and B ands :=
max(deg u, deg(uA), deg(uB)) ,
where
OK
is theinteger ring
of K.LEMMA 2.1.3. For m =
0, 1,...,
L,and
PROOF. We show the four assertions
by
induction on m. For m =0,
we have(P, A, B)~°~
=P, deg
PN, (R, A, B)~°~
=R, ordo R >
L and then(2.1.3.1), (2.1.3.2), (2.1.3.3)
and(2.1.3.4)
are true in this case. Assume that these four assertions are true for agiven m >
0. We prove them for m + 1. Now one hasor
Substituting
the lastequation
intowe have the
right
side of theidentity (2.1.3.6)
hence
By
the inductionassumption,
we find that every term of theright
side of the lastequation belongs
toMn(K[x]).
HenceMoreover
by
theidentity (2.1.3.7)
we findSimilarly
we haveBy
the inductionassumption,
we find that every term of theright
side of the lastequation belongs
toMn ( K [ [x ] ] ) .
HenceBy
theidentity (2.1.3.10)
we findDEFINITIONS 2.1.4. For Z = we write
with
m = 1, 2, ....
Moreover we writeand
For Z E we write
and
For Z E one obtains
immediately
thatLEMMA 2.1.5
(Siegel’s
lemma[3]). Let DK
be the discriminantof
K. Letd =
[K : Q]
and y =Suppose
that M N with M, N E N.Then for
the system
of
linearequations
withcoefficients
in Kthere exists a non-trivial solution
fxi I
C K such thatwhere
Ev
means that v runs over allplaces of
K.PROOF. See
[3, Siegel’s lemma].
LEMMA 2.1.6.
Suppose
thatN, satisfy
Then for
X =Xixi
EGLn(K[[x]])
withXlx=o
= I, there exist non-zero q and P with q EK [x]
and P EMn (K [x])
whichsatisfy the following properties:
and
Here y is the constant as in Lemma
2.1.5, depending only
on K.PROOF. We show the existence of q and P
satisfying
these conditions. PutIf q (0 # q
EI~ [x ] )
satisfiesdeg q N,
then one hassince
Xo -
I. Now wewrite q = qixi
EK[x].
The condi-tions
(2.1.6.3)
and(2.1.6.8) require
thatThe system of linear
equations (2.1.6.10)
has Nunknowns,
~0~1."- qN-i, andn2 (L - N) equations.
The condition(2.1.6.1) gives
N >n2 (L - N)
andthen from Lemma 2.1.5 there exists a non-trivial solution
f qo, q 1, - - - ,
of
(2.1.6.10)
withTherefore we conclude the existence of
0 # q
EK [x)
withdeg q
Nsatisfying
the condition
(2.1.6.4).
We also haveand
Therefore we conclude the existence of
0 ~
P EMn(K[x])
withdeg
P Nsatisfying
the conditions(2.1.6.5)
and(2.1.6.6).
Finally
we prove the assertion(2.1.6.7).
PutFrom the conditions
(2.1.6.1), (2.1.6.2)
and(2.1.6.3),
one hasThis
implies ordo q
=ordo
Pby (2.1.6.12)
andXjx=o
= I. Then2.2. - Proof of Theorem n-1
Here we prove Theorem II-1 in Introduction.
The
following inequality
isrequired
for ourproof.
LEMMA 2.2.1. For
f
EK [x] B {OJ,
we havePROOF. We take a root of
unity 4
such that 0. Put F : :=K (~ ) .
Let v be a
place
of K and w be aplace
of F. Forf
EK[x]
and for oo,one
has
orThe
product
formula in Fgives
Furthermore
for w I 00,
where
d F :
:=[ F : Q ], d F w :
:=[ Fw : Qw].
Therefore we obtainPROOF OF THEOREM II-1. Let N E N
satisfy
and put
where E E R with
0 E
1. As in Lemma2.1.6,
wechoose q
EK[x]
andP E
Mn (K[x])
flGLn (K (x))
withWe write as in Subsect. 2.1
R:=qX-P. By
Lemma 2.1.1 and Lemma 2.1.3we have
and
Hence for any m > 0 with
we obtain
On the other
hand, by
Lemma 1.2.8 we haveand
Moreover
by
theidentity ( 1. 2.7.1 )
for A =0,
c =0, 31
=?2
= I and~3
= Iin Lemma 1.2.7 we have
Therefore under the
hypothesis (2.2.2.6),
we obtainby
theequalities (2.2.2.7)- (2.2.2.10)
Let P denote the
adjoint
matrix of P. Then forv f
oo,By
Lemma2.2.1,
for u E we haveand
similarly
Moreover
Since u E
Substituting
theinequalities (2.2.2.13)-(2.2.2.16)
into theinequality (2.2.2.12),
we obtain
By
theinequalities (2.1.6.5)
and(2.1.6.6)
in Lemma2.1.6,
we findApplying
the lastinequalities (2.2.2.18)
to theinequality (2.2.2.17),
we deduceNow
by
the identities(2.2.2.2)
it is easy to see thatand
Then from Lemma 2.1.6 one has
The last
inequality
and theinequality (2.2.2.19) yield
The last
inequality
holds for msatisfying
theinequality (2.2.2.6).
For thevalidity
of theinequality (2.2.2.6),
we needby (2.2.2.2),
henceWe choose m as the maximal
integer satisfying
theinequality (2.2.2.22).
