A NNALES DE L ’I. H. P., SECTION C
T OSIO K ATO K YÛYA M ASUDA
Nonlinear Evolution Equations and Analyticity. I
Annales de l’I. H. P., section C, tome 3, n
o6 (1986), p. 455-467
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Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
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Nonlinear Evolution Equations
and Analyticity. I
Tosio KATO and
Kyûya
MASUDA Department of Mathematics, University of California,Berkeley, CA 94720, U. S. A.
and
Mathematical Institute, Tohoku University. Sendai, 980 Japan
Henri Poincaré,
Vol. 3, n° 6, 1986. p. 455-467. Analyse non linéaire
ABSTRACT. 2014 We prove a theorem on abstract nonlinear evolution
equations otu
=F(t, u)
in a Banach space, which aims atestimating
certainfamilies of
Liapunov
functions for the solutions. The theorem is useful inproving global analyticity (in
spacevariables)
of solutions of variouspartial
differentialequations,
such as theequations
ofKorteweg de-Vries, Benjamin-Ono, Euler, Navier-Stokes,
nonlinearSchrodinger,
etc. In thispaper it is shown that if the initial state of the KdV or the BO
equation
has an
analytic
continuation that isanalytic
andL2
in astrip containing
the real
axis,
then the solution(which
isunique
in has the sameproperty
for alltime, though
the width of thestrip might
decrease with time.Key-words: Evolution equation, Liapunov function (family), Equations of (generalized) Korteweg de-Vries, Benjamin-Ono, Euler, Navier-Stokes. Sobolev space, Sobolev norm,
Taylor series, Radius of convergence.
RESUME. - On demontre un theoreme sur des
equations
d’evolution non-lineaires abstraites dans un espace deBanach,
visant a estimer cer- taines fonctions deLiapounov
pour les solutions. Ce theoreme sert a demontrerl’analyticité globale (en espace)
des solutions de diversesequa-
tions aux derivees
partielles.
On montre enparticulier
que si la condition initiale de1’equation
deKorteweg
de-Vries ou deBenjamin-Ono
aun
prolongement analytique L~
dans une bande autour de l’axereel,
alors la solution
(unique
dansH2)
a la memepropriete
a toutinstant,
bien que la
largeur
de la bandepuisse
decroitre avec le temps.Annales de Henri PnlllC’(!I’E’ - Analyse non linéaire - 0294-1449 Vol. 3 86 06 455 13 S 3.30 C Gauthier-Villars
1. LIAPUNOV FAMILIES
In what follows we consider nonlinear evolution
equations
of the formWe shall prove a theorem which is useful in
deducing
theanalyticity (in
space
variables)
of solutions of some nonlinearpartial
differentialequations.
The main
problem
here is to estimate the solutions that arealready
knownto exist and have
regularity
sufficient tojustify
various formaloperations.
Actually
it will bepossible
to construct atheory
in which existence andregularity (including analyticity)
can be establishedsimultaneously,
but itseems that such an
attempt
leads to undesirablecomplications.
In this section we prove the main
theorem,
which uses a classof Liapunov
functions
involving
aparameter.
Insubsequent
sections weapply
thetheorem to prove the
analyticity
of solutions of the(generalized)
KdV equa- tion and the BO(Benjamin-Ono) equation.
Othertypical
nonlinear equa-tions,
such as the Eulerequation,
the Navier-Stokesequation,
nonlinearSchrodinger equation,
etc. will be dealt with insubsequent publications.
It should be noted that our results do not prove
analyticity
in t; this is ingeneral impossible.
On the otherhand,
we do not assume thatF(t, u)
is
analytic
in t;only continuity
in t suffices. In thisrespect
our results resemble a theorem ofNagumo [7],
but differ from the latter inbeing
nonlocal.
We start with
preliminary
definitions and lemmas. All Banach spacesX, Z,
... considered below are assumed to be real. X* denotes the dual space of X.Let Z be a Banach space. We say a real-valued function 03A6 on an open subset O c Z is weak*
C~
if the Gateaux derivative DO exists with values in Z* and is demi * continuous from Z to Z*(i.
e. continuous fromstrong
Zto
weak * Z*).
We recall that the mean value theorem holds for c~ :provided
the segment L~v c O.Next suppose that we have another Banach space X =3 Z with the inclu- sion continuous and dense.
Suppose
further that DC considered above is demi * continuous(not only
from Z to Z* butalso)
from Z to X*.(This
statement makes sense since X* c Z*
by
canonicalidentification.)
