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Contents lists available atScienceDirect

Differential Geometry and its Applications

www.elsevier.com/locate/difgeo

Harnack estimates for a nonlinear parabolic equation under Ricci flow

Yi Lia,, Xiaorui Zhub,c

a FacultyofScience,TechnologyandCommunication(FSTC),MathematicResearchUnit,Campus Belval,UniversiteduLuxembourg,MaisonduNombre,6,avenuedelaFonte,L-4364,Esch-sur-Alzette, Luxembourg

bCenterofMathematicalSciences,ZhejiangUniversity,Hangzhou,310027, China

cChinaMaritimePoliceAcademy,Ningbo,315801, China

a r t i cl e i n f o a b s t r a c t

Articlehistory:

Received7September2016 Availableonlinexxxx CommunicatedbyF.Fang

MSC:

53C44

Keywords:

Nonlinearparabolicequation Harnackestimate

Ricciflow

Inthispaper,weconsidertheHarnackestimatesforanonlinearparabolicequation undertheRicciflow.ThegradientestimatesforpositivesolutionsaswellasLi–Yau typeinequalitiesarealsogiven.

©2017ElsevierB.V.Allrightsreserved.

1. Introduction

Thenonlinearparabolicequationisaclassicalsubjectthathasbeen extensivelystudied,whichleadsto lotsofimportantresultsespeciallyinresearchesofdifferentialgeometry.Oneoftheimportanttechniquein studying theheatequation isthedifferential HarnackinequalitydevelopedbyLiandYau[7].This isalso appliedtoRicciflowbyHamilton[6],andplaysanimportantroleinsolvingthePoincaréconjecture[9].

NowwewillstudythecasewhereMisacompletemanifoldwithoutboundary.Considerpositivesolutions ofanonlinearparabolicequationonthemanifoldM,whichevolvesundertheRicciflow.A seriesofgradient estimatesareobtainedforsuchsolutions,includingseveralLi–Yau-typeinequalities.Let(M,g(t))t∈[0,T] be acompletesolutiontotheRicciflow

YiLi is partiallysupportedby theFondsNational de laRecherche Luxembourg (FNR)under the OPENscheme (project GEOMREVO14/7628746).XiaoruiZhuispartiallysupportedbyCPSF(grant)No.2014M551721andZhejiangProvinceNatural ScienceFoundationofChina(grant)No.Q14A010002.

* Correspondingauthor.

E-mailaddresses:[email protected](Y. Li),[email protected](X. Zhu).

https://doi.org/10.1016/j.difgeo.2017.10.017 0926-2245/©2017ElsevierB.V.Allrightsreserved.

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tg(t) =−2Ricg(t), t∈[0, T]. (1.1) WeassumethatitsRiccicurvatureremainsuniformlyboundedforallt∈[0,T].Considerapositivefunction u=u(x,t) definedon[0,T] solvingtheequation

Δg(t)−q−∂t

u=au(lnu)α, t∈[0, T], (1.2)

which hasbeen firststudiedin[14]where g(t)≡g is afixedmetric.Qian[10] and Wu[13] gotaseries of similar conclusions.HereΔg(t) standsfortheLaplacianof g(x,t) definedon[0,T] and q(x,t) isaC2 functiondefinedon[0,T].NoticethattheLaplacianΔg(t)dependsontheparametert,andweshould study thenonlinearparabolic equation (1.2)coupledwiththeRicciflow (1.1).Theformula (1.1)provides us withadditionalinformationaboutthecoefficientsoftheoperatorΔ appearingin(1.2)butisitselffully independent of(1.2).

2. Gradientestimates I:α= 1

Firstly, we introduce a cut-off function (see [1,3,7,8,14]) on Bρ,T := {(χ,t) M × [0,T] : distg(t)(χ,x0) < ρ}, where distg(t)(χ,x0) stands for the distance between χ and x0 with respect to the metricg(t),whichsatisfiesa basicanalyticalresultstatedinthefollowing lemma.

