Hindawi Publishing Corporation Journal of Applied Mathematics Volume 2013, Article ID 761864, 21 pages http://dx.doi.org/10.1155/2013/761864 Research Article Composite Iterative Algorithms for Variational Inequality and Fixed Point Problems in Real Smooth and Uniformly Convex Banach Spaces Lu-Chuan Ceng1 and Ching-Feng Wen2 1 Department of Mathematics, Shanghai Normal University and Scientific Computing Key Laboratory of Shanghai Universities, Shanghai 200234, China 2 Center for Fundamental Science, Kaohsiung Medical University, Kaohsiung 807, Taiwan Correspondence should be addressed to Ching-Feng Wen; cfwen@kmu.edu.tw Received 30 April 2013; Accepted 6 June 2013 Academic Editor: Wei-Shih Du Copyright © 2013 L.-C. Ceng and C.-F. Wen. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. We introduce composite implicit and explicit iterative algorithms for solving a general system of variational inequalities and a common fixed point problem of an infinite family of nonexpansive mappings in a real smooth and uniformly convex Banach space. These composite iterative algorithms are based on Korpelevich’s extragradient method and viscosity approximation method. We first consider and analyze a composite implicit iterative algorithm in the setting of uniformly convex and 2-uniformly smooth Banach space and then another composite explicit iterative algorithm in a uniformly convex Banach space with a uniformly GaΜteaux differentiable norm. Under suitable assumptions, we derive some strong convergence theorems. The results presented in this paper improve, extend, supplement, and develop the corresponding results announced in the earlier and very recent literatures. 1. Introduction Let π be a real Banach space whose dual space is denoted by ∗ π∗ . The normalized duality mapping π½ : π → 2π is defined by σ΅© σ΅©2 π½ (π₯) = {π₯∗ ∈ π∗ : β¨π₯, π₯∗ β© = βπ₯β2 = σ΅©σ΅©σ΅©π₯∗ σ΅©σ΅©σ΅© } , ∀π₯ ∈ π, (1) where β¨⋅, ⋅β© denotes the generalized duality pairing. It is an immediate consequence of the Hahn-Banach theorem that π½(π₯) is nonempty for each π₯ ∈ π. Let πΆ be a nonempty, closed, and convex subset of π. A mapping π : πΆ → C is called nonexpansive if βππ₯ − ππ¦β ≤ βπ₯ − π¦β for every π₯, π¦ ∈ πΆ. The set of fixed points of π is denoted by Fix(π). We use the notation β to indicate the weak convergence and the one → to indicate the strong convergence. A mapping π΄ : πΆ → π is said to be accretive if for each π₯, π¦ ∈ πΆ, there exists π(π₯ − π¦) ∈ π½(π₯ − π¦) such that β¨π΄π₯ − π΄π¦, π (π₯ − π¦)β© ≥ 0. (2) It is said to be πΌ-strongly accretive if for each π₯, π¦ ∈ πΆ, there exists π(π₯ − π¦) ∈ π½(π₯ − π¦) such that σ΅©2 σ΅© β¨π΄π₯ − π΄π¦, π (π₯ − π¦)β© ≥ πΌσ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅© , (3) for some πΌ ∈ (0, 1). The mapping is called π½-inverse stronglyaccretive if for each π₯, π¦ ∈ πΆ, there exists π(π₯ − π¦) ∈ π½(π₯ − π¦) such that σ΅©2 σ΅© β¨π΄π₯ − π΄π¦, π (π₯ − π¦)β© ≥ π½σ΅©σ΅©σ΅©π΄π₯ − π΄π¦σ΅©σ΅©σ΅© , (4) for some π½ > 0 and is said to be π-strictly pseudocontractive if for each π₯, π¦ ∈ πΆ, there exists π(π₯ − π¦) ∈ π½(π₯ − π¦) such that σ΅©2 σ΅©2 σ΅© σ΅© β¨π΄π₯ − π΄π¦, π (π₯ − π¦)β© ≤ σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅© − πσ΅©σ΅©σ΅©π₯ − π¦ − (π΄π₯ − π΄π¦)σ΅©σ΅©σ΅© (5) for some π ∈ (0, 1). 2 Journal of Applied Mathematics Let π = {π₯ ∈ π :β π₯ β= 1} denote the unite sphere of π. A Banach space π is said to be uniformly convex if for each π ∈ (0, 2], there exists πΏ > 0 such that for all π₯, π¦ ∈ π, σ΅© σ΅©σ΅© σ΅©π₯ + π¦σ΅©σ΅©σ΅© σ΅© σ΅©σ΅© ≤ 1 − πΏ. σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅© ≥ π σ³¨⇒ σ΅© 2 (6) It is known that a uniformly convex Banach space is reflexive and strict convex. A Banach space π is said to be smooth if the limit β π₯ + π‘π¦ β − β π₯ β π‘→0 π‘ (7) lim exists for all π₯, π¦ ∈ π; in this case, π is also said to have a GaΜteaux differentiable norm. π is said to have a uniformly GaΜteaux differentiable norm if for each π¦ ∈ π, the limit is attained uniformly for π₯ ∈ π. Moreover, it is said to be uniformly smooth if this limit is attained uniformly for π₯, π¦ ∈ π. The norm of π is said to be the FreΜchet differential if for each π₯ ∈ π, this limit is attained uniformly for π¦ ∈ π. In addition, we define a function π : [0, ∞) → [0, ∞) called the modulus of smoothness of π as follows: 1 σ΅© σ΅© σ΅© σ΅© π (π) = sup { (σ΅©σ΅©σ΅©π₯ + π¦σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅©) 2 σ΅© σ΅© − 1 : π₯, π¦ ∈ π, βπ₯β = 1, σ΅©σ΅©σ΅©π¦σ΅©σ΅©σ΅© = π} . (8) It is known that π is uniformly smooth if and only if limπ → 0 π(π)/π = 0. Let π be a fixed real number with 1 < π ≤ 2. Then a Banach space π is said to be π-uniformly smooth if there exists a constant π > 0 such that π(π) ≤ πππ for all π > 0. As pointed out in [1], no Banach space is π-uniformly smooth for π > 2. In addition, it is also known that π½ is single-valued if and only if π is smooth, whereas if π is uniformly smooth, then the mapping π½ is norm-to-norm uniformly continuous on bounded subsets of π. If π has a uniformly GaΜteaux differentiable norm, then the duality mapping π½ is norm-toweak∗ uniformly continuous on bounded subsets of π. Very recently, Cai and Bu [2] considered the following general system of variational inequalities (GSVI) in a real smooth Banach space π, which involves finding (π₯∗ , π¦∗ ) ∈ πΆ × πΆ such that β¨π1 π΅1 π¦∗ + π₯∗ − π¦∗ , π½ (π₯ − π₯∗ )β© ≥ 0, ∗ ∗ ∗ ∗ β¨π2 π΅2 π₯ + π¦ − π₯ , π½ (π₯ − π¦ )β© ≥ 0, ∀π₯ ∈ πΆ, ∀π₯ ∈ πΆ, (9) where πΆ is a nonempty, closed, and convex subset of π, π΅1 , and π΅2 : πΆ → π are two nonlinear mappings, and π1 and π2 are two positive constants. Here the set of solutions of GSVI (9) is denoted by GSVI(πΆ, π΅1 , π΅2 ). In particular, if π = π», a real Hilbert space, then GSVI (9) reduces to the following GSVI of finding (π₯∗ , π¦∗ ) ∈ πΆ × πΆ such that β¨π1 π΅1 π¦∗ + π₯∗ − π¦∗ , π₯ − π₯∗ β© ≥ 0, ∀π₯ ∈ πΆ, β¨π2 π΅2 π₯∗ + π¦∗ − π₯∗ , π₯ − π¦∗ β© ≥ 0, ∀π₯ ∈ πΆ, (10) which π1 and π2 are two positive constants. The set of solutions of problem (10) is still denoted by GSVI(πΆ, π΅1 , π΅2 ). It is clear that the problem (10) covers as special case the classical variational inequality problem (VIP) of finding π₯∗ ∈ πΆ such that β¨π΄π₯∗ , π₯ − π₯∗ β© ≥ 0, ∀π₯ ∈ πΆ. (11) The solution set of the VIP (11) is denoted by VI(πΆ, π΄). Recently, Ceng et al. [3] transformed problem (10) into a fixed point problem in the following way. Lemma 1 (see [3]). For given π₯, π¦ ∈ πΆ, (π₯, π¦) is a solution of problem (10) if and only if π₯ is a fixed point of the mapping πΊ : πΆ → πΆ defined by πΊ (π₯) = ππΆ [ππΆ (π₯ − π2 π΅2 π₯) − π1 π΅1 ππΆ × (π₯ − π2 π΅2 π₯)] , ∀π₯ ∈ πΆ, (12) where π¦ = ππΆ(π₯−π2 π΅2 π₯) and ππΆ is the the projection of π» onto πΆ. In particular, if the mappings π΅π : πΆ → π» is π½π -inverse strongly monotone for π = 1, 2, then the mapping πΊ is nonexpansive provided ππ ∈ (0, 2π½π ) for π = 1, 2. Let πΆ be a nonempty, closed, and convex subset of a real smooth Banach space π. Let ΠπΆ be a sunny nonexpansive retraction from π onto πΆ, and let π : πΆ → πΆ be a contraction with coefficient π ∈ (0, 1). In this paper we introduce composite implicit and explicit iterative algorithms for solving GSVI (9) and the common fixed point problem of an infinite family {ππ } of nonexpansive mappings of πΆ into itself. These composite iterative algorithms are based on Korpelevich’s extragradient method [4] and viscosity approximation method [5]. Let the mapping πΊ be defined by πΊ (π₯) := ΠπΆ (πΌ − π1 π΅1 ) ΠπΆ (πΌ − π2 π΅2 ) π₯, ∀π₯ ∈ πΆ. (13) We first propose a composite implicit iterative algorithm in the setting of uniformly convex and 2-uniformly smooth Banach space π: π¦π = πΌπ π (π¦π ) + (1 − πΌπ ) ππ πΊ (π₯π ) , π₯π+1 = π½π π₯π + πΎπ π¦π + πΏπ ππ πΊ (π¦π ) , ∀π ≥ 0, (14) where π΅π : πΆ → π is πΌπ -inverse-strongly accretive with 0 < ππ < πΌπ /π 2 for π = 1, 2 and {πΌπ }, {π½π }, {πΎπ }, and {πΏπ } are the sequences in (0, 1) such that π½π + πΎπ + πΏπ = 1 for all π ≥ 0. It is proven that under appropriate conditions, {π₯π } converges strongly to π ∈ πΉ = β∞ π=0 Fix(ππ ) ∩ Ω, which solves the following VIP: β¨π − π (π) , π½ (π − π)β© ≤ 0, ∀π ∈ πΉ. (15) On the other hand, we also propose another composite explicit iterative algorithm in a uniformly convex Banach space π with a uniformly Gateaux differentiable norm: π¦π = πΌπ πΊ (π₯π ) + (1 − πΌπ ) ππ πΊ (π₯π ) , π₯π+1 = π½π π (π₯π ) + πΎπ π¦π + πΏπ ππ πΊ (π¦π ) , ∀π ≥ 0, (16) Journal of Applied Mathematics 3 where π΅π : πΆ → π is π π -strictly pseudocontractive and πΌπ strongly accretive with πΌπ + π π ≥ 1 for π = 1, 2 and {πΌπ }, {π½π }, {πΎπ }, and {πΏπ } are the sequences in (0, 1) such that π½π + πΎπ + πΏπ = 1 for all π ≥ 0. It is proven that under mild conditions, {π₯π } also converges strongly to π ∈ πΉ = β∞ π=0 Fix(ππ ) ∩ Ω, which solves the VIP (15). The results presented in this paper improve, extend, supplement, and develop the corresponding results announced in the earlier and very recent literatures. 2. Preliminaries We list some lemmas that will be used in the sequel. Lemma 2 can be found in [6]. Lemma 3 is an immediate consequence of the subdifferential inequality of the function (1/2)β ⋅ β2 . Lemma 2. Let {π π } be a sequence of nonnegative real numbers satisfying π π+1 ≤ (1 − πΌπ ) π π + πΌπ π½π + πΎπ , ∀π ≥ 0, (17) (i) Π is sunny and nonexpansive; (ii) β Π(π₯) − Π(π¦)β2 ≤ β¨π₯ − π¦, π½(Π(π₯) − Π(π¦))β©, ∀π₯, π¦ ∈ πΆ; (iii) β¨π₯ − Π(π₯), π½(π¦ − Π(π₯))β© ≤ 0, ∀π₯ ∈ πΆ, π¦ ∈ π·. It is well known that if π = π» a Hilbert space, then a sunny nonexpansive retraction ΠπΆ is coincident with the metric projection from π onto πΆ; that is, ΠπΆ = ππΆ. If πΆ is a nonempty, closed, and convex subset of a strictly convex and uniformly smooth Banach space π and if π : πΆ → πΆ is a nonexpansive mapping with the fixed point set Fix(π) =ΜΈ 0, then the set Fix(π) is a sunny nonexpansive retract of πΆ. Lemma 6 (see [9]). Given a number π > 0. A real Banach space π is uniformly convex if and only if there exists a continuous strictly increasing function π : [0, ∞) → [0, ∞), π(0) = 0, such that σ΅©2 σ΅©σ΅© σ΅©σ΅©ππ₯ + (1 − π) π¦σ΅©σ΅©σ΅© σ΅© σ΅©2 σ΅© σ΅© ≤ πβπ₯β2 + (1 − π) σ΅©σ΅©σ΅©π¦σ΅©σ΅©σ΅© − π (1 − π) π (σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅©) where {πΌπ }, {π½π }, and {πΎπ } satisfy the conditions: (21) (i) {πΌπ } ⊂ [0, 1] and ∑∞ π=0 πΌπ = ∞, for all π ∈ [0, 1] and π₯, π¦ ∈ π such that β π₯ β≤ π and β π¦ β≤ π. (ii) lim supπ → ∞ π½π ≤ 0, Lemma 7 (see [10]). Let πΆ be a nonempty, closed, and convex subset of a Banach space π. Let π0 , π1 , . . ., be a sequence of mappings of πΆ into itself. Suppose that ∑∞ π=1 sup{βππ π₯−ππ−1 π₯β : π₯ ∈ πΆ} < ∞. Then for each π¦ ∈ πΆ, {ππ π¦} converges strongly to some point of πΆ. Moreover, let π be a mapping of πΆ into itself defined by ππ¦ = limπ → ∞ ππ π¦ for all π¦ ∈ πΆ. Then limπ → ∞ sup{β ππ₯ − ππ π₯ β: π₯ ∈ πΆ} = 0. (iii) πΎπ ≥ 0, ∀π ≥ 0, and ∑∞ π=0 πΎπ < ∞. Then lim supπ → ∞ π π = 0. Lemma 3. In a smooth Banach space π, there holds the inequality σ΅©2 σ΅©σ΅© 2 σ΅©σ΅©π₯ + π¦σ΅©σ΅©σ΅© ≤ βπ₯β + 2 β¨π¦, π½ (π₯ + π¦)β© , ∀π₯, π¦ ∈ π. (18) Lemma 4 (see [7]). Let {π₯π } and {π§π } be bounded sequences in a Banach space π, and let {πΌπ } be a sequence in [0, 1] which satisfies the following condition: 0 < lim inf πΌπ ≤ lim sup πΌπ < 1. π→∞ π→∞ (19) Suppose that π₯π+1 = πΌπ π₯π + (1 − πΌπ )π§π , ∀π ≥ 0, and lim supπ → ∞ (β π§π+1 − π§π β − β π₯π+1 − π₯π β) ≤ 0. Then limπ → ∞ β π§π − π₯π β= 0. Let π· be a subset of πΆ, and let Π be a mapping of πΆ into π·. Then Π is said to be sunny if Π [Π (π₯) + π‘ (π₯ − Π (π₯))] = Π (π₯) , (20) whenever Π(π₯) + π‘(π₯ − Π(π₯)) ∈ πΆ for π₯ ∈ πΆ and π‘ ≥ 0. A mapping Π of πΆ into itself is called a retraction if Π2 = Π. If a mapping Π of πΆ into itself is a retraction, then Π(π§) = π§ for every π§ ∈ π (Π) where π (Π) is the range of Π. A subset π· of πΆ is called a sunny nonexpansive retract of πΆ if there exists a sunny nonexpansive retraction from πΆ onto π·. The following lemma concerns the sunny nonexpansive retraction. Lemma 5 (see [8]). Let πΆ be a nonempty, closed, and convex subset of a real smooth Banach space π. Let π· be a nonempty subset of πΆ. Let Π be a retraction of πΆ onto π·. Then the following are equivalent: Let πΆ be a nonempty, closed, and convex subset of a Banach space π, and let π : πΆ → πΆ be a nonexpansive mapping with Fix(π) =ΜΈ 0. As previous, let ΞπΆ be the set of all contractions on πΆ. For π‘ ∈ (0, 1) and π ∈ ΞπΆ, let