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R E S E A R C H

Open Access

A new hybrid general iterative algorithm for

common solutions of generalized mixed

equilibrium problems and variational inclusions

Kriengsak Wattanawitoon

1

, Thanyarat Jitpeera

2

and Poom Kumam

2*

* Correspondence: poom. [email protected]

2Department of Mathematics, Faculty of Science, King Mongkuts University of Technology (KMUTT), Bangmod, Thrungkru, Bangkok 10140, Thailand

Full list of author information is available at the end of the article

Abstract

In this article, we introduce a new general iterative method for finding a common element of the set of solutions generalized for mixed equilibrium problems, the set of solution for fixed point for nonexpansive mappings and the set of solutions for the variational inclusions forb1, b2-inverse-strongly monotone mappings in a real

Hilbert space. We prove that the sequence converges strongly to a common element of the above sets under some suitable conditions. Our results improve and extend the corresponding results of Marino and Xu, Su et al., Tan and Chang and some authors.

Mathematics subject Classification: 46C05; 47H09; 47H10.

Keywords:nonexpansive mapping, inverse-strongly monotone mapping, generalized mixed equilibrium problem, variational inclusion

1. Introduction

LetCbe a closed convex subset of a real Hilbert space Hwith the inner product〈·, ·〉and the norm || · ||. LetF be a bifunction ofC ×Cinto R, where R is the set of real numbers,Ψ:C® Hbe a mapping and ϕ:CR be a real-valued function. Thegeneralized mixed equilibrium problemfor findingxÎ Csuch that

F(x,y) +x,yx+ϕ(y)−ϕ(x)≥0, ∀yC. (1:1)

The set of solutions of (1.1) is denoted by GMEP(F,,Ψ), that is

GMEP(F,ϕ,) ={xC:F(x,y) +x,yx+ϕ(y)−ϕ(x)≥0, ∀yC}.

If F ≡ 0, the problem (1.1) is reduced into the mixed variational inequality of Browder type[1] for findingxÎCsuch that

x,yx+ϕ(y)−ϕ(x)≥0, ∀yC. (1:2)

The set of solutions of (1.2) is denoted by MVI(C,,Ψ).

IfΨ≡0, the problem (1.1) is reduced into themixed equilibrium problemfor finding xÎCsuch that

F(x,y) +ϕ(y)−ϕ(x)≥0, ∀yC. (1:3)

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The set of solutions of (1.3) is denoted by MEP(F,).

If ≡ 0, the problem (1.3) is reduced into the equilibrium problem[2] for finding xÎ Csuch that

F(x,y)≥0, ∀yC. (1:4)

The set of solutions of (1.4) is denoted by EP(F). See, e.g. [3-6] and the references therein.

If F≡ 0 and≡ 0, the problem (1.1) is reduced into theHartmann-Stampacchia variational inequality[7] for findingxÎCsuch that

x,yx≥0, ∀yC. (1:5)

The set of solutions of (1.5) is denoted byVI(C,Ψ).

If F≡ 0 andΨ≡0, the problem (1.1) is reduced into theminimize problem for find-ingxÎCsuch that

ϕ(y)−ϕ(x)≥0, ∀yC. (1:6)

The set of solutions of (1.6) is denoted byArgmin().

Iterative methods for nonexpansive mappings have recently been applied to solve convex minimization problems. Convex minimization problems have a great impact and influence in the development of almost all branches of pure and applied sciences. A typical problem is to minimize a quadratic function over the set of the fixed points of a nonexpansive mapping on a real Hilbert space H:

θ(x) = 1

2Ax,x

x,y, ∀xF(S), (1:7)

whereAis a linear bounded operator, F(S) is the fixed point set of a nonexpansive mapping Sandyis a given point inH[8].

Recall, a mappingS: C®Cis said to benonexpansiveif

SxSyxy, ∀x,yC.

IfCis bounded closed convex andSis a nonexpansive mapping ofCinto itself, then F(S) is nonempty [9]. A mappingS:C® Cis said to be ak-strictly pseudo-contraction [10] if there exists 0≤k <1 such that

SxSy2≤xy2+k(IS)x−(IS)y2, ∀x,yC,

whereIdenotes the identity operator onC. A mappingAofCintoHis called mono-toneif

AxAy,xy≥0, ∀x,yC.

A mapping Aof CintoH is called ana-inverse-strongly monotone if there exists a positive real numberasuch that

AxAy,xyαAxAy2, ∀x,yC.

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AxAy,xyαxy2, ∀x,yC.

A linear bounded operator Ais called strongly positive if there exists a constant

¯

γ >0 with the property

Ax,x ≥ ¯γ x 2, ∀xH.

A self mappingf:C®Cis calledcontractiononCif there exists a constantaÎ(0, 1) such that

f(x)−f(y)≤αxy, ∀x,yC.

Let B: H ® H be a single-valued nonlinear mapping andM : H® 2H be a set-valued mapping. Thevariational inclusion problemis to findxÎHsuch that

θB(x) +M(x), (1:8)

whereθis the zero vector in H. The set of solutions of problem (1.8) is denoted by I (B,M). The variational inclusion has been extensively studied in the literature. See, e.g. [11-15] and the reference therein.

A set-valued mappingM : H® 2H is called monotoneif for allx, yÎ H, fÎ M(x) and g Î M(y) imply〈x - y, f- g〉≥ 0. A monotone mappingM is maximalif its graphG(M) := {(f,x)Î H×H:fÎM(x)} ofMis not properly contained in the graph of any other monotone mapping. It is known that a monotone mapping Mis maximal if and only if for (x,f)Î H×H,〈x- y, f-g〉>0 for all (y,g)ÎG(M) implyfÎ M (x).

LetBbe an inverse-strongly monotone mapping ofCinto Hand letNCvbe normal cone toCatvÎC, i.e.,NCv= {wÎH:〈v-u,w〉≥0,∀uÎC}, and define

Mv=

Bv+NCv, ifvC,

∅, ifv∈/C.

Then Mis a maximal monotone andθÎMν if and only ifvÎ VI(C, B) [16]. Let M: H® 2Hbe a set-valued maximal monotone mapping, then the single-valued mapping JM,l:H®Hdefined by

JM,λ(x) = (I+λM)−1(x), xH (1:9)

is called the resolvent operator associated withM, where lis any positive number and Iis the identity mapping. In the worth mentioning that the resolvent operator is nonexpansive, 1-inverse-strongly monotone and that a solution of problem (1.8) is a fixed point of the operatorJM,l(I-lB) for alll> 0 (see also [17]).

