Asymptotic behaviour of nonlocal reaction-diffusion equations
Abstract
The existence of a global attractor in L^2(Ω) is established for a reaction-diffusion equation on a bounded domain Ω in R^d with Dirichlet boundary conditions, where the reaction term contains an operator F : L^2(Ω) → L^2(Ω) which is nonlocal and possibly nonlinear. Existence of weak solutions is established, but uniqueness is not required. Compactness of the multivalued flow is obtained via estimates obtained from limits of Galerkin approximations. In contrast with the usual situation, these limits apply for all and not just for almost all time instants.
Full text
Asymp o ic beha iou o nonlocal
eac ion-di usion equa ions∗
Ma ´ıa Anguiano
Dp o. de Ecuaciones Di e enciales y An´alisis Num´e ico,
Uni e sidad de Se illa, Apdo. de Co eos 1160
41080 Se illa, Spain
E-mail: [email p o ec ed]
P.E. Kloeden and T. Lo enz
Fachbe eich Ma hema ik, Johann Wol gang Goe he Uni e si ¨a
D-60054 F ank u am Main, Ge many
E-mail: kloeden / [email p o ec ed]
Abs ac
The exis ence o a global a ac o in L2(Ω) is es ablished o a eac ion-
di usion equa ion on a bounded domain Ω in Rdwi h Di ichle bounda y
condi ions, whe e he eac ion e m con ains an ope a o F:L2(Ω) →
L2(Ω) which is nonlocal and possibly nonlinea . Exis ence o weak solu-
ions is es ablished, bu uniqueness is no equi ed. Compac ness o he
mul i alued low is ob ained ia es ima es ob ained om limi s o Gale kin
app oxima ions. In con as wi h he usual si ua ion, hese limi s apply
o all and no jus o almos all ime ins an s.
1 In oduc ion
A simple popula ion model wi h spa ial dependence is gi en by he eac ion-
di usion equa ion
∂u
∂ = ∆u+u(1 −u) , (1)
on a bounded domain Ω in Rdwi h Di ichle bounda y condi ions. The long
e m dynamics o his model is well unde s ood.
In he abo e model he popula ion a a poin x∈Ω depends only on i s
alue a his poin , apa om he di usi i y e m. Mo e ealis ically, i could
∗Pa ially suppo ed by he Minis e io de Ciencia y Tecnolog´ıa (Spain) and FEDER (Eu-
opean Communi y) g an BFM2002-03068 as well as he DFG g an s KL1203/7, LO273/5)
1
depend on he popula ion size a o he poin s, in pa icula ly a nea by poin s.
Fo example, i could depend on he a e age o e a small neighbou hood
uδ( , x) = ZB(x;δ)
u( , y)dy ZB(x;δ)
dy ,
o some small δ > 0 ins ead o on u( , x) i sel . This leads o a nonlocal PDE
∂u
∂ = ∆u+uδ(1 −uδ) . (2)
Al e na i ely, uδ( , x) could be some o he unc ional o he solu ion u(·, )
e alua ed a he poin x.
The e a e many applica ions o nonlocal e ec s in pa ial di e en ial equa-
ions in he li e a u e, e.g., in combus ion heo y [13] and he Na ie -S okes
equa ions [5]. The nonlocal e m is o en an in eg al ope a o and he equa ions
a e hen called “in eg o-di e en ial” equa ions. Bol zmann equa ions a e a e y
well known class o in eg o-di e en ial, bu a e i s o de unlike hose o in e es
he e. Howe e , he nonlocal e m could be di e en , see, e.g., he e iew a icle
by Ba es [3]. The e is a la ge li e a u e on he exis ence, egula i y and blow–up
o solu ions o nonlocal e olu ion equa ions, see o example [15, 16, 17] and he
pape s ci ed he ein.
Global a ac o s o nonlocal e olu ion equa ions ha e been in es iga ed
ecen ly o he globally modi ied Na ie -S okes equa ions by Ca aballo e al.
[5], o m-Laplacian pa abolic equa ions wi h a nonlocal nonlinea i y by Chen [6]
and by Hilho s e al [8] o a nonlocal Ku amo o–Si ashinsky equa ion. Se e al
aspec s o eac ion-di usion equa ions a e being analyzed o e he las yea s,
pa icula ly, hei asymp o ic beha iou , see o example [14,15] and [17]. In
his pape we conside gene al nonlinea nonlocal e ms in au onomous eac ion-
di usion equa ions, which gene a e s ic mul i alued semi lows. In pa icula ,
we es ablish he exis ence o a global a ac o a e i s p o ing weak solu ions
and he compac ness o a ainabili y se s o he mul i alued semi low. Fo his
we use es ima es ob ained as limi s o Gale kin app oxima ions which hold o
e e y ime ins an and no jus o almos all ime ins an s. The p oblem
is o mula ed in he nex sec ion and dissipa i i y es ima es a e p esen ed in
Sec ion 3 wi h some longe p oo s gi en a he end o he pape in Sec ion 7.