π₯π‘ ∈ πΆ be the unique fixed point of the contraction π₯ σ³¨→ π‘π(π₯) + (1 − π‘)ππ₯ on πΆ; that is, π₯π‘ = π‘π (π₯π‘ ) + (1 − π‘) ππ₯π‘ . (22) Lemma 8 (see [11, 12]). Let π be a uniformly smooth Banach space or a reflexive and strictly convex Banach space with a uniformly Gateaux differentiable norm. Let πΆ be a nonempty, closed, and convex subset of π, let π : πΆ → πΆ be a nonexpansive mapping with Fix(π) =ΜΈ 0, and π ∈ ΞπΆ. Then the net {π₯π‘ } defined by π₯π‘ = π‘π(π₯π‘ ) + (1 − π‘)ππ₯π‘ converges strongly to a point in Fix(π). If we define a mapping π : ΞπΆ → Fix(π) by π(π) := π − limπ‘ → 0 π₯π‘ , ∀π ∈ ΞπΆ, then π(π) solves the VIP: β¨(πΌ − π) π (π) , π½ (π (π) − π)β© ≤ 0, ∀π ∈ ΞπΆ, π ∈ Fix (π) . (23) Lemma 9 (see [13]). Let πΆ be a nonempty, closed, and convex subset of a strictly convex Banach space π. Let {ππ }∞ π=0 be a sequence of nonexpansive mappings on πΆ. Suppose that β∞ π=0 Fix(ππ ) is nonempty. Let {π π } be a sequence of positive numbers with ∑∞ π=0 π π = 1. Then a mapping π on πΆ defined by π π π₯ for π₯ ∈ πΆ is defined well, nonexpansive, and ππ₯ = ∑∞ π π π=0 Fix(π) = β∞ π=0 Fix(ππ ) holds. 4 Journal of Applied Mathematics 3. Implicit Iterative Schemes In this section, we introduce our implicit iterative schemes and show the strong convergence theorems. We will use the following useful lemmas in the sequel. Lemma 10 (see [2, Lemma 2.8]). Let πΆ be a nonempty, closed, and convex subset of a real 2-uniformly smooth Banach space π. Let the mapping π΅π : πΆ → π be πΌπ -inverse-strongly accretive. Then, one has σ΅©σ΅©σ΅©(πΌ − ππ π΅π ) π₯ − (πΌ − ππ π΅π ) π¦σ΅©σ΅©σ΅©2 σ΅© σ΅© σ΅©σ΅©2 σ΅©σ΅© (24) ≤ σ΅©σ΅©π₯ − π¦σ΅©σ΅© + 2ππ (ππ π 2 − πΌπ ) σ΅©2 σ΅© × σ΅©σ΅©σ΅©π΅π π₯ − π΅π π¦σ΅©σ΅©σ΅© , ∀π₯, π¦ ∈ πΆ, for π = 1, 2, where ππ > 0. In particular, if 0 < ππ ≤ πΌπ /π 2 , then πΌ − ππ π΅π is nonexpansive for π = 1, 2. Lemma 11 (see [2, Lemma 2.9]). Let πΆ be a nonempty, closed, and convex subset of a real 2-uniformly smooth Banach space π. Let ΠπΆ be a sunny nonexpansive retraction from π onto πΆ. Let the mapping π΅π : πΆ → π be πΌπ -inverse-strongly accretive for π = 1, 2. Let πΊ : πΆ → πΆ be the mapping defined by πΊ (π₯) = ΠπΆ [ΠπΆ (π₯ − π2 π΅2 π₯) −π1 π΅1 ΠπΆ (π₯ − π2 π΅2 π₯)] , ∀π₯ ∈ πΆ. (25) If 0 < ππ ≤ πΌπ /π 2 for π = 1, 2, then πΊ : πΆ → πΆ is nonexpensive. Lemma 12 (see [2, Lemma 2.10]). Let πΆ be a nonempty, closed, and convex subset of a real 2-uniformly smooth Banach space π. Let ΠπΆ be a sunny nonexpansive retraction from π onto πΆ. Let π΅1 , π΅2 : πΆ → π be two nonlinear mappings. For given π₯∗ , π¦∗ ∈ πΆ, (π₯∗ , π¦∗ ) is a solution of GSVI (9) if and only if π₯∗ = ΠπΆ(π¦∗ − π1 π΅1 π¦∗ ) where π¦∗ = ΠπΆ(π₯∗ − π2 π΅2 π₯∗ ). (i) limπ → ∞ πΌπ = 0 and ∑∞ π=0 πΌπ = ∞, (ii) 0 < lim inf π → ∞ π½π ≤ lim supπ → ∞ (π½π + πΎπ ) < 1 and lim inf π → ∞ πΎπ > 0, (iii) limπ → ∞ |πΎπ /(1 − π½π ) − πΎπ−1 /(1 − π½π−1 )| = 0. Assume that ∑∞ π=1 supπ₯∈π· β ππ π₯−ππ−1 π₯ β< ∞ for any bounded subset π· of πΆ, and let π be a mapping of πΆ into itself defined by ππ₯ = limπ → ∞ ππ π₯ for all π₯ ∈ πΆ. Suppose that Fix(π) = β∞ π=0 Fix(ππ ). Then {π₯π } converges strongly to π ∈ πΉ, which solves the following VIP: β¨π − π (π) , π½ (π − π)β© ≤ 0, ∀π ∈ πΉ. (28) Proof. Take a fixed π ∈ πΉ arbitrarily. Then by Lemma 12, we know that π = πΊ(π) and π = ππ π for all π ≥ 0. Moreover, by Lemma 11, we have σ΅© σ΅©σ΅© σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© σ΅© σ΅© = σ΅©σ΅©σ΅©πΌπ (π (π¦π ) − π) + (1 − πΌπ ) (ππ πΊ (π₯π ) − π)σ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© ≤ πΌπ σ΅©σ΅©σ΅©π (π¦π ) − π (π)σ΅©σ΅©σ΅© + πΌπ σ΅©σ΅©σ΅©π (π) − πσ΅©σ΅©σ΅© σ΅© σ΅© + (1 − πΌπ ) σ΅©σ΅©σ΅©ππ πΊ (π₯π ) − πσ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© ≤ πΌπ π σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© + πΌπ σ΅©σ΅©σ΅©π (π) − πσ΅©σ΅©σ΅© σ΅© σ΅© + (1 − πΌπ ) σ΅©σ΅©σ΅©πΊ (π₯π ) − πσ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© ≤ πΌπ π σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© + πΌπ σ΅©σ΅©σ΅©π (π) − πσ΅©σ΅©σ΅© σ΅© σ΅© + (1 − πΌπ ) σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© , (29) which hence implies that Remark 13. By Lemma 12, we observe that π₯∗ = ΠπΆ [ΠπΆ (π₯∗ − π2 π΅2 π₯∗ ) − π1 π΅1 ΠπΆ (π₯∗ − π2 π΅2 π₯∗ )] , (26) We now state and prove our first result on the implicit iterative scheme. Theorem 14. Let πΆ be a nonempty, closed, and convex subset of a uniformly convex and 2-uniformly smooth Banach space π. Let ΠπΆ be a sunny nonexpansive retraction from π onto πΆ. Let the mapping π΅π : πΆ → π be πΌπ -inverse-strongly accretive for π = 1, 2. Let π : πΆ → πΆ be a contraction with coefficient π ∈ (0, 1). Let {ππ }∞ π=0 be an infinite family of nonexpansive mappings of πΆ into itself such that πΉ = β∞ π=0 Fix(ππ ) ∩ Ω =ΜΈ 0, where Ω is the fixed point set of the mapping πΊ = ΠπΆ(πΌ − π1 π΅1 )ΠπΆ(πΌ − π2 π΅2 ). For arbitrarily given π₯0 ∈ πΆ, let {π₯π } be the sequence generated by π¦π = πΌπ π (π¦π ) + (1 − πΌπ ) ππ πΊ (π₯π ) , ∀π ≥ 0, σ΅©σ΅© σ΅© σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© ≤ (1 − which implies that π₯∗ is a fixed point of the mapping πΊ. π₯π+1 = π½π π₯π + πΎπ π¦π + πΏπ ππ πΊ (π¦π ) , where 0 < ππ < πΌπ /π 2 for π = 1, 2 and {πΌπ }, {π½π }, {πΎπ }, and {πΏπ } are the sequences in (0, 1) such that π½π + πΎπ + πΏπ = 1, ∀π ≥ 0. Suppose that the following conditions hold: (27) + 1−π σ΅© σ΅© πΌ ) σ΅©σ΅©π₯ − πσ΅©σ΅©σ΅© 1 − πΌπ π π σ΅© π 1 σ΅© σ΅© πΌ σ΅©σ΅©π (π) − πσ΅©σ΅©σ΅© 1 − πΌπ π π σ΅© σ΅© σ΅© ≤ σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + (30) πΌπ σ΅©σ΅© σ΅© σ΅©π (π) − πσ΅©σ΅©σ΅© . 1 − πΌπ π σ΅© Thus, from (27), we have σ΅©σ΅© σ΅© σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© σ΅© σ΅© = σ΅©σ΅©σ΅©π½π (π₯π − π) + πΎπ (π¦π − π) + πΏπ (ππ πΊ (π¦π ) − π)σ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© σ΅© σ΅© ≤ π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + πΎπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© + πΏπ σ΅©σ΅©σ΅©πΊ (π¦π ) − πσ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© σ΅© σ΅© ≤ π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + πΎπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© + πΏπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© = π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + (1 − π½π ) σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© Journal of Applied Mathematics 5 σ΅© σ΅© ≤ π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + (1 − π½π ) × {(1 − + = [1 − which hence yields 1−π σ΅© σ΅© πΌ ) σ΅©σ΅©π₯ − πσ΅©σ΅©σ΅© 1 − πΌπ π π σ΅© π σ΅© σ΅©σ΅© σ΅©σ΅©π¦π − π¦π−1 σ΅©σ΅©σ΅© 1 σ΅© σ΅© πΌ σ΅©σ΅©π (π) − πσ΅©σ΅©σ΅©} 1 − πΌπ π π σ΅© ≤ (1 − π½π ) (1 − π) σ΅© σ΅© πΌπ ] σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© 1 − πΌπ π σ΅© σ΅© (1 − π½π ) (1 − π) σ΅©σ΅©σ΅©π (π) − πσ΅©σ΅©σ΅© + πΌπ 1 − πΌπ π 1−π σ΅© σ΅© σ΅© σ΅©σ΅©π (π) − πσ΅©σ΅©σ΅© σ΅© ≤ max {σ΅©σ΅©σ΅©π₯0 − πσ΅©σ΅©σ΅© , σ΅© }. 