Lemma2.1. Givenτ (0,T],thereexistsasmoothfunctionΨ : [0,)×[0,T]→Rsatisfying thefollowing requirements:

(1) ThesupportofΨ(r,t)isasubsetof [0,ρ]×[0,T],0Ψ(r,t)≤1in[0,ρ]×[0,T],andΨ(r,t)= 1holds in[0,ρ2]×[τ,T].

(2) Ψisdecreasing asaradialfunctionin thespatialvariables.

(3) The estimate |∂tΨ|≤ CτΨ1/2 issatisfiedon[0,)×[0,T] forsomeC >0.

(4) The inequalities−CραΨα≤∂rΨ0and|∂r2Ψ|≤Cρ2αΨα holdon[0,)×[0,T]forevery a∈(0,1) with someconstant Cα dependenton a.

Proof. See[1]. 2

ThesepropertiesarederivedfromCalabi’sargument(see,e.g.,[2,4,11]).Usingthisauxiliaryfunctionand applyingthemaximumprinciple,weareabletoestablishLi–Yau-typeinequalityforthesystem(1.1)–(1.2).

Theorem2.2.Supposethat(M,g(t))t∈[0,T]isacompletesolutiontotheRicciflow(1.1)onann-dimensional manifoldMwithsupBρ,T |Ricg(t)|g(t)≤KforsomeK >0,anduisasmoothpositivefunctiononM×[0,T] satisfyingthenonlinearparabolicequation (1.2)wherethefunctionq(x,t)isdefined onM×[0,T]whichis C2 in thex-variable andC1 inthet-variable.Ifu(x,t)≤1on Bρ,T= 1,|∇g(t)q|g(t)≤γ,and

b:= 1

8+ min

M×[0,T]q−max{a,0}>0, then thereexistsaconstant C that dependsonly onnsuchthat

|∇g(t)u|g(t)

u ≤C

b 1

ρ+ 1

√t +

K+ 1 +√γ+

|a| 1 + ln1 u

(2.1) on Bρ/2,T with t= 0.

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Whenqisnonnegativeanda≤0,theconstantC/bcanbeauniversalconstantwhichmeansaconstant dependingonlyonthedimensionn.Thenumber1/8 inbisnotessential,becauseinthefollowingproofwe shallseethatwecanreplace1/8 by 1.Toprovetheabovetheorem,weneedthefollowingcrucial lemma.

Lemma2.3.Let(M,g(t))t∈[0,T] beacomplete solutiontotheRicciflow (1.1)onann-dimensionalmanifold MwithsupBρ,T |Ricg(t)|g(t)≤KforsomeK >0,anduisasmoothpositivefunctiononM×[0,T]satisfying thenonlinearparabolic equation (1.2) with α= 1,a<0.Weassume that u≤1 onBρ,T.If f := lnu and w:=|∇g(t)ln(1−f)|2g(t)=|∇g(t)f|2g(t)/(1−f)2,thentheinequality

−∂t)w≥ 2f

1−f∇f,∇w+ 2(1−f)w2 +2∇f,∇q

(1−f)2 + 2a |∇f|2

(1−f)2 +2|∇f|2(q+af)

(1−f)3 (2.2)

holdson Bρ,T.

Proof. Sinceuisapositivesolutionto thenonlinearparabolicequation (1.2)withα= 1 anda<0,direct calculationshowsthat

Δf +|∇f|2−ft−q−af = 0, ft:=tf.

Thepartialderivativeofwwithrespect tot isgivenby wt= 2∇f,∇ft

(1−f)2 +2|∇f|2ft

(1−f)3 +2Ric(∇f,∇f) (1−f)2

= 2∇f,∇(Δf +|∇f|2−q−af)

(1−f)2 +2Ric(∇f,∇f) (1−f)2 + 2|∇f|2(Δf+|∇f|2−q−af)

(1−f)3 .