The exis ence o weak solu ions is es ablished in Sec ion 4, while he gene a ion
o a s ic mul i alued semi low and he exis ence o a global a ac o a e shown
in Sec ion 5. Finally an explici example is p esen ed in Sec ion 6.
2 Se ing o he p oblem
Le Ω ⊂RNbe a bounded open se , i sa is ies he Poinca ´e inequali y, i.e.,
he e exis s a cons an λΩ>0 such ha
ZΩ
u2(x)dx ≤λ−1
ΩZΩ
(∇u(x))2dx,∀u∈H1
0(Ω).(3)
2
Le (·,·) deno e he scala p oduc in L2(Ω) and k·kL2(Ω) he co esponding
no m in L2(Ω). In addi ion, le h·,·i deno e he duali y p oduc be ween spaces
H1
0(Ω) and H−1(Ω).
Conside he ollowing ini ial bounda y alue p oblem o a nonlocal eac ion–
di usion equa ion wi h ze o Di ichle bounda y condi ion in Ω,
∂u
∂ +A u =F(u) in Ω ×(0, T),
u= 0 on ∂Ω×[0, T],
u(x, 0) = u0(x), o x∈Ω,
(4)
whe e Ais a uni o mly pa abolic ope a o in di e gence o m wi h aij =aji ∈
L∞(Ω), 1 ≤i, j ≤N, o which he e exis cons an s λA, ΛA>0 such ha
λA|η|2≤
N
X
i,j=1
aij(x)ηiηj≤ΛA|η|2
and
Au(x) := −
N
X
i,j=1
∂xjaij(x)∂xiu(x)(5)
o all x∈Ω and η∈RN.
Rema k 1 The ope a o induced by Acan be in e p e ed as
A∈ LH1
0(Ω), H−1(Ω)
and is symme ic wi h
hA , i ≥ λAk∇ k2
L2(Ω) o all ∈H1
0(Ω).
Since H1
0(Ω) is included in L2(Ω) wi h compac injec ion, as a consequence o
he Hilbe -Schmid Theo em he e exis s a nondec easing sequence o posi i e
eal numbe s,
0< λ1≤λ2≤... ≤λk≤......,
wi h limn→∞ λn= +∞and he e exis s an o hono mal basis {wk:k≥1}o
L2(Ω). Mo eo e , {wk:k≥1}is an o hogonal basis o H1
0(Ω) wi h A wk=
λkwk o all k≥1, whe e
(u, )H1
0(Ω)
De .
=hAu, i.
The ope a o F:L2(Ω) →L2(Ω) ul ills he ollowing assump ions:
a) Fis con inuous wi h espec o he L2no m.
3
b) he e exis β∈(0, λAλΩ) and Cβ>0 wi h
(u, F(u)) ≤βkuk2
L2(Ω) +Cβ o e e y u∈L2(Ω),(6)
c) he e is some nondec easing Ψ : [0,∞)→Rsuch ha o all u∈L2(Ω),
kF(u)k2
L2(Ω) ≤ΨkukL2(Ω)(7)
In special cases Fwill also be assumed o sa is y a local Lipschi z condi ion:
d) Fo all R > 0 he e exis s LRsuch ha i , w ∈L2(Ω) wi h k kL2(Ω) ≤R,
kwkL2(Ω) ≤R, hen
kF( )−F(w)kL2(Ω) ≤LRk −wkL2(Ω) . (8)
Rema k 2 In he subsequen s a emen s and p oo s, condi ion (c) can be
easily eplaced by he sligh ly weake assump ion ha he e is a nondec easing
unc ion e
Ψ : [0,∞)→Rsuch ha o e e y u∈H1
0(Ω) wi h Au ∈H1
0(Ω),
|hF(u), A ui| ≤ e
ΨkukL2(Ω).(9)
kF(u)k2
L2(Ω) ≤e
ΨkukH1,2(Ω).(10)
3 Dissipa i i y es ima es
Bo h he exis ence o weak solu ions and o bounded abso bing se s in L2(Ω),
H1
0(Ω), espec i ely, a e based on he ollowing a p io i es ima es. Thei p oo s
do no equi e he uniquenss o weak solu ions o a gi en ini ial alue. Some
o he auxilia y esul s a e o mula ed o Gale kin app oxima ions, and hei
(qui e echnical) p oo s a e pos poned o §7.