1−π (31) It immediately follows that {π₯π } is bounded, and so are the sequences {π¦π }, {πΊ(π₯π )}, and {πΊ(π¦π )} due to (30) and the nonexpansivity of πΊ. Let us show that βπ₯π+1 −π₯π β → 0 as π → ∞. As a matter of fact, from (27), we have π¦π = πΌπ π (π¦π ) + (1 − πΌπ ) ππ πΊ (π₯π ) , π¦π−1 = πΌπ−1 π (π¦π−1 ) + (1 − πΌπ−1 ) ππ−1 πΊ (π₯π−1 ) , 1 − πΌπ σ΅©σ΅© σ΅© (σ΅©π₯ − π₯π−1 σ΅©σ΅©σ΅© 1 − πΌπ π σ΅© π σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅©) σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨πΌπ − πΌπ−1 σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σ΅© + σ΅©π (π¦π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© 1 − πΌπ π σ΅© σ΅© σ΅© σ΅© σ΅© ≤ σ΅©σ΅©σ΅©π₯π − π₯π−1 σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅¨σ΅¨ σ΅¨ σ΅¨πΌ − πΌπ−1 σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σ΅© +σ΅¨ π σ΅©π (π¦π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© . 1−πΌ π σ΅© π Now, we write π₯π = π½π−1 π₯π−1 + (1 − π½π−1 )π§π−1 , ∀π ≥ 1, where π§π−1 = (π₯π − π½π−1 π₯π−1 )/(1 − π½π−1 ). It follows that for all π ≥ 1, π§π − π§π−1 = = ∀π ≥ 1. (32) + (πΌπ − πΌπ−1 ) (π (π¦π−1 ) − ππ−1 πΊ (π₯π−1 )) = (33) + (1 − πΌπ ) (ππ πΊ (π₯π ) − ππ−1 πΊ (π₯π−1 )) . It follows that σ΅©σ΅© σ΅© σ΅©σ΅©π¦π − π¦π−1 σ΅©σ΅©σ΅© σ΅© σ΅¨ σ΅© σ΅¨ ≤ πΌπ σ΅©σ΅©σ΅©π (π¦π ) − π (π¦π−1 )σ΅©σ΅©σ΅© + σ΅¨σ΅¨σ΅¨πΌπ − πΌπ−1 σ΅¨σ΅¨σ΅¨ σ΅© σ΅© × σ΅©σ΅©σ΅©π (π¦π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + (1 − πΌπ ) σ΅©σ΅©σ΅©ππ πΊ (π₯π ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅¨ σ΅¨ σ΅© ≤ πΌπ π σ΅©σ΅©σ΅©π¦π − π¦π−1 σ΅©σ΅©σ΅© + σ΅¨σ΅¨σ΅¨πΌπ − πΌπ−1 σ΅¨σ΅¨σ΅¨ σ΅© σ΅© × σ΅©σ΅©σ΅©π (π¦π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© + (1 − πΌπ ) (34) σ΅© σ΅© × (σ΅©σ΅©σ΅©ππ πΊ (π₯π ) − ππ πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅©) σ΅© σ΅¨ σ΅¨ σ΅© ≤ πΌπ π σ΅©σ΅©σ΅©π¦π − π¦π−1 σ΅©σ΅©σ΅© + σ΅¨σ΅¨σ΅¨πΌπ − πΌπ−1 σ΅¨σ΅¨σ΅¨ σ΅© σ΅© × σ΅©σ΅©σ΅©π (π¦π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© + (1 − πΌπ ) σ΅© σ΅© × (β π₯π − π₯π−1 β + σ΅©σ΅©σ΅©ππ πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅©) , π₯π+1 − π½π π₯π π₯π − π½π−1 π₯π−1 − 1 − π½π 1 − π½π−1 πΎπ π¦π + πΏπ ππ πΊ (π¦π ) 1 − π½π − Simple calculations show that π¦π − π¦π−1 = πΌπ (π (π¦π ) − π (π¦π−1 )) (35) πΎπ−1 π¦π−1 + πΏπ−1 ππ−1 πΊ (π¦π−1 ) 1 − π½π−1 πΎπ (π¦π − π¦π−1 ) + πΏπ (ππ πΊ (π¦π ) − ππ−1 πΊ (π¦π−1 )) 1 − π½π +( πΎπ πΎπ−1 − )π¦ 1 − π½π 1 − π½π−1 π−1 +( πΏπ−1 πΏπ − ) π πΊ (π¦π−1 ) . 1 − π½π 1 − π½π−1 π−1 (36) This together with (35) implies that σ΅© σ΅©σ΅© σ΅©σ΅©π§π − π§π−1 σ΅©σ΅©σ΅© σ΅©σ΅© σ΅© σ΅©πΎ (π¦ − π¦π−1 ) + πΏπ (ππ πΊ (π¦π ) − ππ−1 πΊ (π¦π−1 ))σ΅©σ΅©σ΅© ≤σ΅© π π 1 − π½π σ΅¨σ΅¨ πΎ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σ΅¨ σ΅© + σ΅¨σ΅¨σ΅¨ π − σ΅¨ σ΅©π¦ σ΅©σ΅© σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨σ΅¨ σ΅© π−1 σ΅© σ΅¨σ΅¨ πΏ πΏπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σ΅¨ σ΅© + σ΅¨σ΅¨σ΅¨ π − σ΅¨ σ΅©π πΊ (π¦π−1 )σ΅©σ΅©σ΅© σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨σ΅¨ σ΅© π−1 σ΅© σ΅© ≤ (πΎπ σ΅©σ΅©σ΅©π¦π − π¦π−1 σ΅©σ΅©σ΅© σ΅© σ΅© + πΏπ (σ΅©σ΅©σ΅©ππ πΊ (π¦π ) − ππ πΊ (π¦π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π¦π−1 ) − ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅©)) 6 Journal of Applied Mathematics −1 × (1 − π½π ) Hence we obtain σ΅¨σ΅¨ πΎ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σ΅¨ σ΅© + σ΅¨σ΅¨σ΅¨ π − σ΅¨ σ΅©π¦ σ΅©σ΅© σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨σ΅¨ σ΅© π−1 σ΅© σ΅¨σ΅¨σ΅¨ πΎ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σ΅© + σ΅¨σ΅¨σ΅¨ π − σ΅¨σ΅¨ σ΅©σ΅©ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅© σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨ σ΅© σ΅© σ΅© σ΅© πΎ σ΅©σ΅©π¦ − π¦π−1 σ΅©σ΅©σ΅© + πΏπ σ΅©σ΅©σ΅©π¦π − π¦π−1 σ΅©σ΅©σ΅© ≤ πσ΅© π πΎπ + πΏπ σ΅©σ΅© lim σ΅©π₯ π → ∞ σ΅© π+1 πΏπ σ΅©σ΅© σ΅© σ΅©π πΊ (π¦π−1 ) − ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅© πΎπ + πΏπ σ΅© π σ΅¨σ΅¨ πΎ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σ΅¨ σ΅© σ΅© σ΅© + σ΅¨σ΅¨σ΅¨ π − σ΅¨ (σ΅©π¦ σ΅©σ΅© + σ΅©σ΅©π πΊ (π¦π−1 )σ΅©σ΅©σ΅©) σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨σ΅¨ σ΅© π−1 σ΅© σ΅© π−1 σ΅© σ΅© σ΅© σ΅© ≤ σ΅©σ΅©σ΅©π¦π − π¦π−1 σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π¦π−1 ) − ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅© σ΅¨σ΅¨ πΎ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σ΅¨ σ΅© σ΅© σ΅© + σ΅¨σ΅¨σ΅¨ π − σ΅¨ (σ΅©π¦ σ΅©σ΅© + σ΅©σ΅©π πΊ (π¦π−1 )σ΅©σ΅©σ΅©) σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨σ΅¨ σ΅© π−1 σ΅© σ΅© π−1 σ΅© σ΅© σ΅© σ΅© ≤ σ΅©σ΅©σ΅©π₯π − π₯π−1 σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨πΌπ − πΌπ−1 σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σ΅© + σ΅©π (π¦π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© 1 − πΌπ π σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π¦π−1 ) − ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅© σ΅¨σ΅¨ πΎ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σ΅¨ σ΅© σ΅© σ΅© + σ΅¨σ΅¨σ΅¨ π − σ΅¨ (σ΅©π¦ σ΅©σ΅© + σ΅©σ΅©π πΊ (π¦π−1 )σ΅©σ΅©σ΅©) σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨σ΅¨ σ΅© π−1 σ΅© σ΅© π−1 σ΅© σ΅© σ΅© σ΅© ≤ σ΅©σ΅©σ΅©π₯π − π₯π−1 σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅¨σ΅¨ σ΅¨ σ΅¨πΌ − πΌπ−1 σ΅¨σ΅¨σ΅¨ σ΅© σ΅© +σ΅¨ π π + σ΅©σ΅©σ΅©ππ πΊ (π¦π−1 ) − ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅© 1−πΌ π π σ΅¨σ΅¨ πΎ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨ + σ΅¨σ΅¨σ΅¨ π − σ΅¨π σ΅¨σ΅¨ 1 − π½π 1 − π½n−1 σ΅¨σ΅¨σ΅¨ σ΅© σ΅© = σ΅©σ΅©σ΅©π₯π − π₯π−1 σ΅©σ΅©σ΅© σ΅¨ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ 1 σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ πΎ σ΅¨) σ΅¨σ΅¨πΌπ − πΌπ−1 σ΅¨σ΅¨σ΅¨ + σ΅¨σ΅¨σ΅¨ π − σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨σ΅¨ 1 − πΌπ π σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π¦π−1 ) − ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅© , (37) + π( where supπ≥0 {βπ(π¦π )β + βππ πΊ(π₯π )β + βπ¦π β + βππ πΊ(π¦π )β} ≤ π for some π > 0. So, from πΌπ → 0, condition (iii), and the assumption on {ππ }, it immediately follows that π→∞ (38) σ΅©σ΅© σ΅© − π₯π σ΅©σ΅©σ΅© = 0. σ΅©2 σ΅© σ΅©2 σ΅©σ΅© σ΅©σ΅©π’π − πσ΅©σ΅©σ΅© = σ΅©σ΅©σ΅©ΠπΆ (π₯π − π2 π΅2 π₯π ) − ΠπΆ (π − π2 π΅2 π)σ΅©σ΅©σ΅© σ΅© σ΅©2 ≤ σ΅©σ΅©σ΅©π₯π − π − π2 (π΅2 π₯π − π΅2 π)σ΅©σ΅©σ΅© σ΅© σ΅©2 σ΅© σ΅©2 ≤ σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© − 2π2 (πΌ2 − π 2 π2 ) σ΅©σ΅©σ΅©π΅2 π₯π − π΅2 πσ΅©σ΅©σ΅© , (41) σ΅©σ΅© σ΅©2 σ΅© σ΅©2 σ΅©σ΅©Vπ − πσ΅©σ΅©σ΅© = σ΅©σ΅©σ΅©ΠπΆ (π’π − π1 π΅1 π’π ) − ΠπΆ (π − π1 π΅1 π)σ΅©σ΅©σ΅© σ΅© σ΅©2 ≤ σ΅©σ΅©σ΅©π’π − π − π1 (π΅1 π’π − π΅1 π)σ΅©σ΅©σ΅© σ΅© σ΅©2 σ΅© σ΅©2 ≤ σ΅©σ΅©σ΅©π’π − πσ΅©σ΅©σ΅© − 2π1 (πΌ1 − π 2 π1 ) σ΅©σ΅©σ΅©π΅1 π’π − π΅1 πσ΅©σ΅©σ΅© . (42) Substituting (41) into (42), we obtain σ΅©σ΅© σ΅©2 σ΅© σ΅©2 σ΅© σ΅©2 2 σ΅©σ΅©Vπ − πσ΅©σ΅©σ΅© ≤ σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© − 2π2 (πΌ2 − π π2 ) σ΅©σ΅©σ΅©π΅2 π₯π − π΅2 πσ΅©σ΅©σ΅© σ΅© σ΅©2 − 2π1 (πΌ1 − π 2 π1 ) σ΅©σ΅©σ΅©π΅1 π’π − π΅1 πσ΅©σ΅©σ΅© . (39) (43) According to Lemma 3, we have from (27) σ΅©σ΅© σ΅©2 σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© σ΅© = σ΅©σ΅©σ΅©πΌπ (π (π¦π ) − π (π)) + (1 − πΌπ ) (ππ Vπ − π) σ΅©2 + πΌπ (π (π) − π) σ΅©σ΅©σ΅© σ΅© σ΅©2 ≤ σ΅©σ΅©σ΅©πΌπ (π (π¦π ) − π (π)) + (1 − πΌπ ) (ππ Vπ − π)σ΅©σ΅©σ΅© + 2πΌπ β¨π (π) − π, π½ (π¦π − π)β© (44) σ΅© σ΅©2 σ΅© σ΅©2 ≤ πΌπ σ΅©σ΅©σ΅©π (π¦π ) − π (π)σ΅©σ΅©σ΅© + (1 − πΌπ ) σ΅©σ΅©σ΅©ππ Vπ − πσ΅©σ΅©σ΅© + 2πΌπ β¨π (π) − π, π½ (π¦π − π)β© σ΅© σ΅©2 σ΅© σ΅©2 ≤ πΌπ πσ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© + (1 − πΌπ ) σ΅©σ΅©σ΅©Vπ − πσ΅©σ΅©σ΅© σ΅©σ΅© σ΅© σ΅© + 2πΌπ σ΅©σ΅©σ΅©π (π) − πσ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© , which hence yields σ΅©σ΅© σ΅©2 σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© ≤ (1 − In terms of condition (ii) and Lemma 4, we get lim σ΅©π§ π→∞ σ΅© π (40) Next we show that β π₯π − πΊ(π₯π ) β → 0 as π → ∞. For simplicity, put π = ΠπΆ(π − π2 π΅2 π), π’π = ΠπΆ(π₯π − π2 π΅2 π₯π ), and Vπ = ΠπΆ(π’π − π1 π΅1 π’π ). Then Vπ = πΊ(π₯π ). From Lemma 10, we have + σ΅© σ΅© σ΅© σ΅© lim sup (σ΅©σ΅©σ΅©π§π − π§π−1 σ΅©σ΅©σ΅© − σ΅©σ΅©σ΅©π₯π − π₯π−1 σ΅©σ΅©σ΅©) ≤ 0. σ΅© σ΅© σ΅© − π₯π σ΅©σ΅©σ΅© = lim (1 − π½π ) σ΅©σ΅©σ΅©π§π − π₯π σ΅©σ΅©σ΅© = 0. π→∞ + 1−π σ΅© σ΅©2 πΌ ) σ΅©σ΅©V − πσ΅©σ΅©σ΅© 1 − πΌπ π π σ΅© π 2πΌπ σ΅©σ΅© σ΅©σ΅© σ΅© σ΅©π (π) − πσ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© . 1 − πΌπ π σ΅© (45) Journal of Applied Mathematics 7 σ΅©2 σ΅© σ΅©2 σ΅© ≤ σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© − σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© + πΌπ π1 This together with (43) and the convexity of β ⋅ β2 , we have σ΅© σ΅© σ΅© σ΅© σ΅© σ΅© ≤ (σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅©) σ΅©σ΅©σ΅©π₯π − π₯π+1 σ΅©σ΅©σ΅© + πΌπ π1 . σ΅©σ΅© σ΅©2 σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© σ΅© σ΅©2 = σ΅©σ΅©σ΅©π½π (π₯π − π) + πΎπ (π¦π − π) + πΏπ (ππ πΊ (π¦π ) − π)σ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅©2 σ΅©2 σ΅©2 ≤ π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + πΎπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© + πΏπ σ΅©σ΅©σ΅©ππ πΊ (π¦π ) − πσ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅©2 σ΅©2 σ΅©2 ≤ π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + πΎπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© + πΏπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© σ΅© σ΅©2 σ΅© σ΅©2 = π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + (1 − π½π ) σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© σ΅© σ΅©2 ≤ π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + (1 − π½π ) × {(1 − + (47) Since 0 < ππ < πΌπ /π 2 for π = 1, 2, from conditions (i), (ii), and (40), we obtain σ΅© σ΅© σ΅© σ΅© lim σ΅©σ΅©π΅ π’ − π΅1 πσ΅©σ΅©σ΅© = 0. lim σ΅©σ΅©π΅ π₯ − π΅2 πσ΅©σ΅©σ΅© = 0, π→∞ σ΅© 2 π π→∞ σ΅© 1 π (48) Utilizing [14, Proposition 1] and Lemma 5, we have σ΅©σ΅© σ΅©2 σ΅©σ΅©π’π − πσ΅©σ΅©σ΅© σ΅© σ΅©2 = σ΅©σ΅©σ΅©ΠπΆ (π₯π − π2 π΅2 π₯π ) − ΠπΆ (π − π2 π΅2 π)σ΅©σ΅©σ΅© 1−π σ΅© σ΅©2 πΌπ ) σ΅©σ΅©σ΅©Vπ − πσ΅©σ΅©σ΅© 1 − πΌπ π ≤ β¨π₯π − π2 π΅2 π₯π − (π − π2 π΅2 π) , π½ (π’π − π)β© 2πΌπ σ΅©σ΅© σ΅©σ΅© σ΅© σ΅©π (π) − πσ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅©} 1 − πΌπ π σ΅© = β¨π₯π − π, π½ (π’π − π)β© + π2 β¨π΅2 π − π΅2 π₯π , π½ (π’π − π)β© σ΅© σ΅©2 ≤ π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + (1 − π½π ) × (1 − ≤ 1−π σ΅© σ΅©2 πΌ ) σ΅©σ΅©V − πσ΅©σ΅©σ΅© + πΌπ π1 1 − πΌπ π π σ΅© π 1−π σ΅© σ΅©2 ≤ π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + (1 − π½π ) (1 − πΌ) 1 − πΌπ π π (46) σ΅© σ΅©2 σ΅© σ΅©2 × [σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© − 2π2 (πΌ2 − π 2 π2 ) σ΅©σ΅©σ΅©π΅2 π₯π − π΅2 πσ΅©σ΅©σ΅© σ΅© σ΅©2 − 2π1 (πΌ1 − π 2 π1 ) σ΅©σ΅©σ΅©π΅1 π’π − π΅1 πσ΅©σ΅©σ΅© ] + πΌπ π1 = (1 − (1 − π½π ) (1 − π) σ΅© σ΅©2 πΌπ ) σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© − 2 (1 − π½π ) 1 − πΌπ π × (1 − 1−π πΌ) 1 − πΌπ π π σ΅© σ΅©2 × [π2 (πΌ2 − π π2 ) σ΅©σ΅©σ΅©π΅2 π₯π − π΅2 πσ΅©σ΅©σ΅© 2 σ΅© σ΅©2 + π1 (πΌ1 − π 2 π1 ) σ΅©σ΅©σ΅©π΅1 π’π − π΅1 πσ΅©σ΅©σ΅© ] + πΌπ π1 1−π σ΅© σ΅©2 ≤ σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© − 2 (1 − π½π ) (1 − πΌ) 1 − πΌπ π π σ΅© σ΅©2 × [π2 (πΌ2 − π 2 π2 ) σ΅©σ΅©σ΅©π΅2 π₯π − π΅2 πσ΅©σ΅©σ΅© σ΅© σ΅©2 + π1 (πΌ1 − π 2 π1 ) σ΅©σ΅©σ΅©π΅1 π’π − π΅1 πσ΅©σ΅©σ΅© ] + πΌπ π1 , where supπ≥0 {2(1−π½π )/(1−πΌπ π) β π(π)−π ββ π¦π −π β} ≤ π1 for some π1 > 0. So, it follows that 2 (1 − π½π ) (1 − 1−π πΌ) 1 − πΌπ π π σ΅© σ΅©2 × [π2 (πΌ2 − π 2 π2 ) σ΅©σ΅©σ΅©π΅2 π₯π − π΅2 πσ΅©σ΅©σ΅© σ΅© σ΅©2 + π1 (πΌ1 − π 2 π1 ) σ΅©σ΅©σ΅©π΅1 uπ − π΅1 πσ΅©σ΅©σ΅© ] 1 σ΅©σ΅© σ΅©2 σ΅© σ΅©2 σ΅© σ΅© [σ΅©π₯ − πσ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©π’π − πσ΅©σ΅©σ΅© −π1 (σ΅©σ΅©σ΅©π₯π − π’π − (π − π)σ΅©σ΅©σ΅©) ] 2 σ΅© π σ΅© σ΅©σ΅© σ΅© + π2 σ΅©σ΅©σ΅©π΅2 π − π΅2 π₯π σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π’π − πσ΅©σ΅©σ΅© , (49) which implies that σ΅©σ΅©σ΅©π’π − πσ΅©σ΅©σ΅©2 ≤ σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅©2 − π1 (σ΅©σ΅©σ΅©π₯π − π’π − (π − π)σ΅©σ΅©σ΅©) σ΅© σ΅© σ΅© σ΅© σ΅© σ΅© σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© + 2π2 σ΅©σ΅©π΅2 π − π΅2 π₯π σ΅©σ΅© σ΅©σ΅©π’π − πσ΅©σ΅© . In the same way, we derive σ΅©σ΅© σ΅©2 σ΅©σ΅©Vπ − πσ΅©σ΅©σ΅© σ΅© σ΅©2 = σ΅©σ΅©σ΅©ΠπΆ (π’π − π1 π΅1 π’π ) − ΠπΆ (π − π1 π΅1 π)σ΅©σ΅©σ΅© (50) ≤ β¨π’π − π1 π΅1 π’π − (π − π1 π΅1 π) , π½ (Vπ − π)β© = β¨π’π − π, π½ (Vπ − π)β© + π1 β¨π΅1 π − π΅1 π’π , π½ (Vπ − π)β© (51) 1 σ΅© σ΅©2 σ΅© σ΅©2 ≤ [σ΅©σ΅©σ΅©π’π − πσ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©Vπ − πσ΅©σ΅©σ΅© 2 σ΅© σ΅© − π2 (σ΅©σ΅©σ΅©π’π − Vπ + (π − π)σ΅©σ΅©σ΅©) ] σ΅© σ΅©σ΅© σ΅© + π1 σ΅©σ΅©σ΅©π΅1 π − π΅1 π’π σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©Vπ − πσ΅©σ΅©σ΅© , which implies that σ΅©σ΅© σ΅©2 σ΅© σ΅©2 σ΅© σ΅© σ΅©σ΅©Vπ − πσ΅©σ΅©σ΅© ≤ σ΅©σ΅©σ΅©π’π − πσ΅©σ΅©σ΅© − π2 (σ΅©σ΅©σ΅©π’π − Vπ + (π − π)σ΅©σ΅©σ΅©) (52) σ΅© σ΅©σ΅© σ΅© + 2π1 σ΅©σ΅©σ΅©π΅1 π − π΅1 π’π σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©Vπ − πσ΅©σ΅©σ΅© . Substituting (50) into (52), we get σ΅©σ΅© σ΅©2 σ΅© σ΅©2 σ΅© σ΅© σ΅©σ΅©Vπ − πσ΅©σ΅©σ΅© ≤ σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© − π1 (σ΅©σ΅©σ΅©π₯π − π’π − (π − π)σ΅©σ΅©σ΅©) σ΅© σ΅© − π2 (σ΅©σ΅©σ΅©π’π − Vπ + (π − π)σ΅©σ΅©σ΅©) (53) σ΅© σ΅©σ΅© σ΅© + 2π2 σ΅©σ΅©σ΅©π΅2 π − π΅2 π₯π σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π’π − πσ΅©σ΅©σ΅© σ΅© σ΅©σ΅© σ΅© + 2π1 σ΅©σ΅©σ΅©π΅1 π − π΅1 π’π σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©Vπ − πσ΅©σ΅©σ΅© . 8 Journal of Applied Mathematics From (46) and (53), we have Utilizing conditions (i), (ii), from (40) and (48), we have σ΅© σ΅©2 σ΅©2 σ΅©σ΅© σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© ≤ πΌπ π1 + π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© lim π π→∞ 1 σ΅© σ΅© lim π2 (σ΅©σ΅©σ΅©π’π − Vπ + (π − π)σ΅©σ΅©σ΅©) = 0. 1−π + (1 − π½π ) (1 − πΌ) 1 − πΌπ π π Utilizing the properties of π1 and π2 , we deduce that σ΅© − π’π − (π − π)σ΅©σ΅©σ΅© = 0, σ΅©σ΅© σ΅© − Vπ + (π − π)σ΅©σ΅©σ΅© = 0. lim σ΅©π’ π→∞ σ΅© π (1 − π½π ) (1 − π) σ΅© σ΅©2 πΌπ ) σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© 1 − πΌπ π 1−π πΌ) 1 − πΌπ π π σ΅© σ΅© × [π1 (σ΅©σ΅©σ΅©π₯π − π’π − (π − π)σ΅©σ΅©σ΅©) σ΅© σ΅© + π2 (σ΅©σ΅©σ΅©π’π − Vπ + (π − π)σ΅©σ΅©σ΅©)] σ΅© σ΅©σ΅© σ΅© + 2π2 σ΅©σ΅©σ΅©π΅2 π − π΅2 π₯π σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π’π − πσ΅©σ΅©σ΅© σ΅© σ΅©σ΅© σ΅© + 2π1 σ΅©σ΅©σ΅©π΅1 π − π΅1 π’π σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©Vπ − πσ΅©σ΅©σ΅© σ΅© σ΅©2 ≤ πΌπ π1 + σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© − (1 − π½π ) − (1 − π½π ) (1 − (57) From (57), we obtain σ΅©σ΅© σ΅© σ΅© σ΅© σ΅©σ΅©π₯π − Vπ σ΅©σ΅©σ΅© ≤ σ΅©σ΅©σ΅©π₯π − π’π − (π − π)σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©π’π − Vπ + (π − π)σ΅©σ΅©σ΅© σ³¨→ 0 as π → ∞. (58) That is, σ΅©σ΅© lim σ΅©π₯ π→∞ σ΅© π σ΅© − πΊ (π₯π )σ΅©σ΅©σ΅© = 0. (59) On the other hand, since {π¦π } and {ππ πΊ(π¦π )} are bounded, by Lemma 6, there exists a continuous strictly increasing function π3 : [0, ∞) → [0, ∞), π3 (0) = 0 such that for π ∈ πΉ σ΅©σ΅© σ΅©2 σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© σ΅© σ΅©2 = σ΅©σ΅©σ΅©π½π (π₯π − π) + πΎπ (π¦π − π) + πΏπ (ππ πΊ (π¦π ) − π)σ΅©σ΅©σ΅© σ΅©σ΅©σ΅© πΎπ = σ΅©σ΅©σ΅©(πΎπ + πΏπ ) [ (π¦ − π) σ΅©σ΅© πΎπ + πΏπ π × (1 − + (54) which implies that 1−π πΌ) 1 − πΌπ π π σ΅© σ΅© × [π1 (σ΅©σ΅©σ΅©π₯π − π’π − (π − π)σ΅©σ΅©σ΅©) σ΅©σ΅© lim σ΅©π₯ π→∞ σ΅© π σ΅© σ΅© − π2 (σ΅©σ΅©σ΅©π’π − Vπ + (π − π)σ΅©σ΅©σ΅©) σ΅© σ΅©σ΅© σ΅© + 2π2 σ΅©σ΅©σ΅©π΅2 π − π΅2 π₯π σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π’π − πσ΅©σ΅©σ΅© σ΅© σ΅©σ΅© σ΅© + 2π1 σ΅©σ΅©σ΅©π΅1 π − π΅1 π’π σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©Vπ − πσ΅©σ΅©σ΅© ] 1−π πΌ) 1 − πΌπ π π σ΅© σ΅© × [π1 (σ΅©σ΅©σ΅©π₯π − π’π − (π − π)σ΅©σ΅©σ΅©) σ΅© σ΅© + π2 (σ΅©σ΅©σ΅©π’π − Vπ + (π − π)σ΅©σ΅©σ΅©)] σ΅© σ΅©σ΅© σ΅© + 2π2 σ΅©σ΅©σ΅©π΅2 π − π΅2 π₯π σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π’π − πσ΅©σ΅©σ΅© σ΅© σ΅©σ΅© σ΅© + 2π1 σ΅©σ΅©σ΅©π΅1 π − π΅1 π’π σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©Vπ − πσ΅©σ΅©σ΅© , (56) π→∞ σ΅© σ΅©2 σ΅© σ΅© × [σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© − π1 (σ΅©σ΅©σ΅©π₯π − π’π − (π − π)σ΅©σ΅©σ΅©) ≤ πΌπ π1 + (1 − σ΅© σ΅© (σ΅©σ΅©σ΅©π₯π − π’π − (π − π)σ΅©σ΅©σ΅©) = 0, σ΅©σ΅© πΎ σ΅©σ΅©2 πΏπ σ΅© σ΅© π ≤ (πΎπ + πΏπ ) σ΅©σ΅©σ΅© (π¦π − π) + (ππ πΊ (π¦π ) − π)σ΅©σ΅©σ΅© σ΅©σ΅© πΎπ + πΏπ σ΅©σ΅© πΎπ + πΏπ σ΅© σ΅©2 + π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© ≤ (πΎπ + πΏπ ) [ (1 − π½π ) (1 − σ΅© σ΅© + π2 (σ΅©σ΅©σ΅©π’π − Vπ + (π − π)σ΅©σ΅©σ΅©)] σ΅© σ΅©2 σ΅© σ΅©2 ≤ πΌπ π1 + σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© − σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© (55) σ΅© σ΅©σ΅© σ΅© + 2π2 σ΅©σ΅©σ΅©π΅2 π − π΅2 π₯π σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π’π − πσ΅©σ΅©σ΅© σ΅© σ΅©σ΅© σ΅© + 2π1 σ΅©σ΅©σ΅©π΅1 π − π΅1 π’π σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©Vπ − πσ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© σ΅© σ΅© ≤ πΌπ π1 + (σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅©) σ΅©σ΅©σ΅©π₯π − π₯π+1 σ΅©σ΅©σ΅© σ΅© σ΅©σ΅© σ΅© + 2π2 σ΅©σ΅©σ΅©π΅2 π − π΅2 π₯π σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π’π − πσ΅©σ΅©σ΅© σ΅© σ΅©σ΅© σ΅© + 2π1 σ΅©σ΅©σ΅©π΅1 π − π΅1 π’π σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©Vπ − πσ΅©σ΅©σ΅© . σ΅©σ΅©2 πΏπ σ΅© (ππ πΊ (π¦π ) − π)] + π½π (π₯π − π) σ΅©σ΅©σ΅© σ΅©σ΅© πΎπ + πΏπ πΎπ σ΅©σ΅© πΏπ σ΅©σ΅© σ΅©2 σ΅©2 σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© + σ΅©π πΊ(π¦π ) − πσ΅©σ΅©σ΅© πΎπ + πΏπ πΎπ + πΏπ σ΅© π − πΎπ πΏπ 2 (πΎπ + πΏπ ) σ΅© σ΅© π3 (σ΅©σ΅©σ΅©π¦π − ππ πΊ (π¦π )σ΅©σ΅©σ΅©)] σ΅© σ΅©2 + π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© σ΅© σ΅© σ΅©2 σ΅©2 ≤ πΎπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© + πΏπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© − πΎπ πΏπ σ΅© σ΅© σ΅© σ΅©2 π (σ΅©σ΅©π¦ − ππ πΊ (π¦π )σ΅©σ΅©σ΅©) + π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© πΎπ + πΏπ 3 σ΅© π πΎπΏ σ΅© σ΅©2 = (1 − π½π ) σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© − π π πΎπ + πΏπ σ΅© σ΅© σ΅© σ΅©2 × π3 (σ΅©σ΅©σ΅©π¦π − ππ πΊ (π¦π )σ΅©σ΅©σ΅©) + π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© , (60) Journal of Applied Mathematics 9 which together with (30) implies that So, σ΅© σ΅© (1 − π½π ) σ΅©σ΅©σ΅©π₯π − π¦π σ΅©σ΅©σ΅© σ΅©σ΅© σ΅©2 σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© σ΅© σ΅© ≤ (1 − π½π ) (σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + − σ΅© σ΅© = σ΅©σ΅©σ΅©πΏπ (ππ πΊ (π¦π ) − π¦π ) − (π₯π+1 − π₯π )σ΅©σ΅©σ΅© 2 πΌπ σ΅©σ΅© σ΅© σ΅©π (π) − πσ΅©σ΅©σ΅©) 1 − πΌπ π σ΅© σ΅© σ΅© σ΅© σ΅© ≤ πΏπ σ΅©σ΅©σ΅©ππ πΊ (π¦π ) − π¦π σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©π₯π+1 − π₯π σ΅©σ΅©σ΅© πΌπ σ΅©σ΅© σ΅© σ΅©π (π) − πσ΅©σ΅©σ΅©) 1 − πΌπ π σ΅© That is, σ΅©σ΅© lim σ΅©π₯ π→∞ σ΅© π σ΅© σ΅© πΎπ πΏπ π3 (σ΅©σ΅©σ΅©π¦π − ππ πΊ (π¦π )σ΅©σ΅©σ΅©) πΎπ πΏπ σ΅© σ΅© π (σ΅©σ΅©π¦ − ππ πΊ (π¦π )σ΅©σ΅©σ΅©) πΎπ + πΏπ 3 σ΅© π σ΅© σ΅© ≤ (σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + 2 πΌπ σ΅©σ΅© σ΅© σ΅©σ΅©π (π) − πσ΅©σ΅©σ΅©) 1 − πΌπ π σ΅© σ΅©2 − σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© (62) σ΅© σ΅© σ΅© σ΅© ≤ ( σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© πΌπ σ΅©σ΅© σ΅© σ΅©σ΅©π (π) − πσ΅©σ΅©σ΅©) . 1 − πΌπ π lim inf πΏπ = lim inf (1 − π½π − πΎπ ) π→∞ = 1 − lim sup (π½π + πΎπ ) > 0. (63) π→∞ Since πΌπ → 0, β π₯π+1 − π₯π β → 0, and lim inf π → ∞ πΎπ > 0, we conclude that σ΅© σ΅© lim π (σ΅©σ΅©π¦ − ππ πΊ (π¦π )σ΅©σ΅©σ΅©) = 0. π→∞ 3 σ΅© π (64) Utilizing the property of π3 , we have σ΅©σ΅© lim σ΅©π¦ π→∞ σ΅© π σ΅© − ππ πΊ (π¦π )σ΅©σ΅©σ΅© = 0. Thus, from (59)–(68), we obtain that σ΅© σ΅© lim σ΅©σ΅©πΊ (π₯π ) − ππ πΊ (π₯π )σ΅©σ΅©σ΅© = 0. π→∞ σ΅© σ΅©σ΅© σ΅© σ΅©σ΅©ππΊ (π₯π ) − πΊ (π₯π )σ΅©σ΅©σ΅© σ΅© σ΅© ≤ σ΅©σ΅©σ΅©ππΊ (π₯π ) − ππ πΊ (π₯π )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ G (π₯π ) − πΊ (π₯π )σ΅©σ΅©σ΅© σ³¨→ 0 as π σ³¨→ ∞. According to condition (ii), we get π→∞ (68) (70) By (70) and Lemma 7, we have πΌπ σ΅©σ΅© σ΅© σ΅©π (π) − πσ΅©σ΅©σ΅©) 1 − πΌπ π σ΅© σ΅© σ΅© × (σ΅©σ΅©σ΅©π₯π − π₯π+1 σ΅©σ΅©σ΅© + σ΅© − π¦π σ΅©σ΅©σ΅© = 0. We observe that σ΅©σ΅© σ΅© σ΅©σ΅©πΊ (π₯π ) − ππ πΊ (π₯π )σ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© σ΅© σ΅© ≤ σ΅©σ΅©σ΅©πΊ (π₯π ) − π₯π σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©π₯π − π¦π σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©π¦π − ππ πΊ (π¦π )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π¦π ) − ππ πΊ (π₯π )σ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© σ΅© σ΅© ≤ σ΅©σ΅©σ΅©πΊ (π₯π ) − π₯π σ΅©σ΅©σ΅© + 2 σ΅©σ΅©σ΅©π₯π − π¦π σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©π¦π − ππ πΊ (π¦π )σ΅©σ΅©σ΅© . (69) It immediately follows that + σ΅© σ΅© + σ΅©σ΅©σ΅©π₯π+1 − π₯π σ΅©σ΅©σ΅© σ³¨→ 0 as π σ³¨→ ∞. 2 πΎπΏ σ΅© σ΅© − π π π3 (σ΅©σ΅©σ΅©π¦π − ππ πΊ (π¦π )σ΅©σ΅©σ΅©) . πΎπ + πΏπ ≤ σ΅© σ΅© ≤ σ΅©σ΅©σ΅©ππ πΊ (π¦π ) − π¦π σ΅©σ΅©σ΅© πΎπ πΏπ σ΅© σ΅© σ΅© σ΅©2 π (σ΅©σ΅©π¦ − ππ πΊ (π¦π )σ΅©σ΅©σ΅©) + π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© (61) πΎπ + πΏπ 3 σ΅© π σ΅© σ΅© ≤ (σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + (67) (65) We note that π₯π+1 − π₯π + π₯π − π¦π = π₯π+1 − π¦π = π½π (π₯π − π¦π ) + πΏπ (ππ πΊ (π¦π ) − π¦π ) . (66) (71) In terms of (59) and (71), we have σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© σ΅© σ΅©σ΅©π₯π − ππ₯π σ΅©σ΅©σ΅© ≤ σ΅©σ΅©σ΅©π₯π − πΊ (π₯π )σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©πΊ (π₯π ) − ππΊ (π₯π )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππΊ (π₯π ) − ππ₯π σ΅©σ΅©σ΅© σ΅© σ΅© ≤ 2 σ΅©σ΅©σ΅©π₯π − πΊ (π₯π )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©πΊ (π₯π ) − ππΊ (π₯π )σ΅©σ΅©σ΅© σ³¨→ 0 as π σ³¨→ ∞. (72) Define a mapping ππ₯ = (1 − π)ππ₯ + ππΊ(π₯), where π ∈ (0, 1) is a constant. Then by Lemma 9, we have that Fix(π) = Fix(π)∩ Fix(πΊ) = πΉ. We observe that σ΅©σ΅© σ΅© σ΅© σ΅© σ΅©σ΅©π₯π − ππ₯π σ΅©σ΅©σ΅© = σ΅©σ΅©σ΅©(1 − π) (π₯π − ππ₯π ) + π (π₯π − πΊ (π₯π ))σ΅©σ΅©σ΅© (73) σ΅© σ΅© σ΅© σ΅© ≤ (1 − π) σ΅©σ΅©σ΅©π₯π − ππ₯π σ΅©σ΅©σ΅© + π σ΅©σ΅©σ΅©π₯π − πΊ (π₯π )σ΅©σ΅©σ΅© . From (59) and (72), we obtain σ΅© σ΅© lim σ΅©σ΅©π₯ − ππ₯π σ΅©σ΅©σ΅© = 0. π→∞ σ΅© π (74) Now, we claim that lim sup β¨π (π) − π, π½ (π₯π − π)β© ≤ 0, π→∞ (75) 10 Journal of Applied Mathematics where π = π − limπ‘ → 0 π₯π‘ with π₯π‘ being the fixed point of the contraction π₯ σ³¨σ³¨→ π‘π (π₯) + (1 − π‘) ππ₯. (76) Then π₯π‘ solves the fixed point equation π₯π‘ = π‘π(π₯π‘ ) + (1 − π‘)ππ₯π‘ . Thus we have σ΅©σ΅© σ΅© σ΅© σ΅© σ΅©σ΅©π₯π‘ − π₯π σ΅©σ΅©σ΅© = σ΅©σ΅©σ΅©(1 − π‘) (ππ₯π‘ − π₯π ) + π‘ (π (π₯π‘ ) − π₯π )σ΅©σ΅©σ΅© . (77) On the other hand, we have β¨π (π) − π, π½ (π₯π − π)β© = β¨π (π) − π, π½ (π₯π − π)β© − β¨π (π) − π, π½ (π₯π − π₯π‘ )β© + β¨π (π) − π, π½ (π₯π − π₯π‘ )β© − β¨π (π) − π₯π‘ , π½ (π₯π − π₯π‘ )β© + β¨π (π) − π₯π‘ , π½ (π₯π − π₯π‘ )β© − β¨π (π₯π‘ ) − π₯π‘ , π½ (π₯π − π₯π‘ )β© + β¨π (π₯π‘ ) − π₯π‘ , π½ (π₯π − π₯π‘ )β© By Lemma 3, we conclude that = β¨π (π) − π, π½ (π₯π − π) − π½ (π₯π − π₯π‘ )β© σ΅©σ΅© σ΅©2 σ΅©σ΅©π₯π‘ − π₯π σ΅©σ΅©σ΅© σ΅© σ΅©2 = σ΅©σ΅©σ΅©(1 − π‘)(ππ₯π‘ − π₯π ) + π‘(π(π₯π‘ ) − π₯π )σ΅©σ΅©σ΅© σ΅© σ΅©2 ≤ (1 − π‘)2 σ΅©σ΅©σ΅©ππ₯π‘ − π₯π σ΅©σ΅©σ΅© + β¨π₯π‘ − π, π½ (π₯π − π₯π‘ )β© + β¨π (π) − π (π₯π‘ ) , π½ (π₯π − π₯π‘ )β© + β¨π (π₯π‘ ) − π₯π‘ , π½ (π₯π − π₯π‘ )β© . (83) It follows that + 2π‘ β¨π (π₯π‘ ) − π₯π , π½ (π₯π‘ − π₯π )β© σ΅© σ΅© σ΅©2 σ΅© ≤ (1 − π‘)2 (σ΅©σ΅©σ΅©ππ₯π‘ − ππ₯π σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©ππ₯π − π₯π σ΅©σ΅©σ΅©) lim sup β¨π (π) − π, π½ (π₯π − π)β© π→∞ + 2π‘ β¨π (π₯π‘ ) − π₯π , π½ (π₯π‘ − π₯π )β© ≤ lim sup β¨π (π) − π, π½ (π₯π − π) − π½ (π₯π − π₯π‘ )β© π→∞ σ΅© σ΅© σ΅© σ΅© ≤ (1 − π‘) (σ΅©σ΅©σ΅©π₯π‘ − π₯π σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©ππ₯π − π₯π σ΅©σ΅©σ΅©) 2 2 σ΅© σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©π₯π‘ − πσ΅©σ΅©σ΅© lim sup σ΅©σ΅©σ΅©π₯π − π₯π‘ σ΅©σ΅©σ΅© (78) + 2π‘ β¨π (π₯π‘ ) − π₯π , π½ (π₯π‘ − π₯π )β© π→∞ (84) σ΅© σ΅© σ΅© σ΅© + π σ΅©σ΅©σ΅©π − π₯π‘ σ΅©σ΅©σ΅© lim sup σ΅©σ΅©σ΅©π₯π − π₯π‘ σ΅©σ΅©σ΅© σ΅©2 σ΅© σ΅© σ΅© = (1 − π‘) [σ΅©σ΅©σ΅©π₯π‘ − π₯π σ΅©σ΅©σ΅© + 2 σ΅©σ΅©σ΅©π₯π‘ − π₯π σ΅©σ΅©σ΅© σ΅© σ΅© × σ΅©σ΅©σ΅©ππ₯π − π₯π σ΅©σ΅©σ΅© + β ππ₯π − π₯π β2 ] π→∞ 2 + lim sup β¨π (π₯π‘ ) − π₯π‘ , π½ (π₯π − π₯π‘ )β© . π→∞ Taking into account that π₯π‘ → π as π‘ → 0, we have from (82) + 2π‘ β¨π (π₯π‘ ) − π₯π‘ , π½ (π₯π‘ − π₯π )β© + 2π‘ β¨π₯π‘ − π₯π , π½ (π₯π‘ − π₯π )β© lim sup β¨π (π) − π, π½ (π₯π − π)β© σ΅©2 σ΅© = (1 − 2π‘ + π‘2 ) σ΅©σ΅©σ΅©π₯π‘ − π₯π σ΅©σ΅©σ΅© + ππ (π‘) π→∞ = lim sup lim sup β¨π (π) − π, π½ (π₯π − π)β© σ΅©2 σ΅© + 2π‘ β¨π (π₯π‘ ) − π₯π‘ , π½ (π₯π‘ − π₯π )β© + 