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The two-scale convergence method applied to generalized Besicovitch spaces

Abstract

The two-scale convergence method has proved to be a very useful tool for dealing with periodic homogenization problems. In the present paper we develop this theory to generalized Besicovitch spaces, which include the almost-periodic functions. The main difficulty comes from the fact that these spaces are not separable. We also show how to apply these results to the homogenization of partial differential problems in this framework.

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The two-scale convergence method applied to generalized Besicovitch spaces

Author: Casado Díaz, Juan; Gayte Delgado, María Inmaculada
Publisher: The Royal Society
Year: 2002
Source: https://idus.us.es/bitstreams/3264fcee-baf2-4e27-869a-8515a74fbe24/download
10.1098/ spa.2002.1003
The wo-scale con e gence me hod applied o
gene alized Besico i ch spaces
By J u an C a sa d o-D¶i a z a n d Inmacul ad a Ga y e
Depa amen o de Ecuaciones Di e enciales y An¶alisis Num¶e ico,
Facul ad de Ma em¶a icas, C/ Ta ¯a s/n, Se illa, CP 41012, Espa~na
(jcasado@nume .us.es; gay e@nume .us.es)
Recei ed 10 Augus 2001; e ised 19 Ma ch 2002; accep ed 16 Ap il 2002;
published online 4 Oc obe 2002
The wo-scale con e gence me hod has p o ed o be a e y use ul ool o dealing
wi h pe iodic homogeniza ion p oblems. In he p esen pape we de elop his heo y
o gene alized Besico i ch spaces, which include he almos -pe iodic unc ions. The
main di¯ cul y comes om he ac ha hese spaces a e no sepa able. We also show
how o apply hese esul s o he homogeniza ion o pa ial di¬e en ial p oblems in
his amewo k.
Keywo ds: pa ial di®e en ial equa ions; homogeniza ion; wo-scale con e gence
1. In oduc ion
I is usual in homogeniza ion heo y o deal wi h composi e pe iodic ma e ials and
s uc u es wi h e y small pe iods. In o de o s udy hei physical beha iou (elec-
ical o he mal conduc i i y, elas ic beha iou , e c.), we need o sol e a pa ial
di¬e en ial equa ion ha , in a model case, can be w i en in he o m
¡di Aµx
"¶ u"= ; (1.1)
besides some bounda y condi ions. He e he ma ix Ais pe iodic and "is a small
pa ame e . F om he nume ical poin o iew, i is e y di¯ cul o calcula e u" om
his p oblem. We need o use a disc e iza ion o size smalle han ", and he e o e
sol ing a e y la ge sys em o equa ions, which equi es a lo o compu e memo y,
is ime-consuming and in ol es se e al s abili y p oblems.
Homogeniza ion heo y seeks o ob ain an app oxima ion o u" h ough he eso-
lu ion o simple pa ial di¬e en ial equa ions. The heo y o asymp o ic expansions
(see Bensoussan e al. 1978; S´anchez Palencia 1980) p o ides us wi h
u"(x)¹u0(x) + "u1µx; x
"¶+"2u2µx; x
"¶+¢¢¢ ;(1.2)
whe e he unc ions uia e ob ained as he solu ions o pa ial di¬e en ial p oblems
much easie o sol e han (1.1). A igo ous way o ob aining his expansion and
showing i s con e gence is he wo-scale con e gence me hod o Ngue seng and Allai e
(see Allai e 1992; A bogas e al. 1990; Ngue seng 1990). I has p o ed o be e y
use ul in he homogeniza ion o pe iodic p oblems.
P oc. R. Soc. Lond. A (2002) 458, 2925{2946
2925
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2926 J. Casado-D¶³ az and I. Gay e
We no e, howe e , ha al hough pe iodic ma e ials a e common in enginee ing
applica ions, hey do no usually occu in na u e. Howe e , we can see a ecu ence
in he s uc u es which sugges s ha a be e app oxima ion is o conside hese
ma e ials as almos -pe iodic. The aim o he p esen pape is o ex end he wo-scale
con e gence me hod o he case o almos -pe iodic (o mo e gene al) coe¯ cien s, in
pa icula , he sum o pe iodic unc ions wi h di¬e en pe iods, in o de o be able
o ea mo e gene al composi e ma e ials han he pe iodic ones. Simila ly o he
pe iodic case, i is necessa y o ha e a cha ac e iza ion o he limi o he exp ession
Z«
"(x)Áµx; x
"¶dx(1.3)
when "is a bounded sequence in a Lebesgue space Lp(«), p > 1, and Áis an
almos -pe iodic smoo h unc ion o , in a wide sense, in a gene alized Besico i ch
space (see Casado D´± az & Gay e 2002; Jiko e al. 1994; Zhiko & K i enko 1983)
in i s second a iable. To p o e he co esponding esul , he  s s ep is o show
he exis ence o a subsequence o ", s ill deno ed by ", such ha he e exis s he
limi o (1.3), o e e y Áas abo e. This is easy, using a diagonal a gumen , i he
space o unc ions Áis sepa able. Howe e , he gene alized Besico i ch spaces a e no
sepa able in gene al. This is he main di¯ cul y in ob aining ou esul . To sol e his
p oblem, we p opose an abs ac heo em gene alizing he well-known esul abou
he weak sequen ial compac ness o he uni ball in a e®exi e space. In a simple
si ua ion his was ca ied ou in Casado D´± az & Gay e (1996). The case whe e he
almos -pe iodic unc ions a e in a sepa able space has been conside ed by Ngue seng
(2000).