P oposi ion 3 I Fsa is ies hypo hesis (b), hen e e y weak solu ion u∈
L20, T;H1
0(Ω)o (4) wi h u0∈L20, T;H−1(Ω) ul ills he es ima es
u( )
2
L2(Ω) ≤M
L+e−L
u(0)
2
L2(Ω)
λAZ
0k∇uk2
L2(Ω) ds ≤1
2+β
L
u(0)
2
L2(Ω) +Cβ+βM
L
o e e y ∈[0, T]wi h he cons an s M:= 2 Cβ>0and L:= 2 λΩλA−2β > 0.
The p oo is gi en in §7.
4
P oposi ion 4 Suppose ha condi ions (a)–(c)hold o Fand ha T < ∞.
Then he e exis s posi i e cons an s C0,C1and C2depending only on β,Cβ,
ΛA,λAand λΩsuch ha e e y weak solu ion u∈L20, T ;H1
0(Ω)o (4) wi h
u0∈L20, T;H−1(Ω)and ku0kL2(Ω) ≤ρsa is ies he a p io i es ima es
ku(s)k2
L2(Ω) ≤C1+e−C0sρ2
∇u( )
2
L2(Ω) ≤C1·max{1,1
}· 1+e−C2 ρ2+ ΨC1·(1 + e−C2 ρ2)
o e e y 0≤s < ≤T.
The p oo , gi en below, uses analogous es ima es o he Gale kin app oxima-
ions in he ollowing lemma, which is p o ed in he §7.
Lemma 5 Le {wk:k≥1}be an o hogonal basis o H1
0(Ω) as in Rema k 1.
Fo each n∈N, suppose ha un( ) =
n
X
k=1
unk( )·wkis a solu ion o
d
d (un( ), wk) + hAun( ), wki= (F(un( )), wk)
(un(0), wk) = (u0, wk), k = 1 . . . n.
(11)
I F:L2(Ω) →L2(Ω) sa is ies he hypo heses (b)and (c), hen he e exis
posi i e cons an s C1,C2and C3depending only on β,Cβ,ΛA,λAand λΩ
such ha whene e ku0kL2(Ω) ≤ρ, he ollowing es ima es holds o e e y s0,s,
∈(0, T]wi h 0< s0≤s≤
∇un( )
2
L2(Ω) ≤C1·max 1,1
·1+e−C2 ρ2+ ΨC1(1 + e−C2 ρ2)
Z
sku0
n(ξ)kL2dξ ≤C3·√ −s·cons (s0, T, ρ).
ku0
n( )kH−1(Ω) ≤cons (β, Cβ,ΛA, λA, λΩ, ρ).
P oo o P oposi ion 4. The inclusions u∈L20, T;H1
0(Ω)and u0∈
L20, T;H−1(Ω)always imply ha u∈C0[0, T ]; L2(Ω), see [7, §5.9].
Le {wk:k≥1}be an o hogonal basis o H1
0(Ω) as in Rema k 1. Then o
each n∈N,
un: [0, T]→H1
0(Ω), 7−→
n
X
k=1 u( ), wkwk
is induced by he o hogonal p ojec ion o u( ) on span{w1. . . wn}in L2(Ω).
I sol es he pe u bed nonlocal Gale kin p oblem
(d
d (un( ), wk) + hAun( ), wki= (G( ), wk)
(un(0), wk) = (u0, wk), k = 1 . . . n,
(12)
wi h he map G: [0, T]→L2(Ω) de ined by G( ) := F(u( )) o each ∈[0, T],
which depends only on ime in combina ion wi h he weak solu ion u(·) (bu no
5
on unexplici ly). In pa icula , G ul ills he condi ions (a)–(c) (uni o mly wi h
espec o ime). Hence, Lemma 5 p o ides a p io i es ima es o each Gale kin
app oxima ion un(·) depending essen ially only on he L2no m o he ini ial
alue u0.
Since {wk, k ≥1}is an o hono mal basis o L2(Ω), he sequence (un( ))n∈N
con e ges o u( ) in L2(Ω) a each ime ∈[0, T]. The L2bound o he H1
0
no m implies a weakly con e gen subsequence o (un)n∈Nin L20, T;H1
0(Ω)
and, i s weak limi is u∈L20, T ;H1
0(Ω)(again). Fo each s0∈(0, T), we
e en ha e a L∞bound o he H1
0no ms o (un)n∈Nin [s0, T] and so Lemma 7
below gua an ees he same es ima es holds o
∇u( )
2
L2(Ω) a e e y ime ∈
[s0, T], no jus o Lebesgue-almos all such .
