A NNALES DE L ’I. H. P., SECTION C
J EAN -P IERRE A UBIN G UISEPPE D A P RATO
Contingent solutions to the center manifold equation
Annales de l’I. H. P., section C, tome 9, n
o1 (1992), p. 13-28
<http://www.numdam.org/item?id=AIHPC_1992__9_1_13_0>
© Gauthier-Villars, 1992, tous droits réservés.
L’accès aux archives de la revue « Annales de l’I. H. P., section C » (http://www.elsevier.com/locate/anihpc) implique l’accord avec les condi- tions générales d’utilisation (http://www.numdam.org/conditions). Toute uti- lisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit conte- nir la présente mention de copyright.
Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
Contingent solutions to the center manifold equation
Jean-Pierre AUBIN
CEREMADE;
Umversite deParis-Dauphine,
75775Paris,
FranceGuiseppe
Da PRATOScuola Notmale di Pisa, 56126 Pisa, Italy
9, n° 1, 1992, p: 13-28.
Analyse
non linéaireABSTRACT. - Given
asystem
ofordinary differential equations with lipschitzian right-hand sides,
we state an existenceand uniqueness theorem
for a
"contingent
solution"of
thefirst-order system of partial differential equations characterizing
centermanifolds,
aswell
asthe
convergence ofthe viscosity method.
Solution
contingente à
uneéquation
de centrale.-
Etant
donne unsysteme d’equations difféientielles à
second membrelipsciitzien,
on demontre uh theoreme d’existenceet d’unicite
d’une sol- ution’’’contingente"
dusysteme d’equations
auxderivees partielles
dupremier
ordre earacterisant les variétésèentrales,
ainsique
laconvergence
de la methode de viscosite.
INTRODUCTION
Let us consider the
system
of differentialequations
Annales de l’lnstitut Henri Poincaré - Analyse non linéaire - 0294-1449 Vol. 9/9~/01 /13/16/$3.b0/© Ga uthier-Villa rs
14 J.-P. AUBIN AND G. DA PRATO
where
X,
Y are finite dimensionalvector-spaces,
andg: X x Y H Y are
lipschitzian
maps and ~, > o.The
problem
offinding
maps r: X H Y whose(closed) graphs
are viabil-ity
domains of thissystem (which
can be called centermanifolds)
has beenstudied in several frameworks: see
[ 11 ], [12]
toquote
a few and theirapplications (see [4], [8], [7]
forinstance). Knowing
a center manifold anda solution x
( . )
tostarting
at xo, then thepair (x ( . ), y ( . ))
is a solution to thesystem
of diffentialequations starting
at(xo, yo)
where y(t) :
= r(x (t)).
We can characterize the maps r: X H Y whose
(closed) graphs
are centermanifolds of this
system
thanks toNagumo’s
Theorem: it states thatwhere
TK (x)
denotes thecontingent
cone to K at x E K definedby
(See [1], [5]
onviability
and invariance domain forinstance.)
We recallthat for any map r, the
contingent
cone to thegraph
of r at(x, r (x))
isthe
graph
of thecontingent derivative,
which is the set-valued map from X to Y definedby
Naturally,
D r(x) (u)
= r’(x)
u coincides with the usual derivative when-ever r is differentiable at x. It has
nonempty
values when r islipschitzian.
(See [3]
for more details on the differential calculus of nonsmooth and set-valuedmaps.)
Therefore,
we can translate this characterizationby saying
that r is asolution to the
quasi-linear
first-ordersystem
of"contingent" partial
differential inclusions.
One can say that such maps r are
contingent
solutions to thequasi-linear
first order
system
ofpartial
differentialequations
(called
the centermanifold equation),
which we shall write in the form because D r(x) (u)
= r’(x)
u whenever r is differentiable.The classical Center Manifold Theorem states that there exists a local
~~2~-solution
to thissystem when g
is~~2~,
vanishes at theorigin
and when, f ’ (x, y) = A x + fo (x, y)
where theeigenvalues
of A have zero realparts, fo
is
~~2~
and vanishes at theorigin.
The latterrequirements
are used for thestudy
of theasymptotic properties
of theequilibrium.
In this paper, we shall show that there exists a
global
bounded andlipschitzian contingent
solution to thisproblem
whenf
and g areonly lipschitzian,
whenand when ~, is
large enough.
It isunique
when ~, is evenlarger.
This
type
of result is known forequations (see [13], [17]
forinstance)
and is announced
by
P.-L. Lions andSouganidis
in moregeneral
casesby
other methods(private communication.)
Denote
by
Ar the map ofcomponents 1,
...,m).