As an example o how ou esul s can be used in he s udy o he asymp o ic
beha iou o composi e ma e ials, we s udy he nonlinea p oblem
¡di aµx
"; u"; u"¶= in « ;
u"= 0 on @« ;
whe e ais a Ca a h´eodo y unc ion which de nes a pseudomono one ope a o o o de
pand belongs o a Besico i ch space in i s second a iable. In his case we ob ain he
limi equa ion and a co ec o esul ela ed o (1.2). To comple e his in oduc ion,
we men ion ha an adap a ion o he wo-scale con e gence o s ochas ic homoge-
niza ion p oblems has been gi en in Bou gea e al. (1994) (assuming sepa abili y).
The no ion o a s ochas ic weak de i a i e gi en in his a icle is s ongly ela ed o
he mean de i a i e we use in he p esen pape . To he s udy o homogeniza ion
p oblems in a s ochas ic ame, we also e e o Dal Maso & Modica (1986) and
Abddaimi e al. (1997).
2. A compac ness heo em
I is well known ha , o a bounded sequence ngin he dual space X0o a e®exi e
space X, he e exis s a subsequence o ngwhich con e ges weakly-¤ o some 2X0,
i.e. ngpoin wise con e ges o . The pu pose o he p esen sec ion is o gene alize
his esul , by showing ha i is necessa y o assume nei he ncon inuous no X
comple e.
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Two-scale me hod applied o Besico i ch spaces 2927
Theo em 2.1. Le Xbe a subspace (no necessa ily closed) o a e°exi e space Y
and le n:X7! Rbe a sequence o linea unc ionals (no necessa ily con inuous).
Assume he e exis s a cons an C > 0which sa is¯es
lim sup
n
n(x)6Ckxk;8x2X: (2.1)
The e hen exis a subsequence nkgo ngand a unc ional 2Y0such ha
9lim
k nk(x) = h ; xi;8x2X: (2.2)
Rema k 2.2. I Xis comple e and nis con inuous, heo em 2.1 easily ollows
om he Banach{S einhauss heo em and he weak-¤sequen ial compac ness o he
uni ball in a e®exi e space. I is also clea ha heo em 2.1 holds i we eplace he
hypo hesis Xincluded in a e®exi e space by Xsepa able. The aim o heo em 2.1
is p ecisely he applica ion o spaces ha a e no sepa able.
Rema k 2.3. Theo em 2.1 has been es ablished in Casado D´± az & Gay e (1996)
when Yis a Hilbe space.
In o de o p o e heo em 2.1, we need o ecall some esul s abou smoo h no ms
(see Cio anescu 1990).
De¯ni ion 2.4. Le Ybe a Banach space. The no m in Yis called smoo h i
o e e y y2Ywi h kyk= 1 he e exis s a unique 2Y0such ha k k= 1 and
h ; yi= 1.
The ollowing heo em is due o Asplund and Lindens auss (see Cio anescu 1990;
Lindens auss 1966).
Theo em 2.5. E e y e°exi e Banach space has an equi alen smoo h no m.
P oo o heo em 2.1. By heo em 2.5, i is no es ic i e o assume ha he no m
in Yis smoo h.
Fi s s ep. Le us p o e ha he e exis a subsequence nkgo ng, a cons an
·
C>0 and a sequence zjg » Xsuch ha
kzjk= 1;(2.3)
lim sup
k
nk(x)6·
Ckxk;8x2X; (2.4)
9lim
k nk(zj)>·
C¡1
j;8j2N:(2.5)
To his end, we de ne
C1= supnlim sup
n
n(x) : x2X; kxk= 1o:
This sup emum is  ni e because o (2.1).
By de ni ion o C1 he e exis z12Xwi h kz1k= 1 and a subsequence n1(k)gk
o ngsuch ha
9lim
k n1(k)(z1)>C1¡1:
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2928 J. Casado-D¶³ az and I. Gay e
Then we de ne C2by
C2= supnlim sup
k
n1(k)(x) : x2X; kxk= 1o:
Ob iously, C26C1and he e exis z22Xwi h kz2k= 1 and a subsequence
n2(k)gko n1(k)gksuch ha
9lim
k n2(k)(z2)>C2¡1
2:
Repea ing his easoning, we deduce ha o e e y j2N he e exis Cj2R,zj2X
and nj(k)gksuch ha , deno ing n0(k) = k o e e y k2N, we ha e
kzjk= 1;(2.6)
Cj= supnlim sup
k
nj¡1(k)(x) : x2X; kxk= 1o;(2.7)
nj(k)gkis a subsequence o nj¡1(k)gk;(2.8)
9lim
k nj(k)(zj)>Cj¡1
j;(2.9)
06Cj+ 1 6Cj:(2.10)
Taking he diagonal subsequence nk(k)g, which we deno e by nkg, we ha e
lim sup
k
nk(x)6Cjkxk;8x2X; 8j2N;
9lim
k nk(zj)>Cj¡1
j;8j2N:
The e o e, o ·
C= limjCjs a emen s (2.4) and (2.5) hold.