UsingBochner’sidentity ∇f,∇Δf=∇f,Δ∇f−Ric(∇f,∇f) weobtain wt= 2∇f,Δ∇f+ 2∇f,∇(|∇f|2−q−af)

(1−f)2 +2|∇f|2(Δf+|∇f|2−q−af) (1−f)3 . Thepartialderivativeofwwithrespect toxisgivenby

Δw= 2 |∇2f|2

(1−f)2 + 2∇f,Δ∇f

(1−f)2 + 4∇f,∇|∇f|2

(1−f)3 + 6 |∇f|4

(1−f)4 + 2|∇f|2Δg(t)f (1−f)3 . Combiningthose partialderivativesimply

−∂t)w= 2 |∇2f|2

(1−f)2 + 4∇f,∇|∇f|2

(1−f)3 + 6 |∇f|4

(1−f)4 2∇f,∇|∇f|2 (1−f)2

2 |∇f|4

(1−f)3 + 2a |∇f|2

(1−f)2 + 2∇f,∇q

(1−f)2 + 2 q|∇f|2

(1−f)3+ 2a f|∇f|2 (1−f)3. Ontheotherhand,thegradientterm∇f,∇wisdeterminedby

∇f,∇w=∇f,∇|∇f|2g(t)

(1−f)2 + 2 |∇f|4 (1−f)3.

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Pluggingitinto theevolutionof (Δ−∂t)wweconcludethat (Δ−∂t)w= 2 |∇2f|2

(1−f)2 + 2∇f,∇|∇f|2 (1−f)3 + 2

1−f∇f,∇w+ 2 |∇f|4 (1−f)4

2∇f,∇w+ 2 |∇f|4

(1−f)3 + 2a |∇f|2 (1−f)2 + 2∇f,∇q

(1−f)2 + 2 q|∇f|2

(1−f)3+ 2a f|∇f|2 (1−f)3. Because oftheidentity

|∇2f|2

(1−f)2 +∇f,∇|∇f|2

(1−f)3 + |∇f|4 (1−f)4 =

2f

1−f +∇f⊗ ∇f (1−f)2

2

we thereforearriveat (Δ−∂t)w= 2

2f

1−f +∇f⊗ ∇f (1−f)2

2+ 2

1−f∇f,∇w+ 2 |∇f|4

(1−f)3 2∇f,∇w + 2∇f,∇q

(1−f)2 + 2a |∇f|2

(1−f)2 +2|∇f|2(q+af) (1−f)3 whichimmediately implies

−∂t)w≥ 2f

1−f∇f,∇w+ 2|∇f|4

(1−f)3 +2∇f,∇q

(1−f)2 +2a|∇f|2

(1−f)2 +2|∇f|2(q+af) (1−f)3 . This completetheproof. 2

Proof of Theorem 2.2. Pick a number τ (0,T] and fix a function Ψ(x,t) satisfying the conditions of Lemma 2.1.Wewillestablish(2.1)at(x,τ) forallxsuchthatdistg(τ)(x,x0)< ρ2.DefineΨ:[0,T]R bysetting

Ψ(x, t) := Ψ

distg(t)(x, x0), t .

Then, using(2.2)andastraightforwardcalculation,onehas (Δ−∂t) (Ψw)ΨΛ,∇w+

2(1−f)w2+2∇f,∇q

(1−f)2 + 2a |∇f|2 (1−f)2 + 2|∇f|2(q+af)

(1−f)3 Ψ + 2∇w,∇Ψ+wΔΨ−w∂tΨ

≥ −Λ,(Ψw)+ 2Ψ(1−f)w2+wΛ,Ψ +wΔΨ−wΨt+ 2

ΨΨ,(Ψw)2|∇Ψ|2

Ψ w

+

2∇f,∇q

(1−f)2 + 2a |∇f|2

(1−f)2 +2|∇f|2(q+af) (1−f)3 Ψ

where Λ=1−f2f ∇f. Byourassumptionthat|Ric|≤K onBρ,T andLemma 2.1thatCρ1Ψ1/2Ψr0, and theidentity

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−wΨt=

Ψt+ Ψrtdistg(t)(·, x0) w, wehave(because−∂tdistg(t)(·,x0)4

(m1)K,cf. Lemma 8.33in[5])

−wΨt≥ −Ψtw−4C1

(m1)K ρ 1/2.