Thenwe say C is
(Z, X)-weak* C1.
Finally
suppose we have ax ~-
of real-valued functions on O such that
~.( . )
is(Z,
onO,
whereAnnales de l’Institut Henri Poincaré - Analyse non linéaire
EQUATIONS
Z = R x
Z,
X = R xX, and Õ
=(- o-)
x O. We denoteby
the
partial
derivative in Z-variableonly.
LEMMA 1.1
(chain rule).
Letu( ~ O)
nC1(I ; X)
and~( ~ ) E C1(I ; f~)
with
6(t) ~ ~,
where I c R is an interval. Then~6~_~(u( ~ ))
EC1(I ; ~)
with(1.2) at ~~~~t~(u(t))~ _ ~ D~~(r~(u(t)) ~
+Proof :
We may assume that 0 E I. Weapply ( 1. 1 )
to the function~_( - )
on
( -
oc,a)
x O intoR,
with ureplaced by (r(0), u(0))
and vby (a(t), u(t)), obtaining
where M =
u(0)
+i (u(t)
-u(U))
and 03C3 =6(U)
+ -03C3(0));
note thatU E O
and 03C3
6 ifI t is sufficiently
small. If we divide(1.3) by t
and lett ~
0,
thent -1 (u(t) - u(0))
-~ in X andt - i {~(t) - ~(o))
~6’(0),
while
D~ ~{ u) ~ (weak * convergence)
in X* for each fixedh,
and
similarly
If[
tis sufficiently small, however,
U isarbitrarily
close tou(0)
inZ, uniformly
in a E[o, 1 ],
andsimilarly
for ~. Therefore and are
uniformly
bounded in X*by
the
demi * continuity. Application
of the bounded convergence theorem thus shows that(1.2)
is true for t = 0. The same is true for each t~I. Since theright
member of(1.2)
is continuousin t,
the lemma isproved.
REMARK 1.2. As is seen from the
proof,
Lemma 1.1 remains true if wereplace
all the t-derivatives involvedby
theright (or left)
derivatives.Thus
u(. )EC(I; O)n C1 +(I; X)
and03C3( . )~C1 +(I ; R) imply +(I; R),
where
C 1 +
indicates that theright
derivative exists and isright-continuous.
REMARK 1.3. - There are some
problems
in which we are not ableto construct the
family
with therequired continuity properties
but inwhich it is still
possible
to find a substitute functionth6
that satisfies theinequality
obtained from(1. 2) by replacing == by
x . Such a function willserve the same purpose.
We now define a
Liapunov family
for(E), assuming
that F is continuouson IT x O to
X,
where IT =[0, T],
T > 0. ALiapunov family {03A603C3; - ~
7 03C3~ }
for(E)
on O is afamily
of real-valued functionson O
satisfying
thefollowing
conditions.03A6(.)
is( -
x,r)
x O into !R andwhenever reO with r, where 03B1(r), 03B2(r) are real-v alued continuous
Vol. 3. n° 6-1986.
458 AND K. MASUDA
functions defined for - x~ r Y It is assumed
(for simplicity)
that
a(r)
~ 0. Note that the left memberof (1. 4)
makes sense sinceF(t, L,)
E Xand E X*.
Given a
Liapunov family { ~~ ~
for(E)
onO,
wesay §
e Ois { D~
sible if there is b r such that
r. If ~ is ~ ~~ }-admissible,
we can solvethe
ordinary
differentialequation
We denote
by p(t)
the maximal solution of( 1. 5) (in
the sense ofvalues,
not of the interval of
existence),
which exists on a certain intervalITI, Ti
> 0. Then we define another function7 also exists on
IT1
and satisfies6(t)
6(recall
that 0 and br).
With these
definitions,
we can state the main theorem.THEOREM 1. - Let O c Z c X be as above. Let F be continuous on
IT x O into X. Let
2 ~~ ; - :r
a6 ~
be aLiapunov family
for(E)
on
0,
so that we haveinequality (1.4)
with certain continuous functions a,~3
defined on
(201400, r).
Let u be a solutionof (E)
such thatuEC(IT; X),
where
= (~ is ~~ ; -admissible,
so that we can construct the functionsp( - ),
f7(-) as above. Under these conditions. Bve cProof
- Theproof
is asimple application
of acomparison
theoremfor
ordinary
differentialequations. Writing
for
simplicity,
we obtain from(E), (1.2), (1.4),
and(1.6)
theinequality
Subtracting ( 1. 5)
from thisinequality gives
where the variable t is
suppressed
in mostplaces.
