A NNALI DELLA
S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze
D ONG G UN P ARK H IROKI T ANABE
On the asymptotic behavior of solutions of linear parabolic equations in L
1space
Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 4
esérie, tome 14, n
o4 (1987), p. 587-611
<http://www.numdam.org/item?id=ASNSP_1987_4_14_4_587_0>
© Scuola Normale Superiore, Pisa, 1987, tous droits réservés.
L’accès aux archives de la revue « Annali della Scuola Normale Superiore di Pisa, Classe di Scienze » (http://www.sns.it/it/edizioni/riviste/annaliscienze/) implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions). Toute utilisa- tion commerciale ou impression systématique est constitutive d’une infraction pénale.
Toute copie ou impression de ce fichier doit contenir la présente mention de copyright.
Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
http://www.numdam.org/
Parabolic Equations in
L1Space
DONG GUN PARK - HIROKI TANABE
(*)
The
object
of this paper is toinvestigate
theasymptotic
behavior of the solution of theinitial-boundary
valueproblem
for the linearparabolic equation
in as t -+ oo.
This
type
ofproblem
for an abstractparabolic
evolutionequation
was first treated in
[9],
and the convergence of the solutionu(t)
to astationary
state was shown under the
assumption
that the domainD.(A(t))
ofA(t)
isindependent
of t.Pazy [8]
established theasymptotic expansion
of the solution of(0.4) assuming
a certainasymptotic
behavior ofA(t)
andf (t),
and as itsapplication
he obtained theasymptotic expansion
of the solution of theparabolic problem (0.1)-(0.3)
inLP(Q),
1 p oo, in case when theboundary
conditions(0.2)
areindependent
of t. ’Recently,
Guidetti[4]
extended the above results to the case whenD (A(t) )
and the
boundary
conditions(0.2) depend
on time. We show thatanalogous
results for the solution of
(0.1)-(0.3)
hold inusing
the method of[7], [ 11 ]
ofestimating
the Green function of theproblem
considered.(*)
The work of the second author wassupported by
Grant-in-aid for Scientific Research61460003,
Ministry
of Education of Japan.Pervenuto alla Redazione il 29 Gennaio 1987 e in forma definitiva il 21 Ottobre 1987.
1. - Notations
Let 12 be a not
necessarily
bounded domain inlocally regular
of classC2m
anduniformly regular
of class Cm in the sense of Browder[2].
Theboundary
of n is denotedby
an. Weput
Let
be a linear differential
operator
of even order m with coefficients defined inf2
for each fixed t E
[o, oo),
and letbe a set of linear differential
operators
ofrespective
orders mj m with coefficients defined on an for each fixed t EThe
principal parts of A(x, t, D)
and are denotedby A *(x,t,D)
and
Bt(x,t,D) respectively.
Let k be a
nonnegative integer.
For 1p
oo, stands for the Banach spaceconsisting
of all measurable functions defined in 0 whose distribution derivatives of order up to kbelong
toIP(Q)-
The norm of
Wk,P(O)
is definedby
We
simply
write11 lip
instead of11 Ilo,p
to denote I,p norm for 1p
oo.We use the notation
11 II
to denote both the norm of andthat
ofbounded linear
operators
fromLl (12)
to itself.We denote
by
the set of all functions which are bounded anduniformly
continuous iri0 together
with their derivatives of order up to k.Bk (-a)
is a Banach space with normFor 0 h
1, Bk+h (f-2)
is the set of allfunctions
inBk(n)
whose kthorder derivatives are
uniformly
Holder continuous of order h. The norm ofB k + h (f-2)
is definedby
denotes the Banach space
consisting
of all functionshaving
bounded and
uniformly
continuousderivatives
of order up to k on is a Banach space with normWe denote the set of all bounded linear
operators
from toLP (Q) , by B (Lp, Lp), respectively.
For a Banach space X we denote
by Bk (I : X)
the set of all functions with values in X which are bounded and continuous in the interval Itogether
with their derivatives of order up to k.