Second s ep. Le us now p o e ha he e exis s 2Y0such ha nkgand sa is y
(2.2). No e ha we can suppose ·
C > 0 because i no , by (2.4) we immedia ely ge
(2.2) wi h = 0. Since Yis e®exi e and zjgis bounded, he e exis a subsequence,
s ill deno ed by zjg, and z02Ysuch ha
zj* z0in Y: (2.11)
By (2.6), z0sa is es
kz0k61:(2.12)
Le x2Xbe a bi a y. Since nk(x)gkis bounded, he e exis s a subsequence
nk(j)gjo nkgk, depending on x, such ha
9lim
j nk(j)(x):(2.13)
Deno ing S= span( xgS zn:n2Ng), s a emen s (2.13), (2.5) and nk(j)linea
imply
9lim
j nk(j)(s);8s2S:
We de ne :S7! Rby
(s) = lim
j nk(j)(s);8s2S:
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Two-scale me hod applied o Besico i ch spaces 2929
By (2.4) and because nk(j)is a subsequence o nk o e e y s2S»X, we ha e
(s) = lim
j nk(j)(s)6lim sup
k
nk(s)6·
CkskX;
and so belongs o S0and sa is es k kS06·
C. On he o he hand, by (2.5) and
(2.6), o e e y j2Nwe ha e
(zj)>·
C¡1
j=µ·
C¡1
j¶kzjk:(2.14)
Thus k k>·
C¡1=j o e e y j2Nand so
k kS0=·
C: (2.15)
By he Hahn{Banach heo em, we can ex end o a unc ional o Y0, s ill deno ed
by , which sa is es k kY0=·
C. By (2.14), (2.15), (2.11) and (2.6), we deduce
·
C= lim
j (zj) = h ; z0i:(2.16)
Using (2.12) and (2.15), we hen ha e
h ; z0i=·
C; k k=·
C; kz0k= 1:(2.17)
Since Yis smoo h he e exis s a unique elemen 2Y0sa is ying (2.17), so in
(2.13) i is no necessa y o ake a subsequence, and he whole o he sequence nkg
poin wise con e ges o in X.¥
Following he idea o heo em 2.1, we can also p o e he ollowing heo em, which
gene alizes heo em 2.1 and con ains he case whe e Xis sepa able. The p oo can
be ound in Gay e Delgado (1998).
Theo em 2.6. Le Xbe a no med space (no necessa ily comple e) such ha
he uni sphe e o X0endowed wi h he weak-¤ opology is ¯ s coun able. Le
n:X7! Rbe a sequence o linea unc ionals (no necessa ily con inuous) sa is ying
(2.1). The e hen exis a subsequence nkgo ngand a unc ional 2X0such ha
(2.2) holds.
Rema k 2.7. I can be p o ed ha he uni sphe e o X0endowed wi h he weak-¤
opology is  s coun able i and only i o e e y 2X0,k k= 1, he e exis s a
sequence zng » Xsuch ha i g2X0sa is es kgk= 1 and hg; zni=h ; zni, o
e e y n2N. Then g= .
3. P elimina ies on gene alized Besico i ch spaces
In his sec ion we ecall some esul s on gene alized Besico i ch spaces we will need
la e . They ha e been p o ed in Casado D´± az & Gay e (2002) (see also Gay e Delgado
(1998); Jiko e al. (1994)). We ecall he de ni ion o he mean alue.
De¯ni ion 3.1. We say ha a unc ion :RN!Rhas a mean alue i he e
exis s a eal numbe M gsuch ha o e e y bounded measu able se K»RN
wi h jKj>0 we ha e
M g= lim
T!+1
1
jT KjZT K
(y) dy: (3.1)
In his case, we say ha M gis he mean alue o .
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2930 J. Casado-D¶³ az and I. Gay e
Following Jiko e al. (1994, 7.5, p. 242), we now gi e he de ni ion o an algeb a
wi h mean alue.
De¯ni ion 3.2. A linea space, X, o eal- alued unc ions de ned in RNis a
Banach algeb a wi h mean alue i he ollowing condi ions a e sa is ed.
(i) The elemen s o Xa e bounded, uni o mly con inuous and possess a mean
alue (see (3.1)).
(ii) The cons an unc ions belong o X.
(iii) Xis an algeb a.
(i ) Xendowed wi h he uni o m con e gence opology is comple e.
( ) Fo e e y 2Xand s2R, he unc ion (¢+s) belongs o X.