Fixing s0∈(0, T) a bi a ily, he Gale kin app oxima ions o any weak solu ion
u(·) wi h ku(0)kL2(Ω) ≤ρa e equi–con inuous w. . . L2(Ω) in [s0, T ] due o he
second es ima e in Lemma 5. Now he poin wise con e gence o he Gale kin
app oxima ions o u(·) implies he ollowing s a emen di ec ly:
Lemma 6 Suppose ha he condi ions (a)–(c)hold o Fand ha T < ∞.
Fo e e y ρ > 0, he subse o C0[0, T ]; L2(Ω)consis ing o all weak solu ions
u∈L20, T;H1
0(Ω)o (4) wi h u0∈L20, T;H−1(Ω)and ku(0)kL2(Ω) ≤ρ
is equi-con inuous in he subin e al [s0, T] o e e y s0∈(0, T).
Lemma 7 Le X, Y be Banach spaces such ha Xis e lexi e, and he in-
clusion X⊂Yis con inuous. Assume ha (un)n∈Nis a bounded sequence in
L∞( 0, T;X)such ha un* u weakly in Lp( 0, T;X) o some p∈[1,+∞)
and u∈C0([ 0, T]; Y).
Then, o e e y ∈[ 0, T ],u( )belongs o Xand sa is ies
ku( )kX≤sup
n≥1kunkL∞( 0,T ;X).
P oo o Lemma 7. We deno e
C:= sup
n≥1kunkL∞( 0,T ;X).
As (un)n∈Nis a bounded sequence in L∞( 0, T ;X), he e exis a subsequence
(uµ) and ∈L∞( 0, T;X) such ha uµ
∗
* in L∞( 0, T;X), i.e.,
ZT
0hw∗( ), uµ( )id −→ ZT
0hw∗( ), ( )id ∀w∗∈L1( 0, T ;X0),
whe e by h·,·i we deno e he duali y p oduc be ween X0and X.
In pa icula , we ha e his con e gence o all w∗∈Lp0( 0, T ;X0). Then, uµ*
weakly in Lp( 0, T;X), and as we also ha e un* u weakly in Lp( 0, T ;X), hen
=u.
6
Then, uµ
∗
* u in L∞( 0, T;X) and by he ∗−weak lowe semicon inui y o he
no m, we ob ain
kukL∞( 0,T ;X)≤lim in
µ→∞ kuµkL∞( 0,T ;X)≤C. (13)
Now ix ∈[ 0, T]. By (13) he e exis s a sequence ( n)n∈Nin [ 0, T ] such ha
n→ and u( n)∈Xwi h ku( n)kX≤C o all n∈N.
As Xis e lexi e, he e exis a subsequence ( µ) and x∈Xsuch ha u( µ)* x
weakly in X. The inclusion X⊂Yis assumed o be con inuous and so,
u( µ)* x weakly in Y. (14)
Due o u∈C0([ 0, T]; Y), we ha e in addi ion ha u( n)→u( ) in Y. This
implies u( ) = x∈X.
Finally he weak lowe semi-con inui y o he no m implies o e e y ∈[ 0, T ]
ku( )kX=kxkX≤lim in
µ→∞ ku( µ)kX≤C
4 Exis ence o weak solu ions
P oposi ion 8 Suppose ha hypo heses (a)–(c)hold o F:L2(Ω) →L2(Ω).
Then, o e e y u0∈L2(Ω), he e exis s a weak solu ion u∈L20, T;H1
0(Ω)
o p oblem (4). Mo eo e , ubelongs o C0[0, T]; L2(Ω)and, u|(0,T ]is locally
bounded in H1
0(Ω).
Fu he mo e, i Fis locally Lipschi z as in hypo hesis (d), hen he weak solu-
ion is unique.
P oo . The p oo is based on a sequence o Gale kin app oxima ions and he
a p io i es ima es in §3. Le {wk, k ≥1}be an o hogonal basis o H1
0(Ω) as in
Rema k 1 and o each n∈N, conside a solu ion un( ) =
n
X
k=1
unk( )wko (11).
Fix s0∈(0, T) a bi a ily.
By P oposi ion 3, he sequence (un)n∈Nis bounded in L20, T ;H1
0(Ω)Due o
Lemma 5, (u0
n)n∈Nis bounded bo h in L2s0, T ;L2(Ω)and L2(0, T ;H−1(Ω)).
Hence Alaoglu’s Theo em p o ides a subsequence (again deno ed by) (un)n∈N
and unc ions u∈L20, T;H1
0(Ω), ∈L2s0, T;L2(Ω),w∈L20, T;H−1(Ω)
wi h
un−→ uweakly in L20, T;H1
0(Ω)
u0
n−→ weakly in L2s0, T;L2(Ω)
u0
n−→ wweakly in L20, T;H−1(Ω).
7
In pa icula , u0= =wholds Lebesgue-almos e e ywhe e, which a simple
check o he dis ibu ional de i a i e p ope y e eals. This implies ha u∈
L2(0, T;H−1(Ω)) ∩C0[0, T]; L2(Ω). S anda d a gumen s conclude u(0) = u0
om un(0) −→ u0in L2(Ω) o n→ ∞ (see e.g. [7, §7.1]).
The sequence (un)n∈Nis equi–con inuous in C0[s0, T ]; L2(Ω)by Lemma 6.
Mo eo e , he se un( ) ∈[s0, T], n ∈Nis ela i ely compac in L2(Ω)
as a consequence o Lemma 5 and he Sobole Embedding Theo em. Hence
he A zel`a–Ascoli Theo em p o ides a u he subsequence (again deno ed by)
(un)n∈Nwi h
un( )−→ u( ) in L2(Ω) uni o mly o ∈[s0, T].
Hypo hesis (a) on he con inui y o Fimplies ha F(un( )) → F(u( )) in L2(Ω)
o e e y ∈[s0, T].
Taking he limi as n→∞gi es ha u∈L2s0, T;H1
0(Ω)is a weak solu ion
o he pa ial di e en ial equa ion in p oblem (4) wi h u0∈L2s0, T;H−1(Ω).
Finally, u|[s0,T ]: [s0, T ]→H1
0(Ω) is bounded due o P oposi ion 4.
I Fsa is ies he local Lipschi z condi ion (d) in addi ion he uniqueness o
he weak solu ion ollows by a s anda d a gumen .
5 The mul i alued semi low o weak solu ions
De ine ΦF: [0,∞)×L2(Ω) → PL2(Ω), whe e PL2(Ω)consis s o all
nonemp y subse s o L2(Ω), by
ΦF( , u0) := u( )∈L2(Ω) ∃u(·)∈L20, ;H1
0(Ω):
u0∈L20, ;H−1(Ω), u(0) = u0and
uis weak solu ion o (4) in Ω ×(0, ).
(15)
I is clea ha his mul i alued map ΦF o ms a s ic mul i alued semi low on
L2(Ω) as in he he ollowing de ini ion o Kapus yan e al. [9, De ini ion 2.1].
De ini ion 9 Le (X, d)be a me ic space and, P(X)consis s o all i s
nonemp y subse s.
A map Φ : [0,∞)×X→ P(X)is called s ic mul i alued semi low (m–semi-
low) on Xi i sa is ies he ollowing condi ions:
(A) Φ(0, x) = {x} o all x∈X
(B) Φ( +s, x) = Φ( , Φ(s, x)) o all s, ≥0, x ∈X.
Rema k 10 Kapus yan e al. [9, De ini ion 2.1] de ine, in ac , a mo e gen-
e al m–semi low Φ : [0,∞)×X→ P(X), which sa is ies condi ion (A), bu
8
ins ead o he equali y condi ion (B), sa is ies he ollowing weake inclusion
condi ion
(C) Φ( +s, x)⊂Φ( , Φ(s, x)) o all s, ≥0, x ∈X.
The eason is ha he coun e pa o he se alued mapping ΦFabo e o many
sys ems, in pa icula he 3-dimensional Na ie –S okes equa ions, is es ic ed
o weak solu ions ha sa is y an ene gy inequali y. Howe e , such ene gy in-
equali ies only hold (o can only be p o ed o hold) o almos all ime ins an s.
Hence a conca en a ion o weak solu ions sa is ying he ene gy inequali y on ad-
jacen ime in e als may no sa is y he ene gy inequali y on he conca ena ed
ime in e al, which means ha he s ic p ope y (B) need no hold. see also
Mo illas & Vale o [12]. This si ua ion does no a ise o he mapping ΦFde ined
abo e o he p oblem (4) unde conside a ion in his pape .
E e y s ic mul i alued semi low Φ : [0,∞)×X→ P(X) (in he sense
o De ini ion 9) induces a map ˜
Φ : [0,∞)× P(X)→ P(X) in he ollowing
canonical way:
˜
Φ( , M)De .
=[
x∈M
Φ( , x) o all nonemp y M⊂X.