In 2000, Moudafi [18] introduced the viscosity approximation method for nonexpan-sive mapping and proved that if His a real Hilbert space, the sequence {xn} defined by the iterative method below, with the initial guess x0Î Cis chosen arbitrarily,

xn+1=αnf(xn) + (1−αn)Sxn, n≥0, (1:10)

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In 2005, Iiduka and Takahashi [19] introduced following iterative processx0 ÎC,

xn+1=αnu+ (1−αn)SPC(xnλnAxn), ∀n≥0, (1:11)

where uÎ C, {an}⊂(0, 1) and {ln}⊂[a, b] for some a,b with 0 <a<b< 2b. They proved that under certain appropriate conditions imposed on {an} and {ln}, the sequence {xn} converges strongly to a common element of the set of fixed points of nonexpansive mapping and the set of solutions of the variational inequality for an inverse-strongly monotone mapping (say x¯C) which solve some variational inequality.

In 2006, Marino and Xu [8] introduced a general iterative method for nonexpansive mapping. They defined the sequence {xn} generated by the algorithmx0ÎC,

xn+1=αnγf(xn) + (IαnA)Sxn, n≥0 (1:12)

where {an} ⊂ (0, 1) andA is a strongly positive linear bounded operator. They proved that if C=Hthen the sequence {xn} converges strongly to a fixed point ofS (say x¯H) which is the unique solution of the following variational inequality.

In 2008, Su et al. [20] introduced the following iterative scheme by the viscosity approximation method in a real Hilbert space:x1,unÎH

⎧ ⎨ ⎩

F(un,y) +

1 rn

yun,unxn

≥0, ∀yC, xn+1=αnf(xn) + (1−αn)SPC(unλnAun),

(1:13)

for all nÎ N, where {an}⊂[0, 1) and {rn}⊂(0,∞) satisfy some appropriate condi-tions. Furthermore, they proved {xn} and {un} converge strongly to the same point z, wherez=PF(S)∩VI(C,A)∩EP(F)f(z).

In 2011, Tan and Chang [14] introduced following iterative process for {Tn:C®C} be a sequence of nonexpansive mappings. Let {xn} be the sequence defined by

xn+1=αnxn+ (1−αn)(SPC((1−tn)JM,λ(IλA)Tn(IμB))xn), ∀n≥0, (1:14)

where {an} ⊂ (0, 1), l Î (0, 2a] and μ Î (0, 2b]. The sequence {xn} converges strongly to a common element of the set of fixed points of nonexpansive mapping, the set of solutions of the variational inequality and the generalized equilibrium problem.

In this article, we modify by Marino and Xu [8], Su et al. [20] and Tan and Chang [14], the purpose of this article, we show that under some control conditions the sequence {xn} converges strongly to a common element of the set of fixed points of nonexpansive mappings, the solution of the generalized mixed equilibrium problems and the solution of the variational inclusions in a real Hilbert space.

2. Preliminaries

Let H be a real Hilbert space andC be a nonempty closed convex subset of H. We denote weak convergence and strong convergence by notations ⇀and®, respectively. Recall that the metric (nearest point) projection PCfromHontoCassigns to eachxÎ H, the unique point inPC xÎ Csatisfying the property

xPCx = inf

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The following characterizes the projection PC. We recall some lemmas which will be needed in the rest of this article.

Lemma 2.1. The function uÎ C is a solution of the variational inequality (1.5)if and only if uÎC satisfies the relation u=PC(u-lΨu)for alll> 0.

Lemma 2.2.For a given zÎH,uÎC,u=PCz⇔〈u-z,v-u〉≥0,∀vÎC. It is well known that PC is a firmly nonexpansive mapping of H onto C and satisfies

PCxPCy2≤

PCxPCy,xy

, ∀x,yH. (2:1)

Moreover, PCx is characterized by the following properties: PCxÎC and for all xÎH, y ÎC,

xPCx,yPCx

≤0. (2:2)

Lemma 2.3. [21]Let M:H®2Hbe a maximal monotone mapping and let B:H®H be a monotone and Lipshitz continuous mapping. Then the mapping L=M+B:H®2H is a maximal monotone mapping.

Lemma 2.4. [22]Each Hilbert space H satisfies Opial’s condition, that is, for any sequence {xn}⊂H with xn⇀x, the inequalitylim infn®∞||xn-x|| < lim infn®∞||xn-y||, hold for each yÎH with y≠x.

Lemma 2.5. [23]Assume{an}is a sequence of nonnegative real numbers such that an+1≤(1−γn)an+δn, ∀n≥0,

where {gn}⊂(0, 1)and{δn}is a sequence in Rsuch that (i) ∞n=1γn=∞.

(ii) lim supn→∞δn

γn

0or ∞n=1|δn|<∞.

Thenlimn®∞an= 0.

Lemma 2.6. [24]Let C be a closed convex subset of a real Hilbert space H and let S: C®C be a nonexpansive mapping. Then I-S is demiclosed at zero, that is,

xn x,xnSxn→0

implies x=Sx.

For solving the mixed equilibrium problem, let us assume that the bifunction F:C×CR and ϕ:CR satisfies the following conditions:

(A1)F(x, x) = 0 for allxÎC;

(A2)Fis monotone, i.e.,F(x,y) +F(y,x)≤0 for anyx, yÎC;

(A3) for each fixedyÎ C,x↦ F(x,y) is weakly upper semicontinuous; (A4) for each fixedxÎC,y↦ F(x,y) is convex and lower semicontinuous;

(B1) for eachx Î Cand r > 0, there exist a bounded subsetDx ⊆C andyx Î C such that for anyzÎC\Dx,

F(z,yx) +ϕ(yx)−ϕ(z) +

1 r

yxz,zx

<0,

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Lemma 2.7. [25]Let C be a nonempty closed convex subset of a real Hilbert space H. Let F:C×CRbe a bifunction mapping satisfies (A1)-(A4)and let ϕ:CRis convex and lower semicontinuous such thatCdomϕ=∅. Assume that either(B1) or (B2) holds. For r> 0and xÎH, then there exists zÎ C such that

F(z,y) +ϕ(y)−ϕ(z) + 1 r

yz,zx≥0, ∀yC.

Define a mapping T(F,ϕ)

r :HCas follows:

Tr(F,ϕ)(x) =

zC:F(z,y) +ϕ(y)−ϕ(z) +1 r

yz,zx≥0, ∀yC

for all xÎH. Then, the following hold:

(i) Tr(F,ϕ)is single-valued;

(ii) T(F,ϕ)

r is firmly nonexpansive, i.e., for any x,y ÎH,

Tr(F,ϕ)xTr(F,ϕ)y

2

Tr(F,ϕ)xTr(F,ϕ)y,xy

;

(iii) F(Tr(F,ϕ)) = MEP(F,ϕ);

(iv) MEP(F,)is closed and convex.