Rema k 3.3. As examples o X, we ha e he space o con inuous (0;1)N-pe iodic
unc ions and he space o uni o mly almos -pe iodic unc ions.
The abo e de ni ion allows us o de ne he gene alized Besico i ch spaces in he
ollowing way.
De¯ni ion 3.4. We de ne he gene alized Besico i ch space o o de p( ela i e o
X), wi h 1 6p < +1, and we deno e i by Bp, as he closu e o X o he semino m
[ ]p=µlim sup
T!+1
1
jBTjZBT
j (x)jpdx¶1=p
;(3.2)
i.e.
Bp= :RN!Rmeasu able: 8" > 0;9’2Xwi h [ ¡’]p< "g:
The gene alized Besico i ch space o o de 1( ela i e o X), B1, is de ned by
B1=n 2B1such ha [ ]1= sup
p>1
[ ]p<+1o:
The spaces Bpa e semino med spaces. The quo ien o Bpwi h he ke nel o [¢]pis
deno ed by Bpand i is a no med space.
Rema k 3.5. When Xis he space o con inuous (0;1)N-pe iodic unc ions, Bpis
he space o unc ions in Lp
loc(RN) which a e (0;1)N-pe iodic. The space o almos -
pe iodic unc ions in he sense o Besico i ch (see, o example, Besico i ch 1954;
Boh 1951) is ob ained by aking Xas he space o uni o mly almos -pe iodic unc-
ions.
The ollowing heo em shows ha he spaces Bpa e analogous o he spaces Lp o
a p obabili y measu e (see Casado D´± az & Gay e (2002) and Gay e Delgado (1998)
o he p oo ).
Theo em 3.6. The spaces Bpsa is y he ollowing p ope ies.
(i) Fo 16p6+1,Bpand hen Bpa e comple e.
(ii) Fo e e y 2Bp,16p < +1, he e exis M gand M j jpg. Besides,
[ ]p=M j jpg1=p.
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Two-scale me hod applied o Besico i ch spaces 2931
(iii) Fo 2B1and ¬= [ ]1, he unc ion T¬( )2L1(RN)sa is¯es
kT¬kL1(
R
N)= [ ]1;[T¬( )¡ ]1= 0;
whe e T¬is de¯ned by
T¬(s) = 8
>
<
>
:
¬i s > ¬ ;
si jsj6¬ ;
¡¬i s < ¡¬ :
(i ) I p < q, hen Bq»Bpand [¢]p6[¢]q. Mo eo e , i ; g 2Bqsa is y [ ¡g]p= 0,
hen [ ¡g]q= 0, and we can also hen see ha Bqis a subspace o Bp.
( ) The dual space o Bp, o 16p < +1, can be iden i¯ed wi h Bp0 h ough he
ollowing isome ic isomo phism:
F:Bp0!(Bp)0
hF( ); gi=M ~
~gg 8 ~
2 2 Bp0;8~g2g2 Bp;i 1<p<+1;
and
hF( ); gi=M T[ ]1(~
)~gg 8 ~
2 2 B1;8~g2g2 B1;i p= 1:
To  nish his sec ion, we ecall some esul s ela ed o he de i a ion heo y o
gene alized Besico i ch spaces (see Casado D´± az & Gay e 2002).
We s a by in oducing he space D1, which plays in he spaces Bp he same ole
as he spaces C10(RN) in he dis ibu ional heo y.
De¯ni ion 3.7. We de ne D1as
D1= ’2C1(RN) : D¬’2B1 L1(RN)8¬2(N[ 0g)Ng:
Reasoning by con olu ion (see Casado D´± az & Gay e 2002), we can show he
ollowing p oposi ion.
P oposi ion 3.8. The space D1is dense in Bp o 16p < +1.
Fo e e y 2B1, he e exis s a sequence ngin D1which con e ges o in
B1and is bounded in B1.
Analogously o dis ibu ional heo y, we use he spaces D1 o gi e a de ni ion o
he de i a i e in Bp.
De¯ni ion 3.9. Fo 2B1, we de ne he mean pa ial ide i a i e o , 1 6i6
N, and we deno e i by @i;m , as he linea applica ion o D1in Rgi en by
@i;m (’) = ¡M½ @’
@xi¾;8’2D1:(3.3)
We also de ne he mean g adien o 2B1, m , as m = (@1;m ; : : : ; @N;m ) and
he mean di e gence o F2(B1)N, di mF, as di mF=PN
i= 1 @i;mFi:Clea ly, hese
de ni ions can also be ex ended o B1.
The ollowing esul , which ela es he dis ibu ional de i a i e wi h he mean
de i a i e, is shown in Casado D´± az & Gay e (2002).
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2932 J. Casado-D¶³ az and I. Gay e
P oposi ion 3.10. I 2B1is such ha he e exis s i2 1; : : : ; Ngwi h
@ =@xi2B1, hen @i;m =@ =@xiin he ollowing sense:
h@i;m ; ’i=M½@
@xi
’¾;8’2D1:
The ollowing space plays a e y impo an ole in applica ions.
