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Asymptotic behaviour of nonlocal reaction-diffusion equations

Anguiano Moreno, María; Kloeden, Peter E.; Lorenz, Thomas

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 ∂xjaij(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∈ LH1 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) ≤ΨkukL2(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 ΨkukL2(Ω).(9) kF(u)k2 L2(Ω) ≤e ΨkukH1,2(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∈ L20, T;H1 0(Ω)o (4) wi h u0∈L20, 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∈L20, T ;H1 0(Ω)o (4) wi h u0∈L20, 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+ ΨC1·(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+ ΨC1(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∈L20, T;H1 0(Ω)and u0∈ L20, 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( ), wkwk 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 L20, T;H1 0(Ω) and, i s weak limi is u∈L20, 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∈L20, T;H1 0(Ω)o (4) wi h u0∈L20, 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∈L20, 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 L20, T ;H1 0(Ω)Due o Lemma 5, (u0 n)n∈Nis bounded bo h in L2s0, 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∈L20, T;H1 0(Ω), ∈L2s0, T;L2(Ω),w∈L20, T;H−1(Ω) wi h          un−→ uweakly in L20, T;H1 0(Ω) u0 n−→ weakly in L2s0, T;L2(Ω) u0 n−→ wweakly in L20, 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 ∈Nis 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∈L2s0, 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∈L2s0, 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) → PL2(Ω), whe e PL2(Ω)consis s o all nonemp y subse s o L2(Ω), by ΦF( , u0) := u( )∈L2(Ω) ∃u(·)∈L20, ;H1 0(Ω): u0∈L20, ;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 ΦkukL2(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∈L20, T ;H1 0(Ω) o p oblem (16) wi h u0∈L20, 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 2ku0k2 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 2kF(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 ∂xjaij(x)∂xiunu0 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 Ψkun(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 Ψkun(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} Ψkun(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+ ΨM 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( )kL2k 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) ≤Ψkun( )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]≤Ψkun( )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 Ψkun( )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 Ψkun(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 Ψkun(ξ)kL2(Ω)dξ. 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