Ob iously, i sa is ies he co esponding condi ions
(A∗)˜
Φ(0, M) = M o all M∈ P(X)
(B∗)˜
Φ( +s, M) = ˜
Φ( , ˜
Φ(s, M)) o all s, ≥0, M ∈ P(X)
o in he gene al nons ic case
(C∗)˜
Φ( +s, M)⊂˜
Φ( , ˜
Φ(s, M)) o all s, ≥0, M ∈ P(X)
Hence one usually does no dis inguish be ween ˜
Φ and Φ.
5.1 Global a ac o s o mul i alued semi lows:
Gene al esul s
De ini ion 11 Aglobal a ac o o a s ic mul i alued semi low Φon a me ic
space (X, d)is a nonemp y subse Ao Xwhich is Φ-in a ian , i.e. Φ( , A) =
A o all ≥0, and a ac s e e y bounded subse Bo X, i.e.
dis X(Φ( , B), A)→0as → ∞,
whe e dis Xis he Hausdo semi–dis ance on P(X). Fo a gene al non-s ic
mul i alued semi low he a ac o Ais only equi ed o be Φ-nega i ly in a ian ,
i.e. A⊂Φ( , A) o all ≥0 [11, De ini ion 6].
The exis ence o a global a ac o is usually concluded om he compac ness
o asymp o ic compac ness o he mul i alued mapping Φ( , ·) o > 0:
9
we obse e ha i we conside m≥1, we ha e
ZΩ|u|mdx ≤|Ω|
|B(0; δ)|m/2kukm
L2(Ω) . (18)
We also ob ain
ZΩ
(F(u))2dx ≤C|Ω|
|B(0; δ)|kuk2
L2(Ω)
+C|Ω|
|B(0; δ)|2kuk4
L2(Ω)
+2C|Ω|
|B(0; δ)|3/2kuk3
L2(Ω) ,
and hen we ha e (7) wi h ΦkukL2(Ω)=C|Ω|
|B(0;δ)|kuk2
L2(Ω) +C|Ω|
|B(0;δ)|2kuk4
L2(Ω) +
2C|Ω|
|B(0;δ)|3/2kuk3
L2(Ω).
We obse e ha i u∈L2(Ω), hen F(u)∈L∞(Ω) ⊂L2(Ω) .
Now, we p o e ha Fis con inuous. We suppose ha un−→ us ongly
in L2(Ω), hen we ha e o p o e ha F(un)−→ F(u) s ongly in L2(Ω). I
is su icien o p o e ha he e exis s {uµ}⊂{un}such ha F(uµ)−→ F(u)
s ongly in L2(Ω).
As un−→ us ongly in L2(Ω), hen (see [4]) he e exis s {uµ}⊂{un}such
ha
uµ(x)−→ u(x) a.e. in Ω.
Then, as is con inuous we ha e
(uµ(x)) −→ (u(x)) a.e. in Ω. (19)
We obse e ha a guing as be o e we ob ain
|uµ(x)−u(x)|=1
|B(x;δ)|ZB(x;δ)∩Ω
(uµ(y)−u(y)) dy
≤1
|B(0; δ)|1/2kuµ−ukL2(Ω) −→ 0,
and hen
uµ(x)−→ u(x) a.e. in Ω. (20)
F om (19) and (20) we ha e
F(uµ)(x)−→ F(u)(x) a.e. in Ω. (21)
16
On he o he hand, we obse e ha kuµkL2(Ω) is bounded because Ω is a
bounded domain and uµ−→ us ongly in L2(Ω). Then, we ha e
|F(uµ(x))| ≤ C|uµ(x)||1−uµ(x)|(22)
≤C1
|B(0; δ)|1/2kuµkL2(Ω) 1 + 1
|B(0; δ)|1/2kuµkL2(Ω)!
≤e
C,
whe e e
Cis a posi i e cons an .
Then, om (21), (22) and by he Domina ed Con e gence Theo em, we
oba in
F(uµ)−→ F(u) s ongly in L2(Ω) ,
hen Fis con inuous.
F om Theo em 8 we ha e ha he e exis s a weak solu ion u∈L20, T ;H1
0(Ω)
o p oblem (16) wi h u0∈L20, T;H−1(Ω).Acco ding o Theo em 15, he
p oblem (16) de ines a mul i alued semi low in L2(Ω), which possesses a com-
pac global a ac o A. Also, Ais he minimal closed a ac ing se .