It follows from the com-parison
theorem thatp(t},
since this is true for t =0;
note that=
~{~)
=p(0). (The
last argument is rather formal andsketchy.
To be more
precise,
one mayreplace
pby
the solution of a modified equa- tionètp
=fJ(p)
+ e withp(0) = ~~{~)
+ e, obtain the desiredinequality,
and then let E ~ 0.
Moreover,
since it is not known apriori
thatr,
one has to work within the interval
IT~
where this is true and show even-tually
thatT,
can be madeequal
tomin { T, Ti }.
Theseprocedures
are moreor less
standard.)
Annales de l’Institut Henri Poincaré - Analyse non linéaire
EQUATIONS
REMARK 1.4. -
a)
Theorem 1 and itsproof
remain valid ifC1 + (IT; X)
satisfies =F(t, u) ;
see Remark 1. 2.b) Suppose
there are severalequations
=1,
...,N,
of the form(E),
where the
right
membersF;
have theproperties
assumed for F with I andO c Z c X in common.
If { ~6 j
is aLiapunov family
on O for each of the(E~),
it is easy to seethat ~ ~~. ~
is also aLiapunov family
for(E)
withF =
Fi
+ ... +FN.
Thisapplies,
forexample,
to the KdVequation
andthe BO
equation
to be discussed in thefollowing
sections. For theKdV,
we may take
Fi(t,u) = - F2(t, u) _ -
and for theBO, Fi = -
with the sameF2.
c)
Afamily analogous
to~~
was usedby
Fritz and Dobrushin[3 ] in
the
study
of certaindynamical systems.
The authors thank Profes-sors Dell’Antonio and
Doplicher
for this information.2. ANALYTICITY OF SOLUTIONS OF THE KdV AND BO
EQUATIONS
In this section we
apply
Theorem 1 to prove theanalyticity (in
the spacevariable)
in a certainglobal
sense for solutions of the(generalized) KdV equa-
tion
(G) ~tu
=F(u) = - ~3u - a(u)lu,
t0,
where c = It is assumed that is
real-analytic
in i E[?;
nogrowth
rate is assumed for
a(~~).
A similar result can beproved
for the BOequation,
for which see Remark
2.1, c),
below.First we summarize known results for the solutions of
(G) (see [6]).
Ifwith s>
2, (G)
has aunique
solutionuEC(IT;
with
~(0) = (~
on an interval IT =[0, T ],
where T > 0 is determinedby ( ~ I ~ only. (We use ( Is
to denote theHS-norm.)
T may be chosenarbitrarily large
ifeither ( § i
i issufficiently
small or3(/.)
has a limitedgrowth
rate(say, a(i )
~o( ~ i ~4)).
It follows that = Inwhat follows we shall
restrict §
E H x to a certain class ofanalytic
functions.For each
r > O,
denoteby S(r)
thestrip { -
30 Re xin the
complex x-plane.
LetA(r)
be the set of allanalytic
functionsf
onS(r)
such thatf
EL2{S(r’))
for each r’ r, r’ > 0 and thatf {x)
E (I~ forx E tR. We shall
identify f
EA(r)
with its trace on the real axis if there isno
possibility
of confusion.A(r)
is a Frechet space with these as thegenerating
system of seminorms. Theanalyticity
for(G)
can now be statedby
thefollowing
theorem.
THEOREM 2. - Let be a solution of
(G).
Iffor some ro >
0,
there is rl > 0 such thatu E C(IT;
Vol. 3, n° 6-1986.
460
REMARK 2.1. -
a)
In terms of the inductive limit A= ~ ~ A(r) ; r
> 0~,
Theorem 2 says that
u(0)
E Aimplies u(t)
EA,
i. e. the propertyu(t)
E A ispersistent
for(G).
b)
For the proper KdVequation,
whichcorresponds
toa(~.)
= ~, in(G),
it is known
[6 ]
that Thusu(t)EA
for allt 0
if §
e A. This result is consistent with a statement in Deift-Trubo- witz[2].
c)
The BOequation
is obtained from the KdVequation simply by replacing a3
withHa2,
where H is the Hilbert transform. For the BO equa-tion,
theH °°-persistence property
stated above has been establishedrecently by
Iorio[4 ].