2. -
Convergence
as t -~ o0We assume the
following:
(1.1) A(z, t, D)
isuniformly strongly elliptic,
i.e. there existsan angle 00
E(0, -2-)
such that for all realvectors I #
0 and all(x, t)
E11
x[0, oa)
(1.2)
is a normal set ofboundary operators,
i.e. ail isnoncharacteristic
for each and mk’for j #
k.(1.3)
For any(x, t)
E ao x[0, oo)
let v be the normal to ail at xand C 0
0 beparallel
to 9H at x. Thepolynomials
in Tare
linearly independent
modulo thepolynomial
inJ-’
for any
complex
number A with00 ~
arg A 27r -00
where,are the
roots withpositive imaginary part
of thepolynomial (1.4)
For each t E[0, cx)
the formaladjoint
ofA(z, t, D)
and the
adjoint system
ofboundary operators
can be constructed.
where I
Similarly,
forand
i For each p E
(1, oo)
there exists a constantCp
such that for t E[0, 00), 90
u, v E
W"P (0)
where gi
and hi
arearbitrary
functions in and such that = gj andBj (x, t, D)v = hi
on 9 f2respectively.
REMARK. It is known that under the
hypothesis (I.1)-(L6)
theinequalities (2.1), (2.2)
hold if we add somepositive
constant toA(x, t, D)
if necessary.For 1 p oo let
Ap (t)
be theoperator
definedby
for u E
D(Ap(t)), (Ap(t)u)(x)
=A(z,t,D)u(z)
in the distribution sense.Similarly,
theoperator Ap(t)
is definedby replacing A(x, t, D)
andby
andFrom the
assumptions
above it follows that-Ap(t), -Ap(t) generate
analytic semigroups
inL.P(f2),
and the resolvent setsp(Ap(t)),
containthe closed sector
p
. The
operator A(t)
is defined as follows:The domain
D(A(t))
is thetotality
of functions usatisfying
thefollowing
three conditions:
(i)
u E for any q with 1 qn/(n - 1),
(ii) A(x, t, D)u
E in the sense ofdistributions,
(iii)
for any p with 0(n/m)(1 - 1/p)
1 and any v ED (A’, (t)), p’ = pl(p - 1),
For u E
D(A(t)) (A(t)u)(x)
=A (x, t, D) u (x)
in the distribution sense.It is known that
-A(t) generates
ananalytic semigroup exp(-rA(t))
in([10], [11]).
It can be shown withoutdifficulty
that for somepositive
constant co the
inequalities (2.1)
and(2.2)
hold if wereplace A(x,t,D) by A(x, t, D) -
co andCp by
some other constant.Hence,
there exists a constantCo
such that for r >0,
0 t o0Let
U(t,s)
be the evolutionoperator
of the evolutionequation
inThe existence of such an
operator
was shown in[6]
and it is constructedas follows:
Our first main result is the
follow.ing:
THEOREM 2.1.
Suppose
that thehypotheses (1. 1)-(1.6), (II)
aresatisfied.
Let
f (t)
be auniformly
Holder continuousfunctions
with values inLl (f2) defined
in[0, oo):
where
01
and h are constants with01
>0,
0 h 1.Moreover,
assume that the , strong , limitfo = t im
t- oof (t)
exists.Then, for
any solutionu(t) of
theevolution
equation (2.5),
we havein the strong
topology of
Ll(f2).
Following
theargument
of[4]
we can prove Theorem 2.1 with the aid of(2.3), (2.4)
and thefollowing
lemma./
LEMMA 2.1. For each
fixed
s > 0For any e > 0 there exists a constant 0 such that
...
We
plan
to prove Lemma 2.1 as follows. First we note thatIf we have a desired estimate of
A(t) PRl (T, s)
for some 0 p1,
thenwe can write the first term of the
right
side of(2.12)
asLet be the real
interpolation
space ofand with norm denoted
by 11 118,1..