7 P oo s o he dissipa i i y es ima es
P oo o P oposi ion 3. The uni o m ellip ici y condi ion o he linea
ope a o Aand assump ion (b) on he nonlocal ope a o Fused in he ene gy
equali y, 1
2
d
d kuk2
L2(Ω) +ZΩ
u(A u)dx =ZΩ
uF(u)dx (23)
gi e 1
2
d
d kuk2
L2(Ω) +λAk∇uk2
L2(Ω) ≤βkuk2
L2(Ω) +Cβ.(24)
Hence, by he Poinca ´e inequali y (3),
1
2
d
d kuk2
L2(Ω) +λΩλAkuk2
L2(Ω) ≤βkuk2
L2(Ω) +Cβ.
i.e.,
d
d kuk2
L2(Ω) ≤M−Lkuk2
L2(Ω) , (25)
whe e M:= 2 Cβ>0 and L:= 2 λΩλA−2β > 0.
Mul iplying by eL , and in eg a ing be ween 0 and , i ollows
eL ku( )k2
L2(Ω) ≤ ku(0)k2
L2(Ω) +MZ
0
eLs ds
≤ ku(0)k2
L2(Ω) +MZ
−∞
eLs ds,
17
i.e., o e e y ∈[0, T],
ku( )k2
L2(Ω) ≤M
L+e−L ku(0)k2
L2(Ω) . (26)
Finally, in eg a ing equa ion (24) wi h espec o ime, we ob ain
λAZ
0k∇uk2
L2(Ω) ds
≤1
2ku0k2
L2(Ω) −ku( )k2
L2(Ω)+βZ
0kuk2
L2(Ω) ds +Cβ
≤ ku0k2
L2(Ω) 1
2+βZ
0
e−L s ds+Cβ+βM
L .
P oo o Lemma 5. Le {wk:k≥1}deno e an o hogonal basis o H1
0(Ω)
as men ioned in Rema k 1. Fo each n≥1, le
un( ) =
n
X
k=1
unk( )wk,
be a Gale kin app oxima ion o p oblem (4) sa is ying he ini e dimensional
sys em o o dina y di e en ial equa ions in he sense ha
(d
d (un( ), wk) + hAun( ), wki= (F(un( )), wk)
(un(0), wk)=(u0, wk), k = 1, . . . , n.
(27)
We obse e ha
Aun( ) =
n
X
k=1
unk( )Awk=
n
X
k=1
unk( )λkwk∈span {w1, . . . , wn}.
Then, mul iplying equa ion (27) by unk( )λk, summing om k= 1 o n, and
using p ope y (c) o F, gi es
hu0
n( ), Aun( )i+kAun( )k2
L2(Ω) = (F(un( )), Aun( ))
≤1
2kF(un( ))k2
L2(Ω) +kAun( )k2
L2(Ω)
≤Ψ(un( )) + 1
2kAun( )k2
L2(Ω) (28)
18
o Lebesgue-almos all ∈[0, T ]. On he o he hand,
hu0
n( ), Aun( )i=−ZΩ
N
X
i,j=1
∂xjaij(x)∂xiunu0
ndx (29)
=
N
X
i,j=1 ZΩ
aij(x)∂xiun(∂ ∂xjun)dx
=d
d 1
2·A[un, un](30)
o he symme ic bilinea o m
A[u, ] := ZΩ
N
X
i,j=1
aij(x)∂xiu ∂xj dx,u, ∈H1
0(Ω).
since i is assumed ha aij =aji, wi h i, j = 1, .., N, and hese coe icien s do
no depend on .
In eg a ing om sand , hen gi es
1
2·A[un( ), un( )] ≤1
2·A[un(s), un(s)] + Z
s
Ψkun(ξ)kL2(Ω)dξ. (31)
Hence, i ollows om he inequali ies o coe ci i y and con inui y
λAk∇un(s)k2
L2(Ω) ≤ A[un(s), un(s)] ≤ΛAk∇un(s)k2
L2(Ω)
ha
λA
2·k∇un( )k2
L2(Ω) ≤ΛA
2·k∇un(s)k2
L2(Ω) +Z
s
Ψkun(ξ)kL2(Ω)dξ. (32)
In eg a ing now he a iable sbe ween 0:= max{0, −1}and , gi es
λA
2·min{ , 1}·k∇un( )k2
L2(Ω) ≤ΛA
2Z
max{0, −1}k∇un(s)k2
L2(Ω) ds +
Z
max{0, −1}
Ψkun(s)kL2(Ω)ds.
On he o he hand, in eg a ing (24) wi h espec o ime in [ 0, ], i ollows ha
kun( )k2
L2(Ω) −kun( 0)k2
L2(Ω) + 2 λAZ
0k∇un(s)k2
L2(Ω) ds
≤2βZ
0kun(s)k2
L2(Ω) ds + 2 Cβ.