It follows that Theorem 2 is also true for the BOequation,
with T
arbitrarily large. Indeed, replacing ~3
withHa2
has no effect atall in the estimates
given
in section 3.d)
For theseequations
one can prove theanalyticity
of the time deri- vatives but we shall not go into theproof.
On the otherhand,
Theo-rem 2 may be
generalized
to include the case in whicha(u)
in(G)
isreplaced
with
a(t, u) involving
texplicitly, provided
a iscontinuous jointly
in t, uand
analytic
in u. A furthergeneralization
to the case a =a(t,
x,u)
ispossible,
if adepends
on xanalytically
in anappropriate global
sense.For the
proof
of Theorem2,
it is convenient to use anequivalent
setof norms in
A(r) involving only f (x)
for real x. Such norms aregiven by
Here the real
parameter s
is notessential,
since it is easy to see thatwith c
depending
on a,6’,
s, and s’.The
equivalence
of the set of norms(2.1)
to theprevious
ones is shownby
thefollowing lemma,
to beproved
in section 4.LEMMA 2 . 2.
2014 A(r)
c HOC for each r > 0.Moreover, f E A(r) implies that II
oo for any a, s with ecr r.Conversely,
iff
E satisfiesII f
for some for each ecr r,then f (has analytic
conti-nuation)
EA(r).
In view of
Lemma 2 . 2,
to prove Theorem 2 it suffices toapply
Theorem 1to the
Liapunov family
with ro. Forpractical computation, however,
it is convenient to work with a finite sum in(2 .1 ).
Thus we setAnnales de r Institut Henri Poincaré - Analyse non linéaire
EVOLUTION EQUATIONS
We
apply
Theorem 1 toestimate II u(t)
with anappropriate
func-tion
a(t), uniformly
in m, and then let m -~ x toobtain
an estimate forII u(t) !!r(f),2-
Since it is sufficient to assumeu(t)
E toperform
variousformal
computations required
in theestimate,
weapply
Theorem 1 withZ = X = and the
Liapunov family
defined on an
appropriate
open set O c Z. Theproperty
of thefamily (2. 2)
to the
Liapunov
for(G) depends
on thefollowing
lemma.for
sufficiently
small a(algebraically !),
where Kand
3 arereal-valued, nonnegative
functions with thefollowing properties.
K is continuous and monotonenondecreasing on R+. v)
is continuous and monotonenondecreasing
on a subset determinedby
aninequality
of the
form (7 ~ 6(~u, v),
with 6 monotonenonincreasing
onll~ +
x Thus vI 2, 03A603C3;m(v))
is well-defined for any v EHm + 2
if 03C3 is smallenough,
and
(2.3)
makes sense(and
is claimed to betrue)
for such a.The
proof
of Lemma 2.3 will begiven
in next section. Here we prove Theorem 2using
Lemma 2. 3. We start with theproof
that(2.2)
is indeeda
Liapunov family
for(G)
on a certain open set O c Z. For this we haveto exhibit the set O and the functions a,
f3
that appear in the basic estimate(1. 4). Actually 0,
a, and~3
willdepend
on the solution u under consideration.(It
may benoted,
inpassing,
that theproof
of Theorem 2 isgreatly simplified
if is entire in~~,
as in the proper KdVequation.
In this casewe may take O =
Z,
and the structure of the function a becomes muchsimpler.)
Given a solution u E
C(IT; Hx)
of(G)
with~(0) == (~
EA(ro),
choose ao such that ro andlet
= 1 +max {| u(t) I2, t
E IT}.
Let O be the set of all v e Zwith L~ ~ , J1; obviously
O is open inZ,
andu(t)
E O for t E IT.Using
the functionsK, a, ~ given
inLemma ? . 3,
we setWe note that
x(r)
is well-defined for r r. The same is of course true offJ(r).
In view ofLemma 2 . 3,
it is now easy to see that( 1. 4)
is satisfied with thesefunctions 03B1, 03B2
and the constants 03C3, r.(Note
that i, e Oimplies .)
This proves
that { ~~;m ~
is aLiapunov family
for(G)
on O.Vol. 3, n° 6-1986.