SupposethatΨw achievesitsmaximumat(x0,t0).By[7],withoutloss ofgenerality,wemayassumethat x0isnotinthecut-locusofM.Atthepoint(x0,t0),onehasΔ(Ψw)0,(Ψw)= 0,(Ψw)t0.Therefore

2Ψ(1−f)w2≤ −wΛ,Ψ+ 2|∇Ψ|2

Ψ w−wΔΨ +wΨt

2∇f,∇q

(1−f)2 + 2a |∇f|2

(1−f)2+2|∇f|2(q+af)

(1−f)3 Ψ (2.3)

at(x0,t0).Weneedtobound eachtermontheright-handsideof(2.3):

|wΛ,Ψ| ≤2w|f|

1−f|∇f||∇Ψ|= 2w3/2|f||∇Ψ| ≤Ψ(1−f)w2+27 16

|f|4|∇Ψ|4 [Ψ(1−f)]3

where we used theYoung’s inequality thatab ≤ap+bq/(q(p)q/p) for any a,b,> 0 andp,q > 1 with p−1+q−1= 1.Thistogetherwith Lemma 2.1implies

|wΛ,Ψ| ≤Ψ(1−f)w2+C2

f4

ρ4(1−f)3. (2.4)

UsingagainLemma 2.1wehave

|∇Ψ|2

Ψ w= Ψ1/2w|∇Ψ|2 Ψ3/2 1

8Ψw2+ 2|∇Ψ|4 Ψ3 1

8Ψw2+C3

ρ4. (2.5)

Furthermore,bythepropertiesofΨ andtheassumption oftheRiccicurvature, onehas(cf.,[12,15])

−wΔΨ≤ 1

8Ψw2+C4

ρ4 +C4K2. (2.6)

Theestimationfortisgiven by(cf. [1])

|wΨt| ≤1

8Ψw2+C5

τ2 +C5K2. (2.7)

Sincef 0 it followsthat

2∇f,∇q (1−f)2 Ψ

|∇f|2+|∇q|2

(1−f)2 Ψ wΨ +γ2Ψ

1

8Ψw2+ (2 +γ2)Ψ, (2.8)

2a |∇f|2 (1−f)2Ψ

= 2awΨ 1

8Ψw2+ 2a2Ψ (2.9)

and

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2|∇f|2(q+af)

(1−f)3 Ψ = 2Ψw2 −q

1−f +a −f 1−f

2Ψw2

min

M×[0,T]q+a −f 1−f

(2.10)

2

max{a,0} − min

M×[0,T]q

Ψw2. Substituting(2.5)–(2.10)totheright-handsideof(2.3),wededucethat

Ψ(1−f)w2≤C6

f4

ρ4(1−f)3 +3

4Ψw2+ 2

max{a,0} − min

M×[0,T]q

Ψw2 + C6

τ2 +C6

ρ4 +C6K2+

2 +γ2+ 2a2 at (x0,t0).Sincef <0,thenf4/(1−f)41.Itfollowsthat

1

4+ 2 min

M×[0,T]q−2 max{a,0}

Ψw2 2C6

ρ4 +C6

τ2 +C6K2+

2 +γ2+ 2a2 at (x0,t0).When

1

8+ min

M×[0,T]q−max{a,0}>0 (2.11) we canconcludethat

Ψw2 C7

1

8+ minM×[0,T]q−max{a,0} 1

ρ4 + 1

τ2 +K2+ 1 +γ2+a2

at (x0,t0).BecauseΨ(x,τ)= 1 whendistg(τ)(x,x0)< ρ/2,wefinally arriveat w2(x, τ) C7

1

8+ minM×[0,T]q−max{a,0} 1

ρ4 + 1

τ2 +K2+ 1 +γ2+a2

onBρ/2,T,which,sinceτ∈(0,T] wasarbitrary,implies

|∇f|

1−f C8

1

8+ minM×[0,T]q−max{a,0} 1

ρ+ 1

√t+

K+ 1 + γ+

|a|

.