We shall prove futhermore that these solutions can be
approximated
inthe
spirit
of the"viscosity
method"by solutions rE
to the second-ordersystem
when E - 0. We use for that purpose the fact that the
graph
of such maps rE are stochasticviability
domains of thesystem
of stochatic differentialequations
where
W (t)
is a Wiener process from X toX, provided
that(We
refer to[2]
forgeneral
results on invariantmanifolds
by
stochastic differentialequations.)
The outline of the paper starts with the
study
of linearcontingent partial
differential inclusions
where we prove that the solution is still
given by
the classical formulawhere
S~ (x, . )
is theunique
solution to the differentialequation
starting
at x at time 0. In the process, weprovide a priori
estimates of the sup-norm(the
classical maximumprinciple)
and theLipschitz
and Holdersemi-norms for first and second order
systems.
Vol. 9, n° 1-1992.
16 J.-P. AUBIN AND G. DA PRATO
In the second
section,
we use these results and fixedpoint
theorems toprove the existence of
contingent
solutions to the first and second orderquasi-linear systems
and prove the convergence of theviscosity
method.1. THE LINEAR CASE
1.1.
Contingent
solutions to first ordersystems
Let X:=R" and be
given.
We introduce two maps cp: X - X and~:
X --~ Y.We shall look for solutions r: X -~ Y to the first-order
system
ofpartial
differential
equations
Actually,
we shall look forLipschitz (or
even, closedgraph)
solutions r to thisequation. Usually,
aLipschitz
map r is notdifferentiable,
butcontingently differentiable
in the sense that itscontingent
derivative associ-ating
to every direction u E X the subsethas
nonempty
values( 1 ). Naturally,
Dr(x) (u)
= r’(x)
u whenever r is differ- entiable at x.So,
we shallprovide contingent
solutions to the first-ordersystem
of differentialequations (1),
which areby
definition the solutions to thecontingent
inclusionsWe recall that the
(closed) graphs
of solutions to thecontingent
inclusion(2)
areviability
domains of thesystem
of differentialequations
thanks to
Nagumo’s
Theorem.We shall also consider second order
elliptic systems
ofpartial
differentialequations
(1)
We recall that for any map r, the graph of the contingent derivative is the contingentcone to the graph of r at (x, r (x)).
which possess
unique
twice differentiable solutions whenever the functions cpand 03C8
arelipschitzian.
We shall establish a
priori
estimatesindependent
of Eenjoyed by
thesolutions to the first and second order
systems.
1.2. The maximum
principle
and other apriori
estimatesWe introduce the Frechet
Y)
of continuous mapsr: X --~ Y
supplied
withcompact
convergencetopology,
as well as thespaces =
(X, Y)
of m-timescontinuously
differentiable maps. We setand
We recall that on the space
~P~1~,
the semi-normsI~
r areequivalent
tothe semi-norms
(again
denotedby)
and that for
oc =1, they
are bothequivalent
to thenorm ]] r’ ~ ~ ~ .
. i . 2 . 1. The maximum
principle
We
begin by adapting
the maximumprinciple
to the case ofsystems:
PROPOSITION 1 . I . - Assume that
r E ~~2~.
Then thefollowing
apriori
estimates
independent of
E >_ 0hold true.
Proof : -
Assume first that there exists xachieving
the maximum ofj ~
r The first-order necessary conditions for a maximumimply
thatThe second-order conditions
yield
Vol. 9, n° 1-1992.
18 . J.-P. AUBIN AND G. DA PRATO
By taking
u = v = e~, we infer thatso that
Let us consider now a twice differentiable solution r to
equation (3).
By applying r (s)
to both sides ofequation (3),
we infer thatso that we derive the a
priori
estimateIf the
nonnegative
bounded functionx ( . ) : - ~
does not achieveits
maximum,
we use a standardargument
which can be found in[10], [19]
for instance. One can findapproximate maxima xn
such that x(xn)
converges to sup x
(x), x’ (xn)
converges to 0and x" ( . , . ) ~
0. Dx~X
1.2.2. A
priori
estimates in~~1~
Let a: X -
R~be
apositive
twice differentiable function outside of theorigin.
Denoteby
In
particular,
r~(r) = I r Ilex
when we take a(z) : z Ilex.
We
adapt
to the case ofsystems
apriori
estimates known forequations (see [9]
forinstance):
PROPOSITION 1 . 2. - Consider a twice
dfferentiable
solution to the second- orderequation (3).