Moreover, § }-admissible,
sinceIf we denote
by
pm the solution of(1. 5)
withpm(o) _ ~~;m(~) p(0),
wehave
obviously p(t),
t ~0,
and we obtainby
Theorem 1where
Note that
(2.9)
holds aslong
aspm(t)
r. But sincep(t)
aslong
as it exists and since r -
1, (2 . 9)
holds for all Onletting m -~
oo, we thus obtain from(2.9)
This shows that
u(t)
EA(r1)
if ri 1 =It remains to prove the
continuity
ofu(t) in I I [ ~ 6, 2
for e~ ri. Forthis we need the
following lemma,
theproof
of which is easy and will be omitted.LEMMA 2 . 4. Let =
1, 2,
..., be a sequence with~~!!cr,2 bounded,
where e6 r. If~n ~
0 in H~ oo, then(1~~~2
~ ~for each r~ 7.
The result obtained above shows
that )) u(t) ~Ia(T),2
is bounded for t E IT.Since
u(t)
is continuous inH ~°,
it follows from the lemma thatu(t)
is conti-nuous
in ~ ~03C3,2
if 03C3 03C3(T).3. PROOF OF LEMMA 2.3
We have to for v E Z = where F is
given by (G)
andby (2 . 2).
To this end we firstcompute (
w,where =
(1/2) 2 2.
If we write A =(1 - ~2) I /2~
then=
(1/2) ( 0 2,
hence =( -
which is inH-m+ 1 c:
H - m - 2
= X* if v E Z = Hm + 5and j
m. Therefore(3 . 0)
w, =l
=( (W
EHn~ + ~ )
^where
( | )S
denotes the HS-innerproduct
on R. Since is a linearcombination of the
~I’;.
we thus obtainAnnales de l’Institut Henri Poincaré - Analyse non linéaire
EQUATIONS 463
We first
compute
Here the contribution of
a3v
vanishes onintegration by
parts. HenceUsing
a standardintegration by parts,
it iseasily seen that
the firstterm in
(3 . 3)
ismajorized by ( 1 /2)K( ~ u ( 2) ~ 2 2, where
K is a certaincontinuous,
monotonenondecreasing function, depending
on a but inde-pendent of j.
Hence _The first term on the
right
of(3.5)
has a formrequired
in(2.3).
Thus itremains to show that the second term has the form of the second term in
(2.3).
Thisrequires
somepreparations.
First we note that the
analytic
function satisfies the estimateswhere = and M can be chosen
independent
of ~, if a~ variesover a bounded set. From this it is easy to deduce the estimates
where I 12,ul
denotes theuniformly
localH2-norm (see
Kato[~ ]),
andwhere M =
b) depends only on u ~ 2.
Second,
we makefrequent
use of the formulaswhere y is a numerical constant.
(For (3 . 8’)
see[5 ].)
Third,
we use thefollowing
formula forhigher
derivatives ofcomposed
functions
(given
e. g. in Bourbaki[l, Chap. I, 3,
Exercise7 ] in
aslightly
different
form) :
where summation is taken over all
positive integers
p,kl,
...,kp
such thatVol. 3, n° 6-1986.
464 T. KATO AND K. MASUDA
If we
apply (3 . 8’)
to(3 . 9) multiplied
with1L,,
we obtainHere we use
(3 . 7)
toestimate Cl~~’~~L~~
Theremaining
factor is estimatedby repeated application
of(3.8)
followedby
thesimple
estimateL ~ ! 2
for k > 1. Thuswhere
(cycl) denotes
terms obtainedby cyclic change of ki, ..., k p
in thepreceding expression.
It is convenient at this
point
to introduce thefollowing
short-handnotation.
We estimate (see
(3.4)) by applying
the Schwarzinequality
to theinner
product ( I )2
andusing
the estimates obtained above. On multi-plying
with we thusobtain,
after somearrangement
of thefactorials,
We have to sum
(3.14)
over0 j jn.
For this we need thefollowing
technical
lemma,
theproof
of which will begiven
at the end of the section.LEMMA 3.1. For
nonnegative
real numbersbo, bl,
...,bm,
we havewhere summation is to bc taken m ur all
positiBc l; l... Iv J, and j
such thatA:i
+ ... with ! 1 ( /11 fixed. Here03B3’
is a numericalconstant, and
Annales de l’Institut Henri Poincare - Analyse non linéaire
465 EQUATIONS
Applying
Lemma 3.1 to(3.14)
andusing (3.17),
wefinally
obtainIn view of the remark
following (3 . ~),
this shows that(? . 3j
is true withSince the series
(3.19)
convergesabsolutely
for every ,u, v > 0provided
that 7 is
sufficiently small,
we haveproved
Lemma 2.3.Proof of
Lemma 3.1. Webegin
with(3.16).