Lemma 2.8. [8]Assume A is a strongly positive linear bounded operator on a Hilbert space H with coefficient γ >¯ 0and0 <r≤||A||-1,then IρA ≤1−ργ¯.

Lemma 2.9. [26]Let H be a real Hilbert space and A:H®H a mapping.

(i)If A is aδ-strongly monotone andμ-strictly pseudo-contraction withδ+μ> 1, then I-A is a contraction with constant (1−δ)/μ.

(ii) If A is aδ-strongly monotone andμ-strictly pseudo-contraction with δ+μ > 1, then for any fixed number τ Î (0, 1), I - τA is a contraction with constant

1−τ(1−(1−δ)/μ).

3. Strong convergence theorems

In this section, we show a strong convergence theorem which solves the problem of finding a common element of F(S), GMEP(F1,1,B1), GMEP(F2, 2,B2),I(A1,M1) and

I(A2,M2).

Theorem 3.1.Let H be a real Hilbert space, C be a closed convex subset of H. Let F1,

F2 be bifunctions of C×C into Rsatisfying(A1)-(A4)and A1,A2, B1, B2: C® H be

b1, b2,h, r-inverse-strongly monotone mappings, ϕ1,ϕ2:CRbe convex and lower

semicontinuous functions, f :C®C be a contraction with coefficienta(0 <a< 1),M1,

M2 :H®2Hbe maximal monotone mappings and A is aδ-strongly monotone andμ

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γ < 1α

1−

1−δ

μ

. Assume that either(B1)or(B2)holds. Let S be a nonexpansive mapping of C into itself such that

:=F(S)∩GMEP(F1,ϕ1,B1)∩GMEP(F2,ϕ2,B2)∩I(A1,M1)∩I(A2,M2)=∅.

Suppose{xn}is a sequences generated by the following algorithm x0Î C arbitrarily: ⎧

⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎩

un=T

(F1,ϕ1)

rn (xnrnB1xn)

vn=Ts(nF2,ϕ2)(xnsnB2xn)

xn+1=ξnPC

αnγf(xn) + (IαnA)SPC[JM1,λ1(1−λ1A1)un]

+(1−ξn)PC[JM2,λ2(Iλ2A2)vn], ∀n≥0,

(3:1)

where{an}, {ξn}⊂(0, 1), l1Î (0, 2b1)such that0 <a1 ≤l1 <b1 < 2b1, l2Î (0, 2b2)

such that 0 <a1 ≤l2 ≤ b2< 2b2, rnÎ (0, 2h)with0 <c ≤d ≤1 - hand snÎ (0, 2r) with0 <e≤f≤1 -rsatisfy the following conditions:

(C1): limn®∞an= 0, ∞n=0αn=∞, ∞n=1|αn+1−αn|<∞,

(C2): 0 < lim infn®∞ξn< lim supn®∞ξn< 1, ∞n=1|ξn+1−ξn|<∞,

(C3): lim infn®∞rn> 0andlimn®∞|rn+1-rn| = 0, (C4): lim infn®∞sn> 0andlimn®∞|sn+1- sn| = 0.

Then {xn}converges strongly to q Î Θ, where q=PΘ(gf+I- A)(q)which solves the following variational inequality:

(γfA)q,pq≤0, ∀p

which is the optimality condition for the minimization problem

min

q

1 2

Aq,qh(q), (3:2)

where h is a potential function forgf (i.e., h’(q) =gf(q)for q ÎH).

Proof. SinceA1,A2areb1,b2-inverse-strongly monotone mappings, we have (Iλ1A1)x−(Iλ1A1)y

2

=(xy)−λ1(A1xA1y) 2

=xy2−2λ1xy,A1xA1y

+λ21A1xA1y 2

xy2+λ1(λ1−2β1)A1xA1y 2

xy2.

In similar way, we can obtain

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AndB1,B2areh,r-inverse-strongly monotone mappings, we have (IrnB1)x−(IrnB1)y

2

=(xy)−rn(B1xB1y) 2

=xy2−2rn

xy,B1xB1y

+rn2B1xB1y 2

xy2+rn(rn−2η)B1xB1y 2

xy2.

In similar way, we can obtain

(IsnB2)x−(IsnB2)y

2

xy2.

It is clear that if 0 <l1 < 2b1, 0 <l2 < 2b2, 0 <rn< 2h, 0 <sn≤ 2rthenI- l1A1,I

-l2 A2,I-rnB1,I- snB2are all nonexpansive. We will divide the proof into six steps.

Step 1. We will show {xn} is bounded. Put yn=JM1,λ1(unλ1A1un) for alln≥0 and wn=JM2,λ2(vnλ2A2vn) for all n≥0. It follows that

ynq=JM1,λ1(unλ1A1un)−JM1,λ1(qλ1A1q)

unq.

(3:3)

In similar way, we can obtain

wnq=JM2,λ2(vnλ2A2vn)−JM2,λ2(qλ2A2q)

vnq.

(3:4)

Putyn=PCyn, n≥0. It follows that

ynq=PCynPCq

ynq.

(3:5)

By Lemma 2.7, we have un=Tr(nF1,ϕ1)(xnrnB1xn),vn=T

(F2,ϕ2)

sn (xnsnB2xn) for all n

≥0. Then, we have

unq

2

=T(F1,ϕ1)

rn (xnrnB1xn)−T

(F1,ϕ1)

rn (qrnB1q)

2 ≤(xnrnB1xn)−(qrnB1q)2

xnq

2

+rn(rn−2η)B1xnB1q 2

xnq2.

(3:6)

In similar way, we can obtain

vnq2=Ts(nF2,ϕ2)(xnsnB2xn)−T

(F2,ϕ2)

sn (qsnB2q)

2 ≤(xnsnB2xn)−(qsnB2q)

2

xnq2+sn(sn−2ρ)B2xnB2q2 ≤xnq

2 .

(3:7)

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(ii), we deduce that

xn+1−q=ξn(znq) + (1−ξn)(PCwnq)

ξnPC[αnγf(xn) + (IαnA)SPCyn]−PCq+ (1−ξn)PCwnPCq

ξnαnγf(xn) + (IαnA)SPCynq+ (1−ξn)wnq

=ξnαn(γf(xn)−Aq) + (IαnA)(SPCynq)+ (1−ξn)wnq

ξnαnγf(xn)−Aq

+ξn

1−αn

1−

1−δ

μ

PCynq+ (1−ξn)wnq

ξnαnγf(xn)−γf(q)+ξnαnγf(q)−Aq

+ξn

1−αn

1−

1−δ

μ

PCynq+ (1−ξn)xnq

ξnαnγ αxnq+ξnαnγf(q)−Aq

+ξn

1−αn

1−

1−δ

μ

ynq+ (1−ξn)xnq

= 1− 1− 1−δ

μ

γ α

ξnαn

xnq+ξnαnγf(q)−Aq

≤ 1− 1−

1−δ

μ

γ α

ξnαn

xnq

+

1−

1−δ

μ

γ α

ξnαn

γf(q)−Aq

1−

1−δ

μ

γ α

≤max ⎧ ⎪ ⎪ ⎨ ⎪ ⎪ ⎩

xnq,

γf(q)−Aq

1−

1−δ

μ

γ α

⎫ ⎪ ⎪ ⎬ ⎪ ⎪ ⎭ .