’
Then,
in view of Grisvard[3]
we have for 0 6 1It is easy to show that for 0 p
0/m
Clearly,
Combining (2.13), (2.14), (2.15)
weget
Consequently,
in order to establish an estimate of it suffices to obtain that of whereB(Ll, W9.1)
is the setof all bounded linear
operators
from to(0).
Since(2.17)
the
problem
is reduced toestimating
and for0 s t oo. In view of
(2.1)
the desired result follows from the estimatesof where
G(x, y, r; t)
is the kernel ofexp(-rA(t)).
3. - Proof of Lemma 2.1.
In what follows we let the notation
Cp
stand for constantsdepending only
on the
hypothesis (1. 1)-(1.6), (II)
and p E(1, oo).
Arguing
as in[7], [11]
we see that for each p E(l,oo)
there exists apositive
constantbp
such that for each t E(0, oo),
A EE,
acomplex
vector tywith
6plAll/-
and u,v Ewhere gj and hj
arearbitrary
functionssatisfying
= gi and We define theoperator A~ (t) by
for u E = in the sense of distributions.
Similarly replacing A(x, t, D ~-- r~), {B~ (x, t, D + r~)}".’’~i by A’(x, t, D -I- r~),
t, D the
operator All? (t)
isdefined..7
= 1It follows
from (3.1), (3.2)
that if AE ,
thenLet
w(t)
be a function defined in[0, oo)
such thatSince the derivative w =
aw/at
of the function satisfiesit follows from
(3.1), (3.3)
thatWe choose natural numbers
E,
s andexponents
2 = q1 q2 . ~ . qa3 as follows
(Beals [1]):
In what follows we consider
only
the case(iii).
According
to Sobolev’simbedding
theorem there exists apositive
constantï such that
for j
=1,...,
s - 1where (
where
where
Similarly, by
virtue of(3.3), (3.4), (3.8), (3.9), (3.12)
we obtainAs is
easily
seenr
where r is a smooth contour
running
inE B{0}
fromFor
~1,..., At E E
and ’7 withbe the kernel of
~
is the kernel ofBy
anelementary
calculusWith the aid of
(
Estimating
other terms of theright
side of(3.21) analogously
we obtainSimilarly
weget
Hence
It is easy to show
Let
(x,
y;t)
be the kernel of Then as was shown in[7], [11]
With the aid of
(3.20), (3.26), (3.27), (3.28)
we obtainMinimizing
theright
side of the aboveinequality
withrespect to 1/
weget (H6nnander [5])
In view of
(3.19)
we haveFor any fixed > 0 let be the contour defined
by
where a =
=,splr,
p = and e is apositive
constant which will be fixed later.Differentiating
both sides of(3.30)
with
respect
to xjand t, deforming
theintegral path
r to andusing (3.29) yield
Estimating
theright
side of the aboveinequality
as in section 5 of[6]
we conclude
Similarly
If we denote the kernel of then in view of
(2.9)
By
virtue of(3.31)
and(3.32)
With the aid of
(3.33), (3.34)
we concludefor any
f E Ll (f2).
We choose constants p and 0 so that 0 p
0/m,
0 0 1.Combining (2.16), (2.17), (3.35), (3.36)
we obtainBy
virtue of(2.8), (3.36)
and Gronwall’sinequality
weget
Using (3.37)
and theinequality
we
get
Making
use of(3.37)
and(3.39) yields
With the aid of
(2.7)
and(3.38)
weget
As was mentioned in section 1 all the
hypothesis (I.I)-(1.6), (II)
aresatisfied
by A(x, t, D) -
co, for some co > 0 if wereplace Cp by
some other constant. If we denoteby
operators
obtainedby replacing A(t) by
=A(t) -
co in the definition ofU(t, s), W (t, s), 1~1 (t, s), R ( t, 8), then
and
(3.41), (3.42)
hold withAO (t), WO (t, s)
inplace
ofA(t), W(s,t).
Hence
which
implies (2.10).