Let us set
If
r~()
+ oo and ~, + oo, then the apriori
estimateindependent of
Eholds true. In
particular, if
cp is monotone, thenand
if
cp islipschitzian,
thenProof. -
Assume first that exists apair (x, y) achieving
the maximum ofThe first-order conditions
imply
and the
second-order
condition thatBy taking
and this formulayields
and
consequently, by taking
u = v, thatIn
particular,
we obtain thefollowing inequality
by summing
up the aboveinequalities
with u = e;,i = l,
..., n.Consider now a twice differentiable solution to the second-order equa- tion
(3). By applying r (x) - r ( y)
to both sides of thisequation,
we inferthat
>
Vol. 9, n° 1-1992.
20 J.-P. AUBIN AND G. DA PRATO
Therefore,
if we setand if we assume that p + ao, we obtain the a
priori
estimate(6)
after
dividing
both sides of thisinequality by
a(x - y)~.
The ~°‘ estimates of the solutions are
obviously
obtainedby taking
a (z) : _ ~ ~ ~ ~ ~°‘,
the derivative of which isequal
toa’ (z) = a ~ ~ z ~ ~°‘ - ~ ~.
In thiscase, ~, measures the
lack
ofmonotonicity
sinceWe observe
that
whenever 03C6 is monotone(in
the sense that(x) -
c~(Y),
x -Y ~ >__
0 for everypair (x, y))
andthat
~.(c~) __ cp ~ ~
1whenever cp is
lipschitzian.
When the function ~,
(x; y) : _ ~ ~
r(x) -
r( y) ~ ~ /a (x - y)
does not achieveits
maximum,
theargument
used above allows to findapproximate
maximaxn such that x
(xn, yn)
converges to r~(r), ~‘ (xn, yn) converges
to 0 and~" (JiCn, in) ( . , . ) ~
o. m~ . 2 . 3. A
priori
estimates in~~2~
PROPOSITION 1. 3. - We assume that the
functions
03C6and 03C8
are continu-ously differentiable.
Consider a solution to the second-orderequation (~).
Then
Proof - Actually,
we shallprove
a moregeneral
apriori
estimate. Leta: X --~
R +
be apositive
twice differentiable function outside of theorigin.
Denote
by
In
particular, r~’ (/)= ~/ ~ when
we takeLet us assume that there exists
(ac, y, fi) achieving
the maximum ofThe first conditions
imply
By taking u1=v1
andw = 0,
we infer thatLet r be a
(2)-solution
to the linearequation (I):
it satisfies theequation By applying (r’ M
fi - r( y) M)
to bothsides
of thisequation,
we obtainthanks to
(10).
Therefore;
afterdividing
both sides of thisinequality by a (.z- y)2 ~~ u ~~2,
we obtain
If the function
does not achieve its
maximum,
we useagain
theapproximation argument.
In the case when a
(z) : z It,
we obtain the estimate(9).
1.3. Existence of
contingent
solutionsWhen cp is
lipschitzian (and thus,
with lineargrowth),
we denoteby
S~ (x, . )
theunique
solution to the differentialequation starting
at x at time d.PROPOSITION 1 . 4. - Assume that cp is
lipschitzian
andthat 03C8~03B1
isbounded. Then
for
all ~, >0,
the map rdefined by
is the
unique
solution to thecontingent
inclusion(2)
andsatisfies
Vol. 9, n° 1-1992.
22 J.-P. AUBIN AND G. DA PRATO
Proof. -
Let p be anonnegative
smooth function withcompact support
andintegral
g to one and setx : = 1 Pn ~ ) ). We approximate
pp the maps cpand 03C8 by
their convolutionproducts
which are smooth functions
satisfying
We recall that the
explicit solution rh
to the first-ordersystem
isgiven by
formulaBy
the apriori
estimate(4),
we infer thatThe
graph of rh
is aviability
domain of thesystem
of differentialequations
By Nagumo’s Theorem,
the solutions(xh ( . ),
yn( . ))
to thissystem
of differentialequations satisfy
They
remain in acompact
subset00; X x Y)
becausethey enjoys
the same lineargrowth,
so that asubsequence (again
denotedby) (xh ( . ),
yh( . ))
convergesuniformly
oncompact
intervals to a function(x ( . ), y ( . )).
Since the maps cphand 03C8h
remain in anequicontinuous
set,we infer that
(x ( . ), y ( . ))
is a solution to thesystem
On the other
hand,
it is easy to check thatwhen Xh
converges to x, the solutions(xh, . )
converge to a solutionS~ (x, . ) uniformly
oncompact
intervals. Since the maps~rh
remain in anequicontinuous
set, we inferthat
~rh (xh, t))
convergespointwise
to~r (Sp (x, . )). Therefore,
the mapB~/ being bounded, rh (x)
converges also to the map r definedby
thetheorem,
which satisfiesThis amounts to
saying
that the(dosed) graph
of a map r is aviability
domain of this
system
of differentialequations,
that is to say that r is asolution to the
contingent
inclusion(2).