(3:8)

It follows from induction that

xnq≤max

⎧ ⎪ ⎪ ⎨ ⎪ ⎪ ⎩

x0−q,

γf(q)−Aq

1−

1−δ

μ

γ α

⎫ ⎪ ⎪ ⎬ ⎪ ⎪ ⎭

, n≥0.

Therefore {xn} is bounded, so are {yn},{zn},{PCwn},{SPCyn},{f(xn)} and {ASPCyn}. Step 2. We claim that limn®∞||xn+2-xn+1|| = 0. From (3.1), we have

xn+2−xn+1 =ξn+1zn+1+ (1−ξn+1)PCwn+1−ξnzn−(1−ξn)PCwn

=ξn+1(zn+1−zn) + (ξn+1−ξn)zn

+(1−ξn+1)(PCwn+1−PCwn) + (ξnξn+1)PCwn

ξn+1 zn+1−zn + (1−ξn+1) wn+1−wn

+|ξn+1−ξn|( zn + PCwn ).

(10)

Since I- l2A2be nonexpansive, we have

wn+1−wn =JM2,λ2(vn+1−λ2A2vn+1)−JM2,λ2(vnλ2A2vn)

≤(vn+1−λ2A2vn+1)−(vnλ2A2vn)

vn+1−vn .

(3:10)

On the other hand, from vn−1=Ts(nF−21,ϕ2)(xn−1−sn−1B2xn−1) and vn=Ts(nF2,ϕ2)(xnsnB2xn), it follows that

F2(vn−1,y) +

B2xn−1,yvn−1

+ϕ2(y)−ϕ2(vn−1)

+ 1

sn−1

yvn−1,vn−1−xn−1

≥0, ∀yC (3:11)

and

F2(vn,y) +

B2xn,yvn

+ϕ2(y)−ϕ2(vn) +

1 sn

yvn,vnxn

≥0, ∀yC.(3:12)

Substituting y=vnin (3.11) andy=vn-1in (3.12), we get

F2(vn−1,vn)+B2xn−1,vnvn−1+ϕ2(vn)−ϕ2(vn−1)+

1

sn−1vnvn−1,vn−1−xn−1 ≥0

and

F2(vn,vn−1) +B2xn,vn−1−vn+ϕ2(vn−1)−ϕ2(vn) +

1 sn

vn−1−vn,vnxn ≥0.

From (A2), we obtain

vnvn−1,B2xn−1−B2xn+

vn−1−xn−1 sn−1 −

vnxn

sn

≥0,

and then

vnvn−1,sn−1(B2xn−1−B2xn) +vn−1−xn−1− sn−1

sn

(vnxn)

≥0,

so

vnvn−1,sn−1B2xn−1−sn−1B2xn+vn−1−vn+vnxn−1− sn−1

sn

(vnxn)

≥0.

It follows that

vnvn−1, (Isn−1B2)xn−(Isn−1B2)xn−1 +vn−1−vn+vnxn

sn−1 sn

(vnxn)

≥0,

vnvn−1,vn−1−vn+

vnvn−1,xnxn−1+

1−sn−1 sn

(vnxn)

≥0.

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vnvn−1 2≤

vnvn−1,xnxn−1+

1−sn−1 sn

(vnxn)

vnvn−1

xnxn−1 +

1−sn−1 sn

vnxn

and hence

vnvn−1 ≤ xnxn−1 + 1 sn

|snsn−1| vnxn

xnxn−1 + M1

e |snsn−1|,

(3:13)

whereM1 = sup{||vn-xn|| :nÎN}. Substituting (3.13) into (3.9) and (3.10) that

xn+2−xn+1 ≤ξn+1 zn+1−zn + (1−ξn+1)

xn+1−xn +

M1

e |snsn−1|

+|ξn+1−ξn|( zn + PCwn ).

(3:14)

By Lemma 2.9 (ii), it follow that zn+1−zn

=PC[αn+1γf(xn+1) + (Iαn+1A)SPCyn+1]

PC[αnγf(xn) + (IαnA)SPCyn]

αn+1γf(xn+1) + (Iαn+1A)SPCyn+1−αnγf(xn)−(IαnA)SPCyn

=αn+1γ(f(xn+1)−f(xn)) + (αn+1−αn)γf(xn)

+(Iαn+1A)(SPCyn+1−SPCyn) + (αnαn+1)ASPCyn

αn+1γ α xn+1−xn +|αn+1−αn|γf(xn)

+

1−αn+1

1−

1−δ

μ

yn+1−yn+|αn+1−αn|ASPCyn

=αn+1γ α xn+1−xn +|αn+1−αn|(γf(xn)+ASPCyn)

+

1−αn+1

1−

1−δ

μ

yn+1−yn.

(3:15)

Since I- l1A1be nonexpansive, we have

yn+1−yn=JM1,λ1(un+1−λ1A1un+1)−JM1,λ1(unλ1A1un)

≤(un+1−λ1A1un+1)−(unλ1A1un)

≤(Iλ1A1)un+1−(Iλ1A1)un

un+1−un .

(3:16)

On the other hand, from un−1=Tr(nF−11,ϕ1)(xn−1−rn−1B1xn−1) and un=Tr(nF1,ϕ1)(xnrnB1xn), it follows that

F1(un−1,y) +

B1xn−1,yun−1

+ϕ1(y)−ϕ1(un−1)

+ 1

rn−1

yun−1,un−1−xn−1

(12)

and

F1(un,y) +

B1xn,yun

+ϕ1(y)−ϕ1(un) +

1 rn

yun,unxn

≥0, ∀yC. (3:18)

Substituting y=unin (3.17) andy=un-1in (3.18), we get

F1(un−1,un)+B1xn−1,unun−1+ϕ1(un)−ϕ1(un−1)+ 1

rn−1unun−1,un−1−xn−1 ≥0

and

F1(un,un−1) +B1xn,un−1−un+ϕ1(un−1)−ϕ1(un) +

1 rn

un−1−un,unxn ≥0.