De¯ni ion 3.11. Fo 1 6p < +1we de ne
Wp= 2W1;p
loc (RN) : 2(Bp)N; M g= 0g
and
Wp= : 2Wpg:
Iden i ying an elemen o Wpwi h i s class in (Bp)N, Wpwill be conside ed as
a subspace o (Bp)N. Mo eo e , we iden i y w1; w22Wpi [ (w1¡w2)]p= 0, and
hen we can conside Wpas a no med space o he no m kwk= [ w]p.
The ollowing heo em gi es some in e es ing p ope ies o Wp(see Casado D´± az
& Gay e (2002) and Gay e Delgado (1998) o he p oo ).
Theo em 3.12. The subspace Wpis closed in (Bp)N(and hen Wpis Banach).
I 2Bp,16p < +1, is such ha m belongs o (Bp)N hen he e exis s g2Wp
such ha m = gin (Bp)N.
To ob ain u he p ope ies o Wp he algeb a mus sa is y ano he p ope y.
De¯ni ion 3.13. An algeb a Xis called e godic i o e e y 2B1such ha
[ ¡ (¢+s)]1= 0 o e e y s2RN(equi alen ly m = 0), we ha e [ ¡M g]1= 0.
P oposi ion 3.14. An algeb a is e godic i and only i
lim
R!+1·1
jBRjZBR
(x+y) dy¡M g¸p
= 0;8 2Bp;16p < +1:(3.4)
In he e godic algeb as we ha e he ollowing densi y esul .
Theo em 3.15. I he algeb a is e godic, hen D1is dense in Wp.
4. The wo-scale con e gence me hod
In his sec ion, we p esen he ex ension o he wo-scale con e gence heo y (see
Allai e 1992; Ngue seng 1990) o he gene alized Besico i ch spaces Bp ela i e o
an algeb a wi h mean alue X. We s a by gi ing he de ni ion o wo-scale con-
e gence.
De¯ni ion 4.1. Le «»RNbe open. We say ha a sequence u"g » L1
loc(«)
wo-scale con e ges o u2L1
loc(«;B1) i o e e y g2B1 L1(RN) and e e y
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Two-scale me hod applied o Besico i ch spaces 2933
E»» «bounded, measu able, we ha e
9lim
"!0Z«
u"(x)Áµx; x
"¶dx=Z«
My u(x; y)Á(x; y)gdx; (4.1)
whe e Á(x; y) = g(y)XE(x) o x2«,y2RN. We will deno e u"
2e
* u.
Rema k 4.2. The le -hand side o (4.1) makes no sense i gis only in B1since
wo ep esen a i es o gmay di¬e in e e y poin o RN. The igh -hand side does
no depend on he ep esen a i e o uchosen.
Rema k 4.3. Since B1can be iden i ed wi h he dual o B1, i is easy o deduce
ha he wo-scale limi , i ha exis s, is unique.
Rema k 4.4. Ou de ni ion o wo-scale con e gence can seem di¬e en o he
usual one o he pe iodic case, which es ablishes ha (4.1) holds o e e y Ápe iodic
in he second a iable and smoo h enough (in gene al, in he space o admissible
unc ions (see Allai e 1992)). As es ablished in p oposi ion 4.6, his is equi alen o
ou de ni ion, because i (4.1) holds o Áas in de ni ion 4.1, hen i holds o Áin all
o he spaces which appea wi h he usual de ni ion. We ha e chosen he de ni ion
gi en abo e because i makes i easie o check i a sequence wo-scale con e ges,
and when u"is bounded in Lp(«) o some p2(1;+1) (usual si ua ion), i does
no depend on p.
Al hough we ha e de ned he wo-scale con e gence me ely o a sequence u"gin
L1
loc(«), in he applica ions we will usually ha e a bounded sequence in Lp(«) o
some p2[1;+1]. In his case, we ha e he ollowing esul .
P oposi ion 4.5. Le u"gbe a bounded sequence in Lp(«) o some p2
[1;+1], which wo-scale con e ges o a unc ion u2L1
loc(«;B1). Then ubelongs
o Lp(«;Bp), he sequence u"gcon e ges weakly in Lp(«) (weakly-¤i p= +1)
o u0=My u(¢; y)gand we ha e
lim in
"!0ku"kLp(«)>kukLp(«;Bp)>ku0kLp(«):(4.2)
P oo . We deno e by S c(«;Bp0) he se o simple unc ions which ha e he sup-
po s ic ly included in «. Fo Á2S c(«;Bp0), jÁj6kÁkL1(«;B1)a.e. in «£RN
i p= 1, we ha e
¯¯¯¯Z«
u"(x)Áµx; x
"¶dx¯¯¯¯
6ku"kLp(«)°
°
°
°
Áµx; x
"¶°
°
°
°Lp0(«)
;
whe e passing o he limi when " ends o ze o, we deduce
¯¯¯¯Z«
My u(x; y)Á(x; y)gdx¯¯¯¯
6lim in
"!0ku"kLp(«)kÁkLp0(«;Bp0)8Á2S c(«;B1):
(4.3)
F om his inequali y and heo em 3.6 we easily deduce ha ubelongs o Lp(«;Bp)
and ha (4.2) holds. ¥
The ollowing esul , which is easy o p o e, ex ends de ni ion 4.1 o a wide class
o admissible unc ion Á.