With the aid of
(3.44)
we haveLet e be an
arbitrary positive
number. If s is solarge that sup cv (T)
c,then the
right
side of(3.45)
does not exceed- -
from
which the second half of the assertion of Lemma 2.1 follows.Thus the
proof
of Lemma 2.1 iscomplete.
4. -
Asymptotic expansion
at t = o0In this
section we
consider theasymptotic expansion
at t = oo.In addition to
(I.1)-(L6), (II)
we make thefollowing assumptions.
(III.1)
For10:1
mwith o~,
a" k
E fork - 0,...~ r’
E~([0,oo) :
L- (f2)).
IfI a = m,
a.,, k E and r~ EBo (i-l
x[0, oo) ),
and henceso do
c~ ~
andr’..
For
where
with
with
where
THEOREM 4.1.
Suppose
that thehypotheses (1.1)-(1.6), (II), (III,I)-(III.4)
are
satisfied.
Letf (t)
be such thatwith
fk
EL1(0) for
k =0, ..., v
and r EThen
for
any mild solutionof (1.5)
wish,
According
to theargument
of theorem 1.4 of[4]
it suffices to show thatwith
Tk, R(t)
EB(L1, L1)
for k =0, ..., L
and t E[0, 00), lim
t ooR(t) = 0,
lim
(dldt)R(t) =
0 in thestrong operator topology. Actually
we shall provet-oo
this convergence in the uniform
operator topology.
In what follows we assume that are extended to the whole
of [2
or 11 x so thatWe
put
for and
Analogously,
theoperators ,
Bi,k (x, D),
~ are defined.It is obvious that
(3.1 )
holds also forA(x, D + r~),
in
place
ofA(x, t, D + r~), {B~ (x, t, D + r~) }’.’~~i :
for A EE,
’1 E en with1r¡1
~ and u Ewhere gj
is anarbitrary
function insatisfying
= gj for
each j
=1, ..., m/2.
This is the same for theinequality (3.2).
Let
Ap
be theoperator
definedby
(Apu)(z)
=A(z,D)u(z)
for u ED(Ap)
in the distribution sense, andAp
be theoperator
definedanalogously
withA(x, D + ~)
and{B; (x, D + rI) } ~ ~i
inplace
of
A(x,D)
and{B; (z, D) }m~~ . Similarly,
theoperator Ap,
are defined.For A
~ EB{0}, ?
withIlll
C andf
E 1 p oo, weput v(t) = ,B)-1 f
and vo =a)-1 f.
In view of(3.1) and.
(4.10)
We define a finite sequence of functions Via,
i = 1, - - ., v, successively
asthe solutions of the
following boundary
valueproblems:
Since the functions
1, ..., v,
areuniquely
determinedby f,
wemay denote them as
’
We
put
Clearly
Applying (4.10)
to v;yields
It follows from
(4.12)
and the aboveinequality
thatWe
put
An
elementary
calculusyields
Hence, applying (4.10)
towe
easily get,
The
inequality (4.15) implies
Similarly, replacing (A, {B; }) by
itsadjoint (A’, {Bjl })
we defineoperators
i = 0, - - ., v,
and so thatWe obtain
We first establish the
asymptotic expansion
of the kernels of thesemigroup exp(-TA2(t))
at t = oo. We choose natural numberst,
s andexponents 2 = 91 92 "’ g 9+i =00,
2 = ri r2 ... re-,, rt-,+, = ooas in
[7], [11] (Beals [1])
i.e. ,(i)
in case m >n/2. t
= 2 and s =1,
hence 2 = q1 q2 - oo and2 = ri
r2 = cxJ;(ii)
in case mn/2.
s >n/2m, t -
s >n/2m, q~ 1 - m/n
forj = 1, ..., s-1,
>m/n
>m-nlq,
is not anonnegative integer, 1, ..., e-s-1,
>is not
a nonnegative integer;
In what follows we
only
consider the case(ii). According
to Sobolev’simbedding
theorem theinequalities (3.10)
and(3.12)
holdfor j
=1, ... , s
andj
=1, - - ., t -
srespectively.