From (A2), we obtain

unun−1,B1xn−1−B1xn+

un−1−xn−1 rn−1 −

unxn

rn

≥0,

and then

unun−1,rn−1(B1xn−1−B1xn) +un−1−xn−1− rn−1

rn

(unxn)

≥0,

so

unun−1,rn−1B1xn−1−rn−1B1xn+un−1−un+unxn−1− rn−1

rn

(unxn)

≥0.

It follows that

unun−1, (Irn−1B1)xn−(Irn−1B1)xn−1 +un−1−un+unxn

rn−1 rn

(unxn)

≥0,

unun−1,un−1−un+

unun−1,xnxn−1+

1−rn−1 rn

(unxn)

≥0.

Without loss of generality, let us assume that there exists a real number csuch that rn-1>c> 0, for allnÎN. Then, we have

unun−1 2≤

unun−1,xnxn−1+

1−rn−1 rn

(unxn)

unun−1

xnxn−1 +

1−rn−1 rn

unxn

and hence

unun−1 ≤ xnxn−1 + 1 rn|

rnrn−1| unxn

xnxn−1 + M2

c |rnrn−1|,

(13)

whereM2 = sup{||un-xn|| :nÎN}. Substituting (3.19) into (3.16), we have

ynyn−1≤ xnxn−1 + M2

c |rnrn−1|. (3:20)

Substituting (3.20) into (3.15), we obtain that

zn+1−znαn+1γ α xn+1−xn +|αn+1−αn|(γf(xn)+ASPCyn)

+

1−αn+1

1−

1−δ

μ xnxn−1 + M2

c |rnrn−1|

(3:21)

And substituting (3.10), (3.13), (3.21) into (3.9), we get

xn+2−xn+1 ≤ξn+1{αn+1γ α xn+1−xn +|αn+1−αn|(γf(xn)+ASPCyn)

+

1−αn+1

1−

1−δ

μ

xnxn−1 + M2

c |rnrn−1|

+ (1−ξn+1)

xnxn−1 + M1

e |snsn−1|

+|ξn+1−ξn|( zn + PCwn )

1−

1−

1−δ

μ

γ α

ξn+1αn+1

xn+1−xn

+ (|αn+1−αn|+|ξn+1−ξn|)M3

+M2

c |rnrn−1|+ M1

e |snsn−1|,

(3:22)

whereM3 > 0 is a constant satisfying

sup

n

γf(xn)+ASPCyn, zn + PCwn

M3.

This together with (C1)-(C4) and Lemma 2.5, imply that

lim

n→∞ xn+2−xn+1 = 0. (3:23)

From (3.20) and (C3), we also have ||yn+1-yn||®0 asn®∞. Step 3. We show the followings:

(i) limn®∞||A1un-A1q|| = 0;

(ii) limn®∞||A2vn- A2q|| = 0;

(iii) limn®∞||B1xn-B1q|| = 0;

(iv) limn®∞||B2xn-B2q|| = 0.

ForqÎΘand q=JM1,λ1(qλ1A1q), then we get

ynq

2

=JM1,λ1(unλ1A1un)−JM1,λ1(qλ1A1q)

2

≤(unλ1A1un)−(qλ1A1q)2 ≤unq

2

+λ1(λ1−2β1)A1unA1q 2

(14)

Using (3.5), it follows that

znq

2

=PC[αnγf(xn) + (IαnA)Syn]−PC(q)

2

αn(γf(xn)−Aq) + (IαnA)(Synq)

2

αn(γf(xn)−Aq) + (IαnA)(ynq)

2

αn(γf(xn)−Aq) + (IαnA)(ynq)

2

αnγf(xn)−Aq

2

+

1−αn

1−

1−δ

μ

ynq

2

+ 2αn

1−αn

1−

1−δ

μ

γf(xn)−Aqynq

αnγf(xn)−Aq2+ 2αn

1−αn

1−

1−δ

μ

γf(xn)−Aqynq

+

1−αn

1−

1−δ

μ xnq

2

+λ1(λ1−2β1)A1unA1q 2

αnγf(xn)−Aq

2

+ 2αn

1−αn

1−

1−δ

μ

γf(xn)−Aqynq

+xnq

2

+

1−αn

1−

1−δ

μ

λ1(λ1−2β1)A1unA1q 2

.

(3:24)

By the convexity of the norm ||·||, we have

xn+1−q2=ξnzn+ (1−ξn)PCwnq2

=ξn(znq) + (1−ξn)(PCwnq)

2

ξnznq2+ (1−ξn)wnq2.

(3:25)

Substituting (3.4), (3.7), (3.24) into (3.25), we obtain

xn+1−q 2

ξn αnγf(xn)−Aq2+ 2αn

1−αn

1−

1−δ

μ

×γf(xn)−Aqynq+xnq

2

+

1−αn

1−

1−δ

μ

×λ1(λ1−2β1)A1unA1q 2

+ (1−ξn)xnq

2

=ξnαnγf(xn)−Aq

2

+ 2ξnαn

1−αn

1−

1−δ

μ

×γf(xn)−Aqynq+ξnxnq

2

+ξn

1−αn

1−

1−δ

μ

×λ1(λ1−2β1)A1unA1q 2

+ (1−ξn)xnq

2

.

So, we obtain

ξn

1−αn

1−1−δ

μ

λ1(2β1−λ1)A1unA1q2

(15)

where εn= 2ξnαn

1−αn

1−

1−δ

μ γf(xn)−Aqynq. Since conditions

(C1), (C2) and limn®∞ ||xn+1-xn|| = 0, then we obtain that ||A1un-A1q||®0 asn®

∞. ForqÎΘand q=JM2,λ2(qλ2A2q), then we get

wnq2=JM2,λ2(vnλ2A2vn)−JM2,λ2(qλ2A2q)

2

≤(vnλ2A2vn)−(qλ2A2q) 2

vnq2+λ2(λ2−2β2)A2vnA2q2 ≤xnq

2

+λ2(λ2−2β2)A2vnA2q 2

.

(3:26)

Substituting (3.24), (3.26) into (3.25), we obtain

xn+1−q2

ξn αnγf(xn)−Aq2+ 2αn

1−αn

1−

1−δ

μ

γf(xn)Aqynq

+xnq

2

+

1−αn

1−

1−δ

μ

λ1(λ1−2β1)A1unA1q 2

+ (1−ξn)

xnq2+λ2(λ2−2β2)A2vnA2q2

=ξnαnγf(xn)−Aq2+ 2ξnαn

1−αn

1−

1−δ

μ

γf(xn)−Aqynq

+ξnxnq2+ξn

1−αn

1−

1−δ

μ

λ1(λ1−2β1)A1unA1q2

+ (1−ξ1)xnq

2

+ (1−ξn)λ2(λ2−2β2)A2vnA2q 2

.