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2940 J. Casado-D¶³ az and I. Gay e
By (4.18), we ha e
u"¡1
jB" jZB"
u"(¢+») d»!0 in Lp
loc(«) s ongly.
So, aking he limi in (4.20), and using (4.19) and lemma 4.12(b), we ge
Z«
My (x; y) Á(y)g’(x) dx
=¡Z«
My½µ¹(x; y)¡1
jB jZB
¹(x; y +») d»¶Á(y)¾’(x) dx;
o e e y ’2C10(«), Á2D1. This implies ha o a.e. x2«,
y;m (x; ¢) = ¹(x; ¢)¡1
jB jZB
¹(x; ¢+») d» ; (4.21)
and hen he igh -hand side o (4.21) belongs o Wp o a.e. x2«. Since i
con e ges a.e. in « o ¹(x; ¢)¡My ¹(x; ¢)gand since Wpis closed, we deduce ha
he e exis s u12Lp(«;Wp) such ha
¹¡My ¹g= yu1:
By p oposi ion 4.5, i is also clea ha My ¹g= u, which oge he wi h he abo e
equali y gi es (4.17). ¥
Analogously o p oposi ion 4.11, we ha e he ollowing esul , which implies ha
he egula i y o u1in heo em 4.13 is op imal a leas o 1 6p < +1.
P oposi ion 4.14. Le u2W1;p(«)and u12Lp(«;Wp), wi h 16p < +1.
Then he e exis s a bounded sequence u"ngin W1;p(«), such ha
u"n* u in W1;p(«)-weak;
u"n
2e
* u+ yu1:)(4.22)
P oo . By heo em 3.15 i is easy o check ha he e exis s a sequence Áng »
C1
0(«;C1(RN)) such ha yÁn2C0(«; (Bp)N),
yÁn! yu1in Lp(«; (Bp)N) (4.23)
and
lim
"!0µZ«¯¯¯¯
yÁnµx; x
"¶¡ yÁmµx; x
"¶¯¯¯¯
p
dx¶1=p
=µZ«
[ y(Án(x; y)¡Ám(x; y))]p
pdx¶1=p
<1
2m8n>m: (4.24)
Thus, o e e y n2N he e exis s a dec easing sequence "ng » (0;+1) such ha
µZ«¯¯¯¯
yÁnµx; x
"n¶¡ yÁmµx; x
"n¶¯¯¯¯
p
dx¶1=p
<1
2m8m; n 2N;16m6n;
(4.25)
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Two-scale me hod applied o Besico i ch spaces 2941
and
µZ«¯¯¯¯
"nÁnµx; x
"n¶¯¯¯¯
p
dx¶1=p
<1
2n;µZ«¯¯¯¯
"n xÁnµx; x
"n¶¯¯¯¯
p
dx¶1=p
<1
2n:
(4.26)
De ning
u"n(x) = u+"nÁnµx; x
"n¶
we deduce (4.14). ¥
5. Applica ions o homogeniza ion p oblems
Simila ly o he `classical’ wo-scale con e gence o pe iodic unc ions (see Allai e
1992; Ngue seng 1990), he main applica ion o he esul s ob ained in he p esen
pape is he homogeniza ion o pa ial di¬e en ial p oblems wi h coe¯ cien s in he
spaces Bp, gene a ed by an e godic algeb a. As an example, o 1 <p<+1, le us
conside he nonlinea p oblem
¡di (a(x="; u"; u")) = in W¡1;p0(«);
u"2W1;p
0(«);)(5.1)
whe e «»RNis a bounded open se , belongs o W¡1;p0(«) and a:RN£R£RN7!
RNsa is es
(1) Fo e e y (s; ¹ )2R£RN,a(¢; s; ¹ ) belongs o (Bp0)N. Fo a.e. x2RNand
e e y s2R,a(x; s; ¢) is con inuous.
(2) The e exis s ¬ > 0 such ha
a(x; s; ¹ )¢¹>¬j¹jp;8(s; ¹ )2R£RN;a.e. x2RN:(5.2)
(3) The e exis h2Bp0and  > 0 such ha
ja(x; s; ¹ )j6h(x) + (jsj+j¹j)p¡18(s; ¹ )2R£RN;a.e. x2RN:(5.3)
(4) We ha e
(a(x; s; ¹ 1)¡a(x; s; ¹ 2)) ¢(¹1¡¹2)>08s2R;8¹1; ¹ 22RN;a.e. x2RN:
(5.4)
(5) The e exis ® > 0, 0 < ¼ 6min p¡1;1gand k2Bp0such ha
ja(x; s1; ¹ )¡a(x; s2; ¹ )j6k(x)+®(j¹j+js1j+js2j)p¡1min js1¡s2j;1g¼;(5.5)
o e e y s1; s22R, e e y ¹2RNand a.e. x2RN.