Wehavecompletedtheproof ofTheorem 2.2.

Thenumber1/8 in(2.11)isnotessential,becauseintheaboveargumentwecanreplace1/8 in(2.5)–(2.9) byagivenpositivenumber,and henceweneedonlyto requirethat

15+ 2 min

M×[0,T]q−2 max{a,0}>0 insteadof(2.11).When

1 + 2 min

M×[0,T]q−2 max{a,0} is positive,wechoosetobe thisnumberdividedby5.

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3. GradientestimatesII:generalcase

InthissectionweextendTheorem 2.2with α= 1 tothegeneralcase.

Lemma 3.1. Suppose (M,g(t))t[0,T] is a complete solution to the Ricci flow (1.1) on an n-dimensional manifold M, with −K1g(t) Ricg(t) ≤K2g(t) for some K1,K2 > 0 on Bρ,T. If u is a smooth positive function satisfying the nonlinear parabolic equation (1.2), then, for given β 1 and any c,d > 0 with c+d= 1/β,wehave

−∂t)F≥ −2∇f,∇F −F

t +2cβt n

|∇f|2−q−ft−afα2

2(β1)t∇f,∇q −2(β1)taαfα−1|∇f|2

−βtaα(α−1)fα−2|∇f|22βtK1|∇f|2−nβt

2d K2 (3.1)

−βaαtfα1

−|∇f|2+ft+q+afα

−βtΔq,

whereK:= max{K1,K2},f := lnu,andF :=t(|∇f|2−βft−βq−βafα).

Proof. Theproofofthislemmawasoriginal from[1].Nowwewillfindaconvenientbound onΔF like the wayin[16].Notice that

iF =t

2jf∇ijf−β∇ift−β∇iq−βaαfα−1if .

ThentheLaplaceofF equals

ΔF =iiF

=t

2|∇2f|2+ 2∇f,Δ∇f −βΔft−βΔq

−βaα

1)fα2|∇f|2+fα1Δf .

UsingtheBochner’sformulaΔ∇f =Δf+ Ric(∇f,·),weget ΔF=t

2|∇2f|2+ 2∇f,∇Δf+ 2Ric(∇f,∇f)−βΔft

−βΔq−βaα

1)fα−2|∇f|2+fα−1Δf

≥t

2(Δf)2

n + 2∇f,∇Δf2K1|∇f|2−β(Δf)t−βΔq

−βaα

1)fα2|∇f|2+fα1Δf

+ 2βRijijf since|∇2f|2 n1(Δf)2 andΔft= (Δf)t2Rijijf.Recallingfromtheresult

Δf =−|∇f|2+q+ft+afα=−F

t 1) (q+ft+afα), wearriveat

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ΔF 2cβt n

|∇f|2−q−ft−afα2

+ 2dβt

n (Δf)2+ 2tβRijijf

2t

∇f,∇ F

t + (β1)(q+ft+afα)

2K1t|∇f|2−tβ

−F

t 1)(q+ft+afα)

t

−βtΔq (3.2)

−βaαt

1)fα−2|∇f|2+fα−1Δf inthesetBρ,T.Because

2dβt

n (Δf)2+ 2tβRijijf =2dβt n

(Δf)2+n

dRijijf

=2dβt n

2f+ n

2dRic2−nβt 2d |Ric|2

≥ −nβt 2d|Ric|2, theinequality(3.2)canbe writtenas

ΔF 2cβt n

|∇f|2−q−ft−afα2

−nβt 2d|Ric|2

2t

∇f,∇ F

t + (β1)(q+ft+afα)

2K1t|∇f|2−tβ

−F

t 1)(q+ft+afα)

t

−βtΔq (3.3)

−βaαt

1)fα2|∇f|2+fα1Δf .