Thenor more
weakly
By
theinequality (2.2.2.1 ),
one hasWe recall the identities
(2.1.4.1)
after Definitions 2.1.4.By
the identities(2.2.2.2)
and the
inequalities (2.2.2.23),
each limit andis
equal to a(X)
and each limitand
vanishes.
Using
theinequalities (2.2.2.23),
weapply (or equivalently
to the
inequality (2.2.2.21).
Then we conclude2.3. - Proof of
Corollary
11-2Before
stating
aproof
ofCorollary 11-2,
we need the definition of the normalized uniformpart
of solution of differentialequation (0.1 ).
We use the notations as in and
Res(A).
Until the end of this
section,
assume that(2.3.0.1 )
everyeigenvalue
ofRes (A )
is containedin Q.
LEMMA 2.3.1
(Shearing
transformation[5]). Suppose that A
Esatisfies
the condition(2.3.0.1).
Let a be aneigenvalue of Res(A).
Then there existsTt
EGLn(K(x)) (resp. T2
E such that(2.3.1.2) T,
andTI-I 1 (resp. T2
andT2 1 )
have nopoles
except at theorigin
and that
(2.3.1.3)
the
eigenvalues of Res(Tl [A])
coincide with thoseof Res(A)
except( 2.3.1.3 )
the
eigenvalue
a isreplaced
a + 1(resp. a-I)
withmultiplicity.
PROOF. Since all
eigenvalues
are rationalnumbers,
there existsPi
EGLn (K)
such that
P, = Res(Pi [A])
is the upper Jordan normal form. Thenone can
immediately
obtain Lemma 2.3.1by
theprocedure
of[5, Proposi-
tion
2.3].
0Repeated application
of Lemma 2.3.1yields:
PROPOSITION 2.3.2.
Suppose
that A Esatisfies
the condi-tion
(2.3.0.1 ).
Then there exists T EG Ln (K (x ))
such that(2.3.2.2)
everyeigenvalue of Res(T[A])
is less than 1 and is not less than 0 and that(2.3.2.3)
T andT-1 have
nopoles
except at theorigin.
The
following proposition
is theuniqueness
of the solution of differentialequation (0.3).
PROPOSITION 2.3.3. Let A E
satisfy
the condition(2.3 .0.1 ).
LetT E
GLn (K (x)). Suppose
thatand that
(2.3.3.2)
none
of
thedifferences
between theeigenvalues of Res(T[A])
is a non-zero
integer.
Then there exists the
unique
solution Y EG L,, (K [ [x ] ]) of the differential equation:
with = I.
PROOF. See
[ 1, Chapt. III,
Subsect.1.4].
DEFINITION 2.3.4. Let A E For a fixed T e
GLn(K(x)) satisfying
the conditions(2.3.3.1 )
and(2.3.3.2),
we call theunique
solution Y EGLn(K[[x]])
of differentialequation (2.3.3.3)
with I the normalizeduniform part
of solution of differentialequation (0.1).
The
following
lemma isrequired
for ourproof.
LEMMA 2.3.5. Let A E
and put B := x Res(A). Suppose
thatThen one has
where
N,,
E I~ is a common denominatorof E.
PROOF. Let C E
Mn (K)
be the normal Jordan form ofRes ( A ) .
Then thereexists H E
GLn(K)
withHBH-1
=’C.
x SinceH[B] = lC,
x one hasby Proposition
1.2.2.Consequently
it isenough
to show thatNow we write
First we show
by
inductionfor m =
0, 1, ....
For m =0,
both sides of theidentity (2.3.5.5)
are I and it istrue in this case. Assume that the
identity (2.3.5.5)
is true for agiven m >
0.Then one has
Therefore the
identity (2.3.5.5)
holds. Next we handle two cases.CASE 1. v
f
oo with > 1. There existsonly
a finite number of suchcases.
Identity (2.3.5.5) gives
Since
we obtain
CASE 2.
v f
oowith
1. We haveLet
CD
denote thediagonal part
of C andCN
thenilpotent part
ofC,
hence C =CD
+CN. By
thecommutativity
ofmultiplication,
we find that(~)
isequal
to"’
Hence
by
=1,
one hasWe
put
a =aa /ba
withaa, ha
EZ, (aa ,
= 1 andba
> 0.By
a standardargument
(cf. [1, Chapt. I, Appendix])
one finds that thefollowing inequality
holds for
sufficiently large
m and for everyprime
pwith v p
in this case:where
¿vip
means that v runs over all finiteplaces
of K withv p.
Consequently
we obtainHere
7r(m)
is the number ofprimes
which are not greater than m and we usedthe
prime
number theorem. 13Finally
we obtainCorollary
11-2 as follows:COROLLARY 2. 3. 6. Let A E and Y be the normalized
uniform
part
of
the solutionof differential equation (2.3.3.3)
with T EGLn (K (x))
as inProposition
2.3.2. Let u, s be denoted as in Theorem II-1 withT [A]
insteadof
Aand B
= x Res ( T [A ] )
and e CQ N,,
as in Lemma 2.3.5. Thenx
PROOF. We choose T E
GLn (K (x))
as inProposition
2.3.2. Since eacheigenvalue
ofRes ( T [A ] ) corresponds
to one of theeigenvalues
ofRes(A)
mod
1,
we findby
Lemma 2.3.5Furthermore
by Proposition
1.2.2 we haveConsequently, by
theinequalities (2.3.6.2), (2.3.6.3)
and TheoremII-1,
we obtainREFERENCES
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