The exis ence o a solu ion u"o (5.1) can be ound in Lions (1969). The nex
heo em gi es he asymp o ic beha iou o u".
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2942 J. Casado-D¶³ az and I. Gay e
Theo em 5.1. Assume he abo e hypo hesis and le u"be a solu ion o (5.1)
o e e y " > 0. The e hen exis a subsequence, s ill deno ed by "g, a unc ion
u2W1;p
0(«)and a unc ion u12Lp(«;Wp)such ha
u"* u in W1;p
0(«)-weak;
u"
2e
* u+ yu1;
whe e (u; u1)2W1;p
0(«)£Lp(«;Wp)is a solu ion o he wo-scale homogenized
sys em
¡di xMy a(y; u; u+ yu1)g= in W¡1;p0(«);
¡di m;y a(y; u; u+ yu1)g= 0 a.e. x2« : )(5.6)
Rema k 5.2. In gene al, he p oblem (5.6) does no ha e a unique solu ion, so
he con e gence o u"gis only o a subsequence. Assuming a u he hypo hesis,
o example, ha a(x; s; ¹ ) does no depend on sand ha in (5.4) he inequali y
is s ic o ¹16=¹2, we ha e he uniqueness o solu ion o he limi p oblem which
assu es ha he whole o he sequence u"gcon e ges.
Rema k 5.3. De ning b:R£RN!Rby
b(s; ¹ ) = My a(y; s; ¹ + y s;¹ )g 8s; ¹ 2R£RN;
wi h s;¹ he solu ion o
¡di m(a(y; s; ¹ + y s;¹ )) = 0 in (Wp)0;
s;¹ 2Wp;¾
he unc ion uin he s a emen o heo em 5.1 sa is es
¡di b(u; u) = in W¡1;p0(«);
u2W1;p
0(«):)
Rema k 5.4. In he pa icula case o a linea equa ion, a(x="; u"; u") =
A(x=") u"and A, a ma ix whose coe¯ cien s a e almos -pe iodic unc ions, he
p oblem has been s udied in Oleinik & Zhiko (1982).
In he case when he equa ion is mono one, wi h a(x="; u") almos -pe iodic in
he  s a iable, he homogeniza ion o (5.1) has been done in B aides e al. (1992),
using app oxima ion esul s in smoo he almos -pe iodic spaces. Co ec o esul s
o hese ope a o s a e p o ed in B aides (1991), exploi ing he geome ic p ope ies
o a.
P oo . By (5.2) he sequence u"gis bounded in W1;p
0(«), and hen by (5.3), he
sequence g"gde ned by
g"=aµx
"; u"; u"¶
is bounded in Lp0(«)N. Theo ems 4.8 and 4.13 hen imply ha he e exis s a sub-
sequence, s ill deno ed by "g, a unc ion u2W1;p
0(«), a unc ion u12Lp(«;Wp)
and a unc ion g02Lp0(«;Bp0)Nsuch ha
u"* u in W1;p
0(«);(5.7)
u"
2e
* u+ yu1;(5.8)
g"
2e
* g0:(5.9)
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Two-scale me hod applied o Besico i ch spaces 2943
Le ’2C10(«), Á2C10(«), 2D1, and conside ’(x) + "Á(x) (x=") as a es
unc ion in (5.1). This gi es
Z«
g"(x)µ ’(x) + " µx
"¶ Á(x) + Á(x) y µx
"¶¶dx=¿ ; ’(x) + "Á(x) µx
"¶À;
and hen, aking he limi when " ends o ze o, we deduce
Z«
My g0(x; y)( ’(x) + Á(x) y (y))gdx=h ; ’i;
o e e y ’,Á, as abo e. Reasoning by linea i y and densi y, g0sa is es
Z«
My g0(x; y)( (x) + y 1(x; y)gdx=h ; i;
8 2W1;p
0(«);8 12Lp(«;Wp);9
=
;
(5.10)
i.e.