Uniqueness
follows fromFinally, a priori
estimates(8) imply that rh
are holderian with(These
estimates can also be obtaineddirectly
from theexplicit
expres- sion ofrh.)
D2. THE
QUASI-LINEAR
CASEWe consider now the
quasi-linear
first-ordersystems
of
partial
differentialequations, and,
moregenerally,
theircontingent
version
We recall that the
(closed) graphs
of solutions to thecontingent equation (13)
areviability
domains of thesystem
of differentialequations
thanks
again
toNagumo’s
Theorem.THEOREM 2 . I . - Assume that the maps
f
X X Y ~ X and g: X X Y ~ Yare
lipschitzian
and thatThen
for
03BB>max(c, 4 ( ( f I I 1 I gill)’
there exists a boundedlipschitzian
sol-ution to the
contingent
inclusion(13).
It isunique for
~,large enough.
Actually,
we shall also prove the convergence of the"viscosity
method"by introducing
the second-ordersystem
We shall prove that solutions to the second-order
system
converge tocontingent
solutions when E - 0.THEOREM 2. 2. - Assume that the maps
f
X x Y --~ X and g: X x Y -~ Yare
lipschitzian
and thatVol. 9, n° 1-1992.
24 J.-P. AUBIN AND G. DA PRATO
Then
for
~, > max(c, 4 ~,1 ~ ~
g( ~ 1 ),
there exists a solution YE to the second-ordersystem (15) converging
to a solution to thecontingent
inclusion(13)
whenE - 0.
Proofs.
1. A
priori
estimates. - We shall denoteby H~
theoperator
defined onlipschitzian
maps sby
r : =
Hg (s)
is the solution to À r(x) = E
Ar(x) -
r’(x) f (x, s (x)) + g (x, s (x)).
(This
makes sense since this(linear) elliptic problem
does have asolution whenever E > 0 and
f ( . , s ( . )) and g (., s ( . ))
arelipschitzian.)
andby Ho
theoperator
defined onlipschitzian
mapsby
r : = H o (s)
is the solution to~, Y (x) = g (x, s (x)) - Y’ (x) f (x,
s(x)).
We observe that the
functions
cp(x) :
=f(x,
s(x)) and 03C8 (x) :
= g(x,
s(x)) satisfy
By
above apriori estimates,
the mapHE obeys
theinequalities
and
which are
independent
of8e[0, oo [.
We first observe that when~, > c,
When we denote
by
the smallest root of the
equation
We observe that for
large À,
We thus infer that
Let us denote
by A~ {~,)
the subset of twicecontinuously
differentiable maps definedby
We have therefore observed that whenever
~, > max (c,
themaps
Ht
sendA~ (~,)
to thecompact
subsetB~ (~,)
definedby
We now check that
they
areuniformly equicontinuous
onA (X).
Indeed,
let s 1and s2 given
inA~ {~,)
and let usset r 1 :
=H£ {S 1 ),
r2 : =Hg (S2)
and r : = r 1 - r2 their difference. The map r is a solution to the
equation
By
the maximumprinciple,
we deduce thatbecause
Since the 1 are
equivalent
on~~ 1 ~,
weinfer that there exists a constant v such
Hence,
forevery ~~0, s1
and s2given
inA1~ (03BB),
we obtain theinequality
Therefore,
we can extendby continuity
these mapsHE
to maps(again
denoted
by) HE mapping
the ballB (~,)
to itself andsatisfying
the sameinequalities.
2. Existence and
uniquenes. -
Assume thatgilt).
Since the ball
B~ (~,)
iscompact
and convex andHg
is continuous from this ball toitself,
there exists a fixedpoint B (~,)
of the mapHE by
the Brouwer-Schauder-Fan Fixed-Point Theorem in
locally
convex spaces,i. e.,
a solution to theequation (15).
For
8=0,
is a solution to thecontingent
inclusion( 13).
Uniqueness
isguaranteed
forlarge enough ~,’s, actually
whenThis is
possible
becauseVol. 9, n° 1-1992.
26 J.-P. AUBIN AND G. DA PRATO
3.
Convergence of
theviscosity
method. - Since the maps r£ remain inan
equicontinuous
andpointwise
boundedsubset,
which iscompact,
asubsequences (again
denotedby) rE
converges to a map r. It remains to prove that r is a solution to thecontingent
inclusion(13).
For that purpose, we observe that the
graph
of a solution to the second- orderequation (15)
is aviability
domain of thesystem
of stochastic differentialequations
where
W (t)
is a Wiener process from X toX, provided
thatrE (x)) = E r£ (x).