So, we obtain

(1−ξn)λ2(2β2−λ2)A2vnA2q 2

ξnαnγf(xn)−Aq

2

+εn+ξn

1−αn

1−

1−δ

μ

λ1(λ1−2β1)

×A1unA1q2+ xnxn+1 (xnq+xn+1−q),

where εn= 2ξnαn

1−αn

1−

1−δ

μ γf(xn)−Aqynq. Since conditions

(C1), (C2), limn®∞ ||xn+1- xn|| = 0 and limn®∞ ||A1un- A1q||® 0 then we obtain

that ||A2vn-A2q||®0 as n® ∞. We consider this inequality in (3.24) that znq

2

αnγf(xn)−Aq

2 +

1−αn

1−

1−δ

μ

ynq

2

+ 2αn

1−αn

1−

1−δ

μ

γf(xn)−Aqynq.

(16)

Substituting (3.3) and (3.6) into (3.27), we have

znq2≤αnγf(xn)−Aq2+

1−αn

1−

1−δ

μ

×xnq2+rn(rn−2η)B1xnB1q2

+ 2αn

1−αn

1−

1−δ

μ

γf(xn)−Aqynq

=αnγf(xn)−Aq

2 +

1−αn

1−

1−δ

μ

xnq

2

+

1−αn

1−

1−δ

μ

rn(rn−2η)B1xnB1q2

+ 2αn

1 +αn

1−

1−δ

μ

γf(xn)−Aqynq

αnγf(xn)−Aq2+xnq2

+

1−αn

1−

1−δ

μ

rn(rn−2η)B1xnB1q2

+ 2αn

1−αn

1−

1−δ

μ

γf(xn)−Aqynq.

(3:28)

Substituting (3.4), (3.7) and (3.28) into (3.25), we obtain

xn+1−q2

ξn αnγf(xn)−Aq2+xnq2+

1−αn

1−

1−δ

μ

×rn(rn−2η)B1xnB1q 2

+ 2αn

1−αn

1−

1−δ

μ

×γf(xn)−Aqynq}+ (1−ξn)xnq

2

=ξnαnγf(xn)−Aq

2

+ξnxnq

2 +ξn

1−αn

1−

1−δ

μ

×rn(rn−2η)B1xnB1q2+ 2ξnαn

1−αn

1−

1−δ

μ

×γf(xn)−Aqynq+ (1−ξn)xnq

2 .

(3:29)

So, we also have

ξn

1−αn

1−

1−δ

μ

rn(2ηrn)B1xnB1q 2

(17)

where εn= 2ξnαn

1−αn

1−

1−δ

μ γf(xn)−Aqynq. Since conditions

(C1), (C2), (C3), limn®∞||xn+1- xn|| = 0, then we obtain that ||B1xn-B1q||® 0 asn

® ∞. Substituting (3.4), (3.7) and (3.28) into (3.25), we obtain

xn+1−q 2

ξn αnγf(xn)−Aq

2

+xnq

2 +

1−αn

1−

1−δ

μ

×rn(rn−2η)B1xnB1q2+ 2αn

1−αn

1−

1−δ

μ

×γf(xn)−Aqynq

+ (1−ξn){xnq2+sn(sn−2ρ)B2xnB2q2} =ξnαnγf(xn)−Aq2+ξnxnq2+ξn

1−αn

1−

1−δ

μ

×rn(rn−2η)B1xnB1q 2

+ 2ξnαn

1−αn

1−

1−δ

μ

×γf(xn)−Aqynq+ (1−ξn)xnq2

+ (1−ξn)sn(sn−2ρ)B2xnB2q 2

=ξnαnγf(xn)−Aq2+xnq2+ξn

1−αn

1−

1−δ

μ

×rn(rn−2η)B1xnB1q2+ 2ξnαn

1−αn

1−

1−δ

μ

×γf(xn)−Aqynq

+ (1−ξn)sn(sn−2ρ)B2xnB2q2.

So, we also have

(1−ξn)sn(2ρsn)B2xnB2q2 ≤ξnαnγf(xn)−Aq

2

+εn+ xnxn+1 (xnq+xn+1−q) +ξn

1−αn

1−

1−δ

μ

rn(rn−2η)B1xnB1q 2

,

where εn= 2ξnαn

1−αn

1−

1−δ

μ γf(xn)−Aqynq. Since conditions

(C1), (C2), (C4), limn®∞ ||xn+1 - xn|| = 0 and limn®∞ ||B1xn - B1q|| = 0, then we

obtain that ||B2xn-B2q||®0 as n® ∞.

(18)

(v) limn→∞unyn= 0;

(vi) limn→∞ynSyn= 0.

Since T(F1,ϕ1)

rn is firmly nonexpansive, we observe that

unq

2

=T(F1,ϕ1)

rn (xnrnB1xn)−T

(F1,ϕ1)

rn (qrnB1q)

2 ≤(xnrnB1xn)−(qrnB1q),unq

= 1

2((xnrnB1xn)−(qrnB1q) 2

+unq

2

−(xnrnB1xn)

−(qrnB1q)−(unq)2)

≤ 1

2(xnq 2

+unq2−(xnun)−rn(B1xnB1q)2)

= 1

2(xnq 2

+unq2− xnun 2

+ 2rn

B1xnB1q,xnun

rn2B1xnB1q 2

).

Hence, we have

unq

2

xnq

2

xnun 2+ 2rnB1xnB1q xnun . (3:30)

Since JM1,λ1 is 1-inverse-strongly monotone, we compute

ynq2=JM1,λ1(unλ1A1un)−JM1,λ1(qλ1A1q)

2

≤(unλ1A1un)−(qλ1A1q),ynq

= 1

2((unλ1A1un)−(qλ1A1q) 2

+ynq

2

−(unλ1A1un)−(qλ1A1q)−(ynq)2

= 1

2(unq 2

+ynq

2

−(unyn)−λ1(A1unA1q) 2

)

≤ 1

2(unq 2

+ynq

2

unyn

2

+ 2λ1

unyn,A1unA1q

λ2

1A1unA1q2), which implies that

ynq

2

unq

2

unyn

2

+ 2λ1unynA1unA1q. (3:31)

Substitute (3.30) into (3.31), we have

ynq

2

≤ {xnq

2

xnun 2+ 2rnB1xnB1q xnun }

unyn2+ 2λ1unynA1unA1q.