We first sumin j
fork m. Then +
B 2 by
the Schwarzinequality.
The
remaining
factor does not exceed a sum, taken for 1 inde-pendently
for v =1,
..., p, whichseparates
into theproduct of p single
series
y’B (again by Schwarz),
wherey’
=(~k - 2) 1 /2
2. Thisproves
(3.16).
To prove(3.15),
wemultiply
the summandby ( j/k 1 ) 1 ~2,
which is not smaller than one. We sum the
resulting majorizing
seriesagain in j first, obtaining
BBby
Schwarz. Theremaining
factor is
majorized by
theproduct
of p - 1 identical series considered above(which
is smaller thany’B each),
and another seriesy’B (Schwarz again).
The result isagain
smaller thany’PB2.
4. PROOF OF LEMMA 2.2
We first prove the second
part
of the lemma.Let f
E H xwith !! f ~
~c,and let r eeT. We have to show that
f
hasanalytic
continuation intoS(r)
with
L2-norm
finite. For this purpose we may assume that s = 0.(This
isobvious
if s 0;
if s0,
note that there is y’ such that r and~~ .~ 00.)
In what follows we
write I f for
theL2-norm | f| 0,
to avoid confusion with thepointwise values ! /(x) ~.
SetVol. 3, n° 6-1986.
Then we
have
henceThus the
Taylor
seriesfor J
about A has radius of convergence at leastequal
toe~, and f
hasanalytic
continuation intoS(r),
which we denoteby
the sameletter f
~The
Taylor
seriesf(x
+iy)
=gives, by
the Schwarzinequality, - o
for e6. It follows on
integration
thatIntegration
in y shows thatf
eL2(S(r)),
asrequired.
To prove the first
part
of thelemma,
assume thatf
isanalytic
andbelongs
to
L2(S(r)),
where r > e6. TheCauchy integral
theoremgives
for 0 y r,We
apply
the Schwarzinequality
to(4 . 3) by factoring
into
equal parts. Using
the estimatewe thus obtain
(note that x - ~ - iy == ( x - ~
+Integrating (4.5)
in x andagain using (4.4),
and thenmultiplying
withjy2’,
we obtainfor j 1,
0 y r,Integration
in y E(0, r) gives
Annales de l’Institut Henri Poincaré - Analyse non linéaire
EQUATIONS
So far we have assumed
that j
1.Actually (4. 7)
is truefor j
= 0 too.To see this we note
that, by
the mean valuetheorem, f (x) ~ 2
does not exceed(~cr2)-1 j I f(x + ~
+ whereDr
denotes thedisk ~ ~ ~
+ir~ I
Dr
If we
replace Dr
with the square( ~ ~ ~ r, ~ r~ ~ I r)
andintegrate
the resultin x e
[R,
we seeeasily
that(4. 7)
also holdsfor j
= 0.It follows that
If s >
0,
wehave ((
xby choosing
~’ such that e6e6~
r. This proves the lemma.REFERENCES
[1] N. BOURBAKI, Fonctions d’une variable réelle. Paris, Hermann, 1949.
[2] P. DEIFT and E. TRUBOWITZ, Inverse scattering on the line, Comm. Pure Appl. Math., t. 32, 1979, p. 121-251.
[3] J. FRITZ and R. L. DOBRUSHIN, Non-equilibrium dynamics of two-dimensional infinite particle systems with a singular interaction, Comm. Math. Phys., t. 57, 1977, p. 67-81.
[4] R. J. IORIO, Jr., On the Cauchy problem for the Benjamin-Ono equation, Comm. Partial
Differential Equations, t. 11, 1986, p. 1031-1081.
[5] T. KATO, The Cauchy problem for quasi-linear symmetric hyperbolic systems, Arch.
Rational Mech. Anal., t. 58, 1975, p. 181-205.
[6] T. KATO, On the Cauchy problem for the (generalized) Korteweg-de Vries equation,
Studies in Appl. Math., Advances in Math. Suppl. Studies, t. 8, Academic Press, 1983,
p. 93-128.
[7] M. NAGUMO, Über das Anfangswertproblem partieller Differentialgleichungen, Japan. J. Math., t. 18. 1942, p. 41-47.
( Mansucrit reçu le 26 aout 1985) (revise le 14 janvier 1986)
Vol. 3, n° 6-1986.