To getthetime derivativeofF,weshallusetheidentity Ft= F

t +t

|∇f|2−βft−βq−aβfα

t

.

Subtractingthisfrom (3.3),weget

−∂t)F≥ −2∇f,∇F −F

t +2cβt n

|∇f|2−q−ft−afα2

−βtΔq−2(β1)t∇f,∇q −nβt 2d |Ric|2

2(β1)taαfα−1|∇f|2−βtaα(α−1)fα−2|∇f|2

−βaαtfα−1

− |∇f|2+ft+q+afα

2βK1t|∇f|2.

Now theinequality(3.1)followsimmediately bynotingthat|Ricg(t)|2g(t)≤K2. 2

Nowwecanconsiderthelocalspace–timegradientestimatewithLemma 2.3.Inthefollowingpart,nis thedimensionofM.

Theorem3.2.Supposethat(M,g(t))t[0,T]isacompletesolutiontotheRicciflow(1.1)onann-dimensional manifold M with −K1g(t) Ricg(t) K2g(t) for some K1,K2 > 0 on Bρ,T. If u is a smooth positive

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functionsatisfyingthenonlinearparabolicequation (1.2),thenthereexistsaconstantC depending onlyon nsuch that,onBρ/2,T,

(1) fora≥0,wehave

|∇g(t)f|2g(t)−βft−βq−βafα

2c(1−)t+(A+γ)nβ

2c(1−) + n2β3C2 4c2(1−)(β−1)ρ2 + nβ[βK1+a(β−1)α|fα−1|]

c(1−)(β−1) + 2aα|α−1||fα2|

2c(β1)(1−) +

[βθ+ (β1)γ+2dK2]nβ

2c(1−) ,

(2) fora≤0,wehave

|∇g(t)f|2g(t)−βft−βq−βafα

2c(1−)t+(A+γ)nβ

2(1−c) + n2β3C12 4c2(1−)(β−1)ρ2 + nβ[βK1a21)α|fα1|]

c(1−)(β−1) +

[βθ+ (β1)γ+2dK2]nβ

2c(1−) .

Heref := lnu,|f|:= maxM|f|,K:= max{K1,K2},β >1,0< <1,|∇g(t)q|g(t)≤γ,Δg(t)q≤θ, A=C

1 ρ2 +

√K1 ρ +1

t +K

andc,d>0with c+d= 1/β.

Proof. Wewill usethesamenotation f = lnuandF =t(|∇f|2−βft−βq−βafα) as inLemma 3.1.For thefixedτ (0,T],chosethecut-offfunctionΨ constructedinLemma 2.1. DefineΨ:[0,T]→R by setting

Ψ(x, t) = Ψ

distg(t)(x, x0), t .

Lemma 3.1impliesthat

−∂t) (ΨF)≥ −2∇f,∇(ΨF)+ 2F∇f,∇Ψ +

2cβt n

|∇f|2−q−ft−afα2

−F

t βtΔq

2(β1)t∇f,∇q −2(β1)taαfα1|∇f|2

−βtaα(α−1)fα−2|∇f|22βtK1|∇f|2−nβt 2d K2

−βaαtfα−1

−|∇f|2+ft+q+afα Ψ +FΔΨ + 2

ΨΨ,(ΨF)2|∇Ψ|2

Ψ F−F∂Ψ

∂t.

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Let(x0,t0) beamaximumpointforthefunctionΨF intheset{(x,t)|0≤t≤τ,dg(t)(x,x0)≤ρ}.Thenat thepoint (x0,t0) wehave

02F∇f,∇Ψ+F−∂t) Ψ2|∇Ψ|2

Ψ F

+

−F

t +2cβt n

|∇f|2−q−ft−afα2

−βtΔq

2(β1)t∇f,∇q −2(β1)taαfα−1|∇f|2

−βtaα(α−1)fα−2|∇f|2−βaαtfα−1

−|∇f|2+ft+q+afα

2βtK1|∇f|2−nβt 2dK2 Ψ.