(19)

Substitute (3.32) into (3.27), we have znq

2

αnγf(xn)−Aq 2

+

1−αn

1−

1−δ

μ

{xnq 2

xnun 2

+ 2rnB1xnB1q xnununyn2+ 2λ1unynA1unA1q}

+ 2αn

1−αn

1−

1−δ

μ

γf(xn)−Aqynq

αnγf(xn)−Aq 2

+xnq

2

xnun 2

+ 2

1−αn

1−

1−δ

μ

rnB1xnB1q xnununyn 2

+ 2

1−αn

1−

1−δ

μ

λ1unynA1unA1q

+ 2αn

1−αn

1−

1−δ

μ

γf(xn)−Aqynq.

(3:33)

Since T(F2,ϕ2)

sn is firmly nonexpansive, we observe that

vnq

2

=T(F2,ϕ2)

sn (xnsnB2xn)−T

(F2,ϕ2)

sn (qsnB2q)

2 ≤(xnsnB2xn)−(qsnB2q),vnq

= 1

2((xnsnB2xn)−(qsnB2q) 2

+vnq

2

−(xnsnB2xn)−(qsnB2q)−(vnq)2)

≤ 1

2(xnq 2

+vnq2−(xnvn)−sn(B2xnB2q)2)

= 1

2(xnq 2

+vnq2− xnvn 2

+ 2sn

B2xnB2q,xnvn

s2nB2xnB2q 2

).

Hence, we have

vnq2≤xnq2− xnvn 2+ 2snB2xnB2q xnvn . (3:34)

Since JM2,λ2 is 1-inverse-strongly monotone, we compute

wnq2=JM2,λ2(vnλ2A2vn)−JM2,λ2(qλ2A2q)

2

≤(vnλ2A2vn)−(qλ2A2q),wnq

= 1

2((vnλ2A2vn)−(qλ2A2q) 2

+wnq2

−(vnλ2A2vn)−(qλ2A2q)−(wnq)

2 )

= 1

2(vnq 2

+wnq

2

−(vnwn)−λ2(A2vnA2q) 2

)

≤ 1

2(vnq 2

+wnq2− vnwn 2

+ 2λ2

vnwn,A2vnA2q

λ2

2A2vnA2q 2

),

which implies that

(20)

Substitute (3.34) into (3.35), we have

wnq

2

≤ {xnq

2

xnvn 2+ 2snB2xnB2q xnvn }

vnwn 2+ 2λ2 vnwn A2vnA2q.

(3:36)

Substitute (3.33) and (3.36) into (3.25), we obtain xn+1q

2

ξnznq 2

+ (1−ξn)wnq 2

ξnαnγf(xn)−Aq 2

+xnq 2

xnun 2−unyn 2

+ 2

1−αn

1−

1−δ μ

rnB1xnB1q xnun

+ 2

1−αn

1−

1−δ

μ

λ1unynA1unA1q

+2αn

1−αn

1−

1−δ

μ

γf(xn)−Aqynq

+ (1−ξn){xnq 2

xnvn 2

+ 2snB2xnB2q xnvnvnwn 2

+ 2λ2 vnwn A2vnA2q}

ξnαnγf(xn)−Aq 2

+ξnxnq 2

xnun 2−unyn 2

+ 2ξn

1−αn

1−

1−δ

μ

rnB1xnB1q xnun

+ 2ξn

1−αn

1−

1−δ μ

λ1unynA1unA1q

+ 2ξnαn

1−αn

1−

1−δ μ

γf(xn)−Aqynq

+ (1−ξn)xnq 2

xnvn 2+ 2(1−ξn)snB2xnB2q xnvn

vnwn 2+ 2(1−ξn)λ2 vnwn A2vnA2q.

Then, we derive

xnun 2+unyn

2

+ xnvn 2+ vnwn 2

ξnαnγf(xn)−Aq 2

+xnq 2

xn+1q 2

+ 2ξn

1−αn

1−

1−δ μ

rnB1xnB1q xnun

+ 2ξn

1−αn

1−

1−δ

μ

λ1unynA1unA1q

+ 2ξnαn

1−αn

1−

1−δ

μ

γf(xn)−Aqynq

+ 2(1−ξn)snB2xnB2q xnvn + 2(1−ξn)λ2 vnwn A2vnA2q

=ξnαnγf(xn)−Aq 2

+ xn+1xn (xnq+xn+1q)

+ 2ξn

1−αn

1−

1−δ

μ

rnB1xnB1q xnun

+ 2ξn

1−αn

1−

1−δ

μ

λ1unynA1unA1q

+ 2ξnαn

1−αn

1−

1−δ

μ

γf(xn)−Aqynq

(21)

By conditions (C1)-( C4), limn®∞||xn-xn+1|| = 0, limn®∞||B1xn-B1q|| = 0, limn®∞ || B2xn-B2q|| = 0, limn®∞ ||A1un- A1q|| = 0 and limn®∞||A2vn- A2q|| = 0. So, we have

||xn-un||®0, ||un- yn||®0, ||xn-vn||®0, ||vn-wn||®0 asn®∞. From (2.1), we have

ynq2=PCJM1λ1(unλ1A1un)−PCJM1λ1(qλ1A1q)

2

JM1,λ1(unλ1A1un)−JM1,λ1(qλ1A1q)

2

≤(unλ1A1un)−(qλ1A1q),ynq

= 1

2((unλ1A1un)−(qλ1A1q) 2

+ynq2

−(unλ1A1un)−(qλ1A1q)−(ynq)

2 )

= 1

2(unq 2

+ynq2−(unyn)−λ1(A1unA1q) 2

)

≤ 1

2(unq 2

+ynq2−unyn

2

+ 2λ1

unyn,A1unA1q

λ2

1A1unA1q2), which implies that

ynq2≤unq2−unyn

2

+ 2λ1unynA1unA1q. (3:37) Substitute (3.30) into (3.37), we have

ynq2≤ {xnq2− xnun 2+ 2rnB1xnB1q xnun }

unyn

2

+ 2λ1unynA1unA1q.

(3:38)

We consider this inequality in (3.24) that

znq

2

αnγf(xn)−Aq

2 +

1−αn

1−

1−δ

μ

ynq2

+ 2αn

1−αn

1−

1−δ

μ

γf(xn)−Aqynq.

(3:39)

Substitute (3.38) into (3.39), we have znq2≤αnγf(xn)−Aq2+

1−αn

1−

1−δ

μ

{xnq2− xnun 2

+ 2rnB1xnB1q xnununyn 2

+ 2λ1unynA1unA1q}

+ 2αn

1−αn

1−

1−δ

μ

γf(xn)−Aqynq

αnγf(xn)−Aq 2

+xnq 2

xnun 2

+ 2

1−αn

1−

1δ

μ

rnB1xnB1q xnununyn

2

+ 2

1αn

1

1−δ

μ

λ1unynA1unA1q

+ 2αn

1−αn

1−

1δ

μ

γf(xn)−Aqynq.