¡di xMy g0(x; y)g= in W¡1;p0(«);
¡di m;y g0(x; y)g= 0;a.e. x2« : )(5.11)
Le us use he Min y ule o cha ac e ize g0. Fo ª ; © 2S c(«; (Bp)N), such ha
ª(x; ¢), ©(x; ¢) belong o D1 o a.e. x2«, and 2(0;1), we de ne
·"= u(x) + ªµx; x
"¶+ © µx; x
"¶;
which wo-scale con e ges o ·0de ned by
·0(x; y) = u(x) + ª(x; y) + © (x; y):(5.12)
By (5.4) we ha e
Z«µg"¡aµx
"; u"; · "¶¶¢( u"¡·") dx>0:(5.13)
Le us pass o he limi in he di¬e en e ms o his inequali y. Taking u"as a es
unc ion in (5.1) and uas a es unc ion in he  s equa ion o (5.11), we ge
lim
"!0Z«
g" u"dx= lim
"!0h ; u"i=h ; ui=Z«
My g0 ugdx: (5.14)
By (5.9), we ha e
lim
"!0Z«
g"·"dx=Z«
My g0·0gdx: (5.15)
The hypo hesis (5.5) o aimplies
¯¯¯¯
aµx
"; u"; · "¶¡aµx
"; u; · "¶¯¯¯¯
6kµx
"¶+®(j·"j+ju"j+juj)p¡1min ju"¡uj;1g¼:
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2944 J. Casado-D¶³ az and I. Gay e
Taking he powe p0and in eg a ing in «, we deduce
Z«¯¯¯¯
aµx
"; u"; · "¶¡aµx
"; u; · "¶¯¯¯¯
p0
dx
621=(p¡1) Z«
kµx
"¶p0
+®p03p¡1(j·"jp+ju"jp+jujp) min ju"¡uj;1g¼ p0dx:
(5.16)
Since he powe p0o kand he powe po j·"jand ju"jha e a mean alue,
he sequence k(x=")p0+®p03p¡1(j·"jp+ju"jp+jujp)gcon e ges weakly in L1(«).
Mo eo e , he sequence min ju"¡uj;1g¼ p0gis bounded in L1(«) and con e ges
a.e. in « o ze o. Thus (use Ego o ’s heo em), we conclude ha he igh -hand side
o (5.16) con e ges o ze o, and hen
aµx
"; u"; · "¶¡aµx
"; u; · "¶!0 in Lp0(«):(5.17)
So, by (5.8) we deduce
lim
"!0Z«
aµx
"; u"; · "¶( u"¡·") dx= lim
"!0Z«
aµx
"; u; · "¶( u"¡·") dx
=Z«
My a(y; u; · 0)(( u+ yu1)¡·0)gdx:
(5.18)
Thus, passing o he limi when " ends o ze o in (5.13) we conclude
Z«
My g0g udx¡Z«
My g0·0gdx¡Z«
My a(y; u; · 0)(( u+ yu1)¡·0)gdx>0:
Replacing ·0by (5.12) and using he second equa ion o (5.11) we ha e
Z«
My [g0¡a(y; u; · 0)][ª+ © ¡ yu1]gdx60:(5.19)
Choosing ªcon e ging o yu1in Lp(«;Bp)Nand ©con e ging o a unc ion W2
Lp(«; (Bp)N), we deduce
Z«
My [g0¡a(y; u; u+ yu1+ W )W]gdx608W2Lp(«; (Bp)N):
Di iding by and hen aking he limi when ends o ze o, we ge
Z«
My (a(y; u; u+ yu1)¡g0)Wgdx>08W2Lp(«; (Bp)N);
i.e. g0=a(y; u; u+ yu1), which by (5.11)  nishes he p oo o heo em 5.1. ¥
In o de o ob ain a co ec o esul , le us now assume ha ais uni o mly mono-
one, i.e. he e exis s ¯ > 0 such ha o e e y s2R,¹1; ¹ 22RNand a.e. x2«we
ha e
(a(x; s; ¹ 1)¡a(x; s; ¹ 2)) ¢(¹1¡¹2)>8
>
<
>
:
¯j¹1¡¹2jpi p>2;
¯j¹1¡¹2j2
(j¹1j+j¹2j)2¡pi 1 <p<2:(5.20)
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Two-scale me hod applied o Besico i ch spaces 2945
Theo em 5.5. Unde he hypo hesis o heo em 5.1 and (5.20), i u1is
smoo h enough ( o example, u12C1(·
«£RN)wi h xu12L1(«£RN), yu12
C(·
«;B1) L1(«£RN), hen
u"(¢)¡u(¢)¡"u1µ¢;¢
"¶!0in W1;p(«):(5.21)
P oo . Le Z"= u(x)+ yu1(x; x="). Reasoning simila ly o he p oo o (5.17),
we can p o e
aµx
"; u"; Z"¶¡aµx
"; u; Z"¶!0 in Lp0(«):
So,
lim
"!0Z«µaµx
"; u"; u"¶¡aµx
"; u"; Z"¶¶¢( u"¡Z") dx
= lim
"!0Z«µaµx
"; u"; u"¶¡aµx
"; u; Z"¶¶¢( u"¡Z") dx: (5.22)
In o de o pass o he limi on he igh -hand side o his equali y, i is enough o use
he ac ha a(x="; u; u") wo-scale con e ges o a(y; u; u+ yu1) (see he p oo
o heo em 5.1), he ac ha u" wo-scale con e ges o u+ yu1and (5.14),
which imply
lim
"!0Z«µaµx
"; u"; u"¶¡aµx
"; u; Z"¶¶¢( u"¡Z") = 0:(5.23)
F om (5.22), (5.23) and (5.20) we conclude ha u"¡Z"con e ges s ongly o ze o
in Lp(«) and hen (5.21) holds. ¥
This wo k has been pa ly suppo ed by P ojec PB98-1162 o he DGESIC o Spain.
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