Put 6 =
min{bp;
l P = ql · · · qa I ri I * * * LetÅ1,..., Åt E E B101
and1/ be a
complex
n-vectorsatisfying
In view of
(4.13)
is the sum of terms which contain at least one of
as a factor. With the aid of
(4.14)
and(3.10)
we see thatHence
Analogously
Therefore,
if we denote the kernel ofby MI? (x, y),
then in view of(4.25), (4.26)
and Lemma 2 of[1]
As was shown in
[7], [11] if q
is pureimaginary,
then(if
il isbounded,
t7 need not be pureimaginary).
Sinceit follows from
(4.28), (4.29)
thatSimilarly
we obtainHence, arguing
as in[7], [11]
if we denote the kernel ofby M (x, y),
then we havefor any
complex
n-vectorsatisfying (4.22). Combining (4.27), (4.30)
andarguing
as in section 4 of
[7]
weget
Analogously,
if we denote the kernel of ~ Jwhere
Cv(t) =max W2(t),
It follows from
(4.23), (4.31), (4.32)
thatare
operators
with kernelsIf
we denoteby
We denote the kernels of the
operators exp ~
Iby G(z,y,r;t), 6(xy,tr;t).
Thenby
virtue of theequality (3.19)
and that withA2
inplace
of we haveArguing
as in[7], [11]
weget
for r in the
region 1;
With the aid of the
argument
of[7], [11]
we obtainFrom
(4.13) with 17
= 0 and theequality
t2013~
it follows that
~,~(a:,!/),
and are the kernels of andRa,p(t) respectively
for 1 p 00. If we define theoperators
asintegral operators
inL1 (~)
with kernels~~(x,~),
thenIn view of
(4.39)
we haveSince the above
argument
remains valid if wereplace A(x, t, D) by
A (x, t, D) -
co for some co > 0(section 1),
theexpansion (4.40)
also holds for A = 0. Thus theproof
of(4.9)
iscomplete.
REFERENCES
[1]
R. BEALS, Asymptotic behavior of the Green’s function and spectral function of an elliptic operator, J. Func. Anal., 5 (1970), pp. 484-503.[2]
F.E. BROWDER, On the spectraltheory
of elliptic operators. I, Math. Ann., 142 (1961), pp. 22-130.[3]
P. GRISVARD,Équations
differentielles abstraites, Ann. Scient. Ecole Norm.Sup.,
2 (1969), pp. 311-195.[4]
D. GUIDETTI, On the asymptotic behavior of solutions of linear nonautonomousparabolic equations,
preprint.
[5]
L. HÖRMANDER, On the Riesz means of spectral functions and eigenfunction expansions for ellipticdifferential
operators, Some Recent Advances in the Basic Sciences, 2 (Proc. Annual. Sci. Conf., Belfer Grad. School Sci., Yeshiva Univ., New York, 1965-1966), pp. 155-202.[6]
D.G. PARK, Initial-boundary value problem for parabolic equation inL1,
Proc.Japan
Acad., 62 (1986), pp. 178-180.[7]
D.G. PARK,Regularity
in time of the solution of parabolicinitial-boundary
valueproblem
inL1
space, Osaka J. Math., 24(1987),
pp. 911-930.[8]
A. PAZY,Asymptotic
behavior of the solution of an abstract evolution equation andsome applications, J. Diff. Eq., 4 (1968), pp. 493-509.
[9]
H. TANABE, Convergence to a stationary state of the solution of some kinds of differential equations in a Banach space, Proc.Japan
Acad., 37 (1961), pp. 127-130.[10]
H. TANABE, On semilinear equations of elliptic and parabolic type, FunctionalAnalysis and Numerical Analysis,
Japan-France
Seminar,Tokyo
and Kyoto, 1967 (ed. H.Fujita),
JapanSociety
for the Promotion of Science, 1978, pp. 455-463.[11]
H. TANABE, Functional Analysis. II,Jikkyo Shuppan Publishing Company, Tokyo,
1981 (in