(22)

Substitute (3.36) and (3.40) into (3.25), we obtain xn+1q

2

ξnznq 2

+ (1−ξn)wnq 2

ξnαnγf(xn)−Aq2+xnq2− xnun 2−unyn 2

+ 2

1−αn

1−

1−δ

μ

rnB1xnB1q xnun

+ 2

1−αn

1−

1δ

μ

λ1unynA1unA1q

+2αn

1αn

1

1−δ

μ

γf(xn)−Aqynq

+ (1−ξn){xnq2− xnvn 2+ 2snB2xnB2q xnvnvnwn 2

+ 2λ2 vnwn A2vnA2q}

ξnαnγf(xn)−Aq 2

+ξnxnq 2

xnun 2−unyn 2

+ 2ξn

1−αn

1−

1−δ

μ

rnB1xnB1q xnun

+ 2ξn

1−αn

1−

1δ

μ

λ1unynA1unA1q

+ 2ξnαn

1αn

1

1−δ

μ

γf(xn)−Aqynq

+ (1−ξn)xnq2− xnvn 2+ 2(1−ξn)snB2xnB2q xnvn

vnwn 2+ 2(1−ξn)λ2 vnwn A2vnA2q.

Then, we derive

xnun 2+unyn

2

+ xnvn 2+ vnwn 2

ξnαnγf(xn)−Aq2+xnq2−xn+1−q2

+ 2ξn

1−αn

1−

1−δ

μ

rnB1xnB1q xnun

+ 2ξn

1−αn

1−

1−δ

μ

λ1unynA1unA1q

+ 2ξnαn

1−αn

1−

1−δ

μ

γf(xn)−Aqynq

+ 2(1−ξn)snB2xnB2q xnvn + 2(1−ξn)λ2 vnwn A2vnA2q

=ξnαnλf(xn)−Aq2+ xn+1−xn (xnq+xn+1−q)

+ 2ξn

1−αn

1−

1−δ

μ

rnB1xnB1q xnun

+ 2ξn

1−αn

1−

1−δ

μ

λ1unynA1unA1q

+ 2ξnαn

1−αn

1−

1−δ

μ

γf(xn)−Aqynq

(23)

By conditions (C1)-(C4), limn®∞||xn-xn+1|| = 0, limn®∞||B1xn-B1q|| = 0, limn®∞ || B2xn-B2q|| = 0, limn®∞||A1un -A1q|| = 0, limn®∞||A2vn- A2q|| = 0, ||xn-un||® 0, ||xn-vn||® 0, ||vn-wn||®0 as n® ∞. So, we have unyn→0. It follows that

xnwnxnvn + vnwn →0, asn→ ∞.

We compute that

xn+1−xn =ξn(znxn) + (1−ξn)(PCwnxn)

ξn znxn + (1−ξn) wnxn .

From limn®∞||xn-wn|| = 0, limn®∞||xn+1-xn|| = 0, and hence

lim

n→∞ znxn = 0. (3:41)

It follows by step 4 (i) and (ii),

xnynxnun +unyn→0, asn→ ∞.

Since

znynznxn +xnyn.

So, by (3.41) and limn®∞||xn-yn|| = 0, we obtain

lim

n→∞znyn= 0. (3:42)

We show Synzn→0asn®∞. By nonexpansiveness ofPCnotice that

Synzn=SynPC[αnγf(xn) + (IαnA)Syn]

=PCSynPC[αnγf(xn) + (IαnA)Syn]

Synαnγf(xn)−(IαnA)Syn

αnγf(xn)−ASyn.

By condition (C1), we get limn→∞Synzn= 0. Since

SynynSynzn+znyn+ynun+unyn, so by (3.42),

limn→∞Synzn= 0, limn→∞ynun= 0 and limn→∞unyn= 0, we obtain

limn→∞Synyn= 0.

Step 5. We show thatq ÎΘ:=F(S)∩ GMEP(F1,1,B1)∩GMEP(F2, 2,B2)∩I(Al,

M1)∩I(A2, M2) and lim supn→∞

(γfA)q,Synq≤0. It is easy to see that PΘ(gf + (I-A)) is a contraction ofHinto itself. In fact, from Lemma 2.9, we have

P(γf+ (IA))xP(γf+ (IA))y≤(γf+ (IA))x−(γf+ (IA))y

γf(x)−f(y)+ (IA)xy

γ αxy+

1−

1−

1−δ

μ

xy

=

1−δ

μ +γ α

(24)

HenceHis complete, there exists a unique fixed pointq ÎHsuch thatq =PΘ(gf+ (I-A))(q). By Lemma 2.2 we obtain that〈(gf- A)q, w- q〉≤0 for allwÎΘ.

Next, we show that lim supn→∞(γfA)q,Synq≤0, whereq =PΘ(gf+I - A) (q) is the unique solution of the variational inequality〈(gf- A)q, p- q〉≥ 0,∀pÎ Θ. We can choose a subsequence {yni} of {yn} such that

lim sup

n→∞

(γfA)q,Synq= lim

i→∞

(γfA)q,Syniq.

Since {yni} is bounded, there exists a subsequence {ynij} of {yni} which converges

weakly to w. We may assume without loss of generality that yni w.

We claim thatwÎΘ. Since ynSyn→0 and by Lemma 2.6, we havewÎF(S). Next, we show that wÎ GMEP(F1,1,B1). Since un=Tr(nF1,ϕ1)(xnrnB1xn), we know

that

F1(un,y) +ϕ1(y)−ϕ1(un) +

B1xn,yun

+ 1

rn

yun,unxn

≥0, ∀yC.

It follows by (A2) that

ϕ1(y)−ϕ1(un) +

B1xn,yun

+ 1

rn

yun,unxn

F1(y,un), ∀yC.

Hence,

ϕ1(y)−ϕ1(uni) +

B1xni,yuni

+ 1

rni

yuni,unixni

F1(y,uni), ∀yC. (3:43)

FortÎ(0, 1] andy ÎH, letyt=ty+ (1 -t)w. From (3.43), we have

ytuni,B1yt

ytuni,B1yt

ϕ1(yt) +ϕ1(uni)−

B1xni,ytuni

− 1 rni

ytuni,unixni

+F1(yt,uni)

=ytuni,B1ytB1uni

+ytuni,B1uniB1xni

ϕ1(yt) +ϕ1(uni)

− 1 rni

ytuni,unixni

+F1(yt,uni).

From unixni→0, we have B1uniB1xni→0. Further, from (A4) and the

weakly lower semicontinuity of ϕ1,unixni

rni →0 and uni w, we have

ytw,B1yt

References

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