ByLemma 2.1andtheLaplaciancomparison theorem,wehave

|∇Ψ|2

Ψ ≤C1/22 ρ2 , ΔΨ≥ −C1/2Ψ1/2

ρ2 −C1/2Ψ1/2

ρ (n1)

K1coth(

k1ρ)

≥ −d1

ρ2 −d1Ψ1/2 ρ

K1,

−∂tΨ≥ −CΨ1/2

τ −C1/21/2

where C1/2,C and d1 are positive constants depending only on n. Plugging those estimates into above inequalityyieldsthat

0≥d2

1

ρ2 Ψ1/2 ρ

K1Ψ1/2

τ −KΨ1/2

F−2F|∇f||∇Ψ| +

2cβt n

|∇f|2−q−ft−afα2

−F

t βtΔq−nβt 2d K2

2(β1)t∇f,∇q −2(β1)taαfα−1|∇f|22βtk1|∇f|2 (3.4)

−βtaα(α−1)fα2|∇f|2−βaαtfα1

−|∇f|2+ft+q+afα Ψ at (x0,t0),whered2 isequalto max{d1,C,C1/2,2C1/22 }.Introduceafunction

A:=d2 1

ρ21/2 ρ

K11/2

τ +1/2

.

If onemultipliesbytΨ andmakesafewelementarymanipulations,onewillobtain 0≥ −2F|∇f||∇Ψ|Ψt−AFΨt+

2cβt n

|∇f|2−q−ft−afα2

−βtΔq−2(β1)t∇f,∇q −2(β1)taαfα1|∇f|2

−βtaα(α−1)fα2|∇f|2−βaαtfα1

−|∇f|2+ft+q+afα

(3.5)

2βtK1|∇f|2−nβt

2dK2 Ψ2t−FΨ2

(11)

at(x0,t0).Asin[3,14],weset

μ:=|∇f|2(x0, t0) F(x0, t0) 0.

Because|∇f|=μ1/2F1/2 and

|∇f|2−ft−q−afα=F

μ−μt−1 βt

,

∇f,∇Ψ ≤ |∇f||∇Ψ| ≤ C1

ρ Ψ1/2|∇f| wecansimplify(3.5)into thefollowing inequality

AF tΨ≥ −2C1t

ρ Ψ3/2μ1/2F3/2Ψ2F+2cΨ2

[1 + (β1)μt]2F2−nβ

2dK2(Ψt)2

2(tΨ)2[βK1+a(β−1)αfα1]μF+atΨ2αfα1[1 + (β1)tμ]F (3.6)

−β(tΨ)2θ−2(β1)(tΨ)2γ(μF)1/2−β(tΨ)2aα(α−1)fα2μF at(x0,t0).Ifweset G:= ΨF,thenat thepoint(x0,t0) theinequality(3.6)becomes

AtG≥ −2C1t

ρ μ1/2G3/2ΨG+ 2c

[1 + (β1)μt]2G2−nβ

2dK2(Ψt)2

2Ψt2[βK1+a(β−1)αfα1]μG+aΨtαfα1[1 + (β1)μt]G (3.7)

−β(Ψt)2θ−2(β1)t2Ψ3/2γμ1/2G1/2−βt2Ψaα(α1)fα2μG at(x0,t0).Accordingto theCauchyinequality,where0< <1,

2C1t

R μ1/2G3/2 2c

[1 + (β1)μt]2G2+ nβC12t2μG 2cρ2[1 + (β1)μt]2,1/2G1/21 +μG,

wecansimplify(3.7)as

AtG≥2c(1−)

[1 + (β1)μt]2G2ΨG 2C12t2μ 2cρ2[1 + (β1)μt]2G

2Ψt2[βK1+a(β−1)αfα−1]μG+aΨtαfα−1[1 + (β1)μt]G

−βΨ2t2θ−1)t2Ψ3/2γ−1)t2Ψ3/2γμG

−βt2Ψaα(α1)fα−2μG−nβ

2dK2(Ψt)2, at(x0,t0),or equivalently,

2c(1−)[1 + (β−1)μt]2G2

2C12t2μ

2cρ2[1 + (β1)μt]2 +βt2Ψaα(α1)fα−2μ

−aΨtαfα−1[1 + (β1)μt] + (β1)t2Ψ3/2γμ

(12)