Indeed,
if thegraph
of a is aviability
domain of thissystem
of stochastic differentialequations, then,
for any initial statethe solution to .
satisfies
y (t) = r (x (t))
for everyt >_ o,
so that Ito’s formulaimplies
that ris a solution to
(15).
Conversely,
Ito’s formulaimplies
that for any~~2~-solution
r to thesystem (15)
r(x)),
we haveso that
(x (t),
r(x (t)))
is a solution to thesystem
of stochastic differentialequations.
Let
(xE ( . ),
yE( . ))
be solutions to thesystem
Ltisfying
it is well known that when E converges to
0,
the solutions(xE ( . ), y£ ( . ))
converges almostsurely
to a solution(x ( . ), y ( . ))
to the
system
of differential(14).
Since the maps rE remain in anequiconti-
nuous
subset, they satisfy
This shows that r is a solution to the
quasi-linear contingent
inclusion(13).
DREFERENCES
[1] J.-P. AUBIN and A. CELLINA, Differential Inclusions,
Springer-Verlag,
1984.[2] J.-P. AUBIN and G. DA PRATO, Stochastic Viability and Invariance, Ann. Scuola Norm.
di Pisa, Vol. 27, 1990, pp. 595-694.
[3] J.-P. AUBIN and H. FRANKOWSKA, Set- Valued Analysis, Birkhäuser, Boston, Basel, 1990.
[4] J.-P. AUBIN and H. FRANKOWSKA, Contingent partial Differential Equations Governing Feedback Controls, Preprint (to appear).
[5] J.-P. AUBIN, Viability Theory, Birkhäuser, Boston, Basel, 1991.
[6] C.I. BYRNES and A. ISIDORI, A Frequency Domain Philosophy for Nonlinear Systems, with applications to stabilization and adaptive control, 23rd I.E.E.E. Conf. Dec.
Control, 1984, pp. 1569-1573 in Comutation and Control, K. BOWERS and J. LUND Eds., Birkhäuser, pp. 23-52.
[7] C.I. BYRNES and A. ISIDORI, Output Regulation of Non linear Systems, I.E.E.E. Trans.
Automn. Control, Vol. 35, 1990, pp. 131-140.
[8] C.I.BYRNES and A. ISIDORI, Asymptotic Stabilization of Minimum Phase Nonlinear Systems, Preprint (to appear).
[9] I. CAPUZZO DOLCETTA and J.L. MENALDI, Asymptotic Behavior of the First Order Obstacle Problem, J. Diff. Eq., Vol. 75, 1988, pp. 303-328.
[10] P. CANNARSA and G. DA PRATO, Direct Solutions of a Second-Order Hamilton-Jacobi Equation in Hilbert Spaces, Preprint (to appear).
[11] J. CARR, Applications of Centre Manifold Theory, Springer-Verlag, 1981.
[12] G. DA PRATO and A. LUNARDI, Stability, Instability and Center Manifold Theorem for Fully Nonlinear Autonomous Parabolic Equations in Banach Spaces, Arch. Rat.
Mech. Anal., Vol. 101, 1988, pp. 115-141.
[13] L.C. EVANS and P.E. SOUGANIDIS, Fully Nonlinear Second Order Elliptic Equations
With Large Order Coefficient, Ann. Inst. Fourier, Vol. 31, 1981, pp. 175-171.
[14] H. FRANKOWSKA, L’équation d’Hamilton-Jacobi contingente, C.R. Acad. Sci. Paris,
T. 304, Series I, 1987, pp. 295-298.
[15] H. FRANKOWSKA, Optimal trajectories associated a solution of Hamilton-Jacobi Equa- tions, I.E.E.E., 26th, CDC Conference, Los Angeles, December 9-11, 1987.
[16] H. FRANKOWSKA, Nonsmooth solutions of Hamilton-Jacobi-Bellman Equations, Procee- dings of the International Conference Bellmann Continuum, Antibes, France, June 13-
14, 1988, Lecture Notes in Control and Information Sciences, Springer Verlag.
Vol. 9, n° 1-1992.
28 J.-P. AUBIN AND G. DA PRATO
[17] O. HIJAB, Discounted Control of Degenerate Diffusions in Rd, preprint (to appear).
[18] P.-L. LIONS, Generalized solutions of Hamilton-Jacobi equations, Pitman, 1982.
[19] A. LUNARDI, Existence in the small and in the large in Fully Nonlinear Parabolic Equations, in Differentia Equations and Applications, Ed. Aftabizadeh, Ohio University Press, 1988.