19
Then, using P oposi ion 3,
ΛAZ
0k∇un(s)k2
L2(Ω) ds ≤ΛA
2β+ 1
2λA
sup
s∈[ 0, ]kun(s)k2
L2(Ω) +CβΛA
λA
≤C2·1 + e−L ku0k2
L2(Ω)(33)
o all ≥0 wi h a cons an C2=C2(β, ΛA, λA, λΩ, Cβ)>1. Thus, whene e
ku0kL2(Ω) ≤ρ,
k∇un( )k2
L2(Ω) ≤2C2
λAmin{ , 1}1 + e−L ρ2+ ΨM
L+e−L ρ2.(34)
Mo eo e , his uppe bound holds o e e y ∈(0, T] — in con as o he
immedia e consequence o inequali y (28) and he coe ci i y o A.
The nex s ep is o es ablish an es ima e o ku0
nkL∞(0,T ;H−1(Ω)). This ol-
lows essen ially he a gumen s o he s anda d ene gy es ima e, aking he
p eceding a p io i bounds in o conside a ion.
Fo e e y ∈H1
0(Ω), he e is a unique ep esen a ion = 1+ 2wi h 1∈
span{w1, . . . , wn}and ( 2, wk) = 0 o k= 1, . . .,nsince {wk, k ≥1}is an
o hono mal basis o L2(Ω).
Fo Lebesgue-almos e e y ∈[0, T ] i ollows ha
u0
n( ), 1+Aun( ), 1=F(un( )), 1
hu0
n( ), i= (u0
n( ), ) = u0
n( ), 1
=F(un( )), 1−Aun( ), 1
≤(kF(un( ))kL2+ ΛAk∇un( )kL2)k 1kH1
0(Ω).
Then, inequali y (7) in assump ion (c) o Fimplies ha
hu0
n( ), i ≤ pΨ (kun( )kL2)+ΛAk∇un( )kL2k 1kH1
0(Ω).
Hence, in iew o he es ima es (26) and (34),
ku0
n( )kH−1(Ω) ≤pΨ (kun( )kL2)+ΛAk∇un( )kL2
≤cons β, Cβ,ΛA, λA, λΩ,ku0kL2(Ω).
Finally, mul iplying (27) by u0
nk( ) and summing om k= 1 o n, i ollows
20
om inequali y (10) in assump ion (c) o F ha
hu0
n( ), u0
n( )i+hAun( ), u0
n( )i= (F(un( )), u0
n( ))
≤ kF(un( ))k2
L2(Ω) +1
4ku0
n( )k2
L2(Ω)
≤Ψkun( )kL2(Ω)+1
4ku0
n( )k2
L2(Ω).
Using (30), his can be e o mula ed as
ku0
n( )k2
L2(Ω) +d
d 1
2A[un, un]≤Ψkun( )kL2(Ω)+1
4ku0
n( )k2
L2(Ω)
i.e., o Lebesgue-almos e e y ∈[0, T ],
ku0
n( )k2
L2(Ω) +d
d A[un, un]≤2 Ψkun( )kL2(Ω).
Now ix s0∈(0, T[ a bi a ily and in eg a e be ween s0and T o ob ain
ZT
s0ku0
n(ξ)k2
L2(Ω) dξ +A[un(T), un(T)] ≤A[un(s0), un(s0)]
+ 2 ZT
s0
Ψkun(ξ)kL2(Ω)dξ.
The gene al inequali ies o coe ci i y and con inui y
0≤λAk∇un( )k2
L2(Ω) ≤ A[un( ), un( )] ≤ΛAk∇un( )k2
L2(Ω) ,
imply ha
ZT
s0ku0
n(ξ)k2
L2(Ω) dξ ≤ΛAk∇un(s0)k2
L2(Ω) + 2 ZT
s0
Ψkun(ξ)kL2(Ω)dξ.
Hence, om he es ima es (26), (34) and he mono onici y o Ψ one concludes
ha
ZT
s0ku0
n(ξ)k2
L2(Ω) dξ ≤cons (β, ΛA, λA, λΩ, Cβ, s0, T, ku0kL2(Ω)).
Finally, H¨olde ’s inequali y gua an ees he claimed inequali y o e e y s, ∈
[s0, T] wi h s< , i.e.,
Z
sku0
n(ξ)kL2(Ω) dξ ≤cons β, ΛA, λA, λΩ, Cβ, s0, T, ku0kL2(Ω)·√ −s .
21
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