+ 2Ψt2[βK1+a(β−1)αfα−1]μ+At+ Ψ G +

βΨ2θ+ (β1)Ψ3/2γ+

2dK2Ψ2 t2 at (x0,t0).Notethat0Ψ1 and1+ (β1)μt01.Therefore

2c(1−)G2

At+ 1 + 2C12t2μ

2cρ2[1 + (β1)μt]+2Ψt2[βK1+a(β−1)αfα−1]μ [1 + (β1)μt]2

aΨtαfα1

1 + (β1)μt + (β1)γt2μ

1 + (β1)μt +βt2Ψaα|α−1|fα2μ 1 + (β1)μt G +

βθ+ (β1)γ+ 2dK2 t2

At+ 1 + 2C12t

2cρ21)+2Ψt2[βK1+a(β−1)α|fα−1|

[1 + (β1)μt]2 (3.8)

+γt− aΨtαfα1

1 + (β1)μt+βtΨaα|α−1||fα2|

β−1 G

+

βθ+ (β1)γ+ 2dK2 t2.

Beforecompletingtheproof,werecallafact:ifx2≤ax+bforsomea,b,x≥0,then x≤a

2+

b+ a

2 2

≤a 2+

b+a

2 =a+

b. (3.9)

If a≥0 in(3.8),then from(3.8)wededucethat G2

(A+γ)nβt

2c(1−) +

2c(1−)+ n2β3C12t 4c2(1−)ρ21) + 2aα|α−1||fα2|t

2c(β1)(1−) +nβ[βK1+a(β−1)α|fα1|]t

c(1−)(β−1) G (3.10)

+ [βθ+ (β1)γ+2dK2]nβt2

2c(1−) .

Applying (3.9)to theinequality(3.10), wegetanupperbound forG:

G≤

(A+γ)nβ

2c(1−) + n2β3C12

4c2(1−)(β−1)ρ2 +[βK1+a(β−1)α|fα−1|] c(1−)(β−1) + 2aα|α−1||fα2|

2c(β1)(1−) τ+

[βθ+ (β1)γ+2dK2]nβ

2c(1−) τ+

2c(1−),

since t1 ≤τ. Bythe constructionof Ψ, we havesupBρ/2,TF supBρ,T(ΨF)≤G(x0,t0) forall t∈ [0,τ].

Because τ≤T isarbitrary,itfollowsthat

|∇f|2−βft−βq−βafα

2c(1−)t+(A+γ)nβ

2c(1−) + n2β3C12 4c2(1−)(β−1)ρ2 + nβ[βK1+a(β−1)α|fα1|]

c(1−)(β−1)

(13)

+ 2aα|α−1||fα−2|

2c(β1)(1−) +

[βθ+ (β1)γ+2dK2]nβ 2c(1−)

where|f|:= maxM|f|.Similarly,whena≤0,we have G2

(A+γ)nβt

2c(1−) +

2c(1−)+ n2β3C12t

4c2(1−)ρ21)+ 2K1t c(1−)(β−1)

nβatα|fα−1|

2c(1−) G+[βθ+ (β1)γ+2dK2]nβt2

2c(1−) . (3.11)

From(3.9),(3.11),andaboveargument,anupperboundfordesiredquantityinthiscaseis

|∇f|2−βft−βq−βafα

2c(1−)t +(A+γ)nβ

2c(1−) + n2β3C12 4c2(1−)(β−1)ρ2 + [βK1a21)α|fα−1|]

c(1−)(β−1) +

[βθ+ (β1)γ+2dK2]nβ

2c(1−) .

Hence,wecompletetheproof. 2 Acknowledgements

TheauthorsthankforProfessorKefeng Liu’sconstantguidanceandhelp.

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