2π‘σ΅©σ΅©σ΅©π₯π‘ − π₯π σ΅©σ΅©σ΅© , π‘→0 π→∞ ≤ lim sup lim sup β¨π (π) − π, π½ (π₯π − π) − π½ (π₯π − π₯π‘ )β© . where π‘→0 σ΅© σ΅© σ΅© σ΅© ππ (π‘) = (1 − π‘)2 (2 σ΅©σ΅©σ΅©π₯π‘ − π₯π σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©π₯π − ππ₯π σ΅©σ΅©σ΅©) σ΅© σ΅© × σ΅©σ΅©σ΅©π₯π − ππ₯π σ΅©σ΅©σ΅© σ³¨→ 0, as π σ³¨→ ∞. (85) (79) It follows from (78) that π‘σ΅© σ΅©2 1 β¨π₯π‘ − π (π₯π‘ ) , π½ (π₯π‘ − π₯π )β© ≤ σ΅©σ΅©σ΅©π₯π‘ − π₯π σ΅©σ΅©σ΅© + ππ (π‘) . (80) 2 2π‘ Letting π → ∞ in (80) and noticing (79), we derive π‘ lim sup β¨π₯π‘ − π (π₯π‘ ) , π½ (π₯π‘ − π₯π )β© ≤ π2 , 2 π→∞ Since π has a uniformly FreΜchet differentiable norm, the duality mapping π½ is norm-to-norm uniformly continuous on bounded subsets of π. Consequently, the two limits are interchangeable, and hence (75) holds. From (68), we get (π¦π − π) − (π₯π − π) → 0. Noticing that π½ is norm-to-norm uniformly continuous on bounded subsets of π, we deduce from (75) that lim sup β¨π (π) − π, π½ (π¦π − π)β© π→∞ (81) = lim sup (β¨π (π) − π, π½ (π₯π − π)β© π→∞ 2 where π2 > 0 is a constant such that β π₯π‘ − π₯π β ≤ π2 for all π‘ ∈ (0, 1) and π ≥ 0. Taking π‘ → 0 in (81), we have lim sup lim sup β¨π₯π‘ − π (π₯π‘ ) , π½ (π₯π‘ − π₯π )β© ≤ 0. π‘→0 π→∞ π→∞ (82) + β¨π (π) − π, π½ (π¦π − π) − π½ (π₯π − π)β©) = lim sup β¨π (π) − π, π½ (π₯π − π)β© ≤ 0. π→∞ (86) Journal of Applied Mathematics 11 Finally, let us show that π₯π → π as π → ∞. We observe that σ΅©2 σ΅©σ΅© σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© σ΅© = σ΅©σ΅©σ΅©πΌπ (π (π¦π ) − π (π)) + (1 − πΌπ ) σ΅©2 × (ππ πΊ (π₯π ) − π) + πΌπ (π (π) − π)σ΅©σ΅©σ΅© σ΅© ≤ σ΅©σ΅©σ΅©πΌπ (π (π¦π ) − π (π)) σ΅©2 + (1 − πΌπ ) (ππ πΊ (π₯π ) − π) σ΅©σ΅©σ΅© + 2πΌπ β¨π (π) − π, π½ (π¦π − π)β© (87) σ΅©2 σ΅© ≤ πΌπ σ΅©σ΅©σ΅©π (π¦π ) − π (π)σ΅©σ΅©σ΅© σ΅© σ΅©2 σ΅© σ΅©2 ≤ πΌπ πσ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© + (1 − πΌπ ) σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© (iii) limπ → ∞ |(πΎπ /(1 − π½π )) − (πΎπ−1 /(1 − π½π−1 ))| = 0. (88) By (27) and the convexity of β ⋅ β2 , we get σ΅©σ΅© σ΅©2 σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅©2 σ΅©2 σ΅©2 ≤ π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + πΎπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© + πΏπ σ΅©σ΅©σ΅©ππ πΊ (π¦π ) − πσ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅©2 σ΅©2 σ΅©2 ≤ π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + πΎπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© + πΏπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© σ΅© σ΅©2 σ΅© σ΅©2 = π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + (1 − π½π ) σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© , (89) which together with (88) leads to σ΅©σ΅© σ΅©2 σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© σ΅© σ΅©2 ≤ π½π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + (1 − π½π ) + = [1 − (91) (ii) 0 < lim inf π → ∞ π½π ≤ lim supπ → ∞ (π½π + πΎπ ) < 1 and lim inf π → ∞ πΎπ > 0, which implies that × { (1 − ∀π ≥ 0, (i) limπ → ∞ πΌπ = 0 and ∑∞ π=0 πΌπ = ∞, + 2πΌπ β¨π (π) − π, π½ (π¦π − π)β© , πΌπ (1 − π) 2 β¨π (π) − π, π½ (π¦π − π)β© ⋅ . 1 − πΌπ π 1−π π¦π = πΌπ π (π¦π ) + (1 − πΌπ ) ππΊ (π₯π ) , where 0 < ππ < πΌπ /π 2 for π = 1, 2 and {πΌπ }, {π½π }, {πΎπ }, and {πΏπ } are the sequences in (0, 1) such that π½π + πΎπ + πΏπ = 1, ∀π ≥ 0. Suppose that the following conditions hold: + 2πΌπ β¨π (π) − π, π½ (π¦π − π)β© + Corollary 15. Let πΆ be a nonempty, closed, and convex subset of a uniformly convex and 2-uniformly smooth Banach space π. Let ΠπΆ be a sunny nonexpansive retraction from π onto πΆ. Let the mapping π΅π : πΆ → π be πΌπ -inverse-strongly accretive for π = 1, 2. Let π : πΆ → πΆ be a contraction with coefficient π ∈ (0, 1). Let π be a nonexpansive mapping of πΆ into itself such that πΉ = Fix(π) ∩ Ω =ΜΈ 0, where Ω is the fixed point set of the mapping πΊ = ΠπΆ(πΌ − π1 π΅1 )ΠπΆ(πΌ − π2 π΅2 ). For arbitrarily given π₯0 ∈ πΆ, let {π₯π } be the sequence generated by π₯π+1 = π½π π₯π + πΎπ π¦π + πΏπ ππΊ (π¦π ) , σ΅© σ΅©2 + (1 − πΌπ ) σ΅©σ΅©σ΅©ππ πΊ (π₯π ) − πσ΅©σ΅©σ΅© 1−π σ΅©2 σ΅© σ΅©2 σ΅©σ΅© πΌ ) σ΅©σ΅©π₯ − πσ΅©σ΅©σ΅© σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© ≤ (1 − 1 − πΌπ π π σ΅© π Applying Lemma 2 to (88), we obtain that π₯π → π as π → ∞. This completes the proof. 1−π σ΅© σ΅©2 πΌ ) σ΅©σ΅©π₯ − πσ΅©σ΅©σ΅© 1 − πΌπ π π σ΅© π πΌπ (1 − π) 2 β¨π (π) − π, π½ (π¦π − π)β© ⋅ } 1 − πΌπ π 1−π (1 − π½π ) (1 − π) σ΅© σ΅©2 πΌπ ] σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© 1 − πΌπ π (1 − π½π ) (1 − π) 2 β¨π (π) − π, π½ (π¦π − π)β© + πΌπ ⋅ . 1 − πΌπ π 1−π (90) Then {π₯π } converges strongly to π ∈ πΉ, which solves the following VIP: β¨π − π (π) , π½ (π − π)β© ≤ 0, ∀π ∈ πΉ. (92) Further, we illustrate Theorem 14 by virtue of an example, that is, the following corollary. Corollary 16. Let πΆ be a nonempty, closed, and convex subset of a uniformly convex and 2-uniformly smooth Banach space π. Let ΠπΆ be a sunny nonexpansive retraction from π onto πΆ. Let π : πΆ → πΆ be a contraction with coefficient π ∈ (0, 1). Let π be an π-strictly pseudocontractive mapping of πΆ into itself, and let π be a nonexpansive mapping of πΆ into itself such that πΉ = Fix(π) ∩ Fix(π) =ΜΈ 0. For arbitrarily given π₯0 ∈ πΆ, let {π₯π } be the sequence generated by π¦π = πΌπ π (π¦π ) + (1 − πΌπ ) π (πΌ − π (I − π)) π₯π , π₯π+1 = π½π π₯π + πΎπ π¦π + πΏπ π (πΌ − π (πΌ − π)) π¦π , ∀π ≥ 0, (93) where 0 < π < max{1, π/π 2 } and {πΌπ }, {π½π }, {πΎπ }, and {πΏπ } are the sequences in (0, 1) such that π½π + πΎπ + πΏπ = 1, ∀π ≥ 0. Suppose that the following conditions hold: (i) limπ → ∞ πΌπ = 0 and ∑∞ π=0 πΌπ = ∞, (ii) 0 < lim inf π → ∞ π½π ≤ lim supπ → ∞ (π½π + πΎπ ) < 1 and lim inf π → ∞ πΎπ > 0, (iii) limπ → ∞ |(πΎπ /(1 − π½π )) − (πΎπ−1 /(1 − π½π−1 ))| = 0. Then {π₯π } converges strongly to π ∈ πΉ, which solves the following VIP: β¨π − π (π) , π½ (π − π)β© ≤ 0, ∀π ∈ πΉ. (94) 12 Journal of Applied Mathematics Proof. In Corollary 15, put π΅1 = πΌ − π, π΅2 = 0, π1 = π, and πΌ1 = π. Since π is an π-strictly pseudocontractive mapping, it is clear that π΅1 = πΌ − π is an π-inverse strongly accretive mapping. Hence, the GSVI (9) is equivalent to the following VIP of finding π₯∗ ∈ πΆ such that (π΅1 π₯∗ , π½ (π₯ − π₯∗ )) ≥ 0, ∀π₯ ∈ πΆ, (95) which leads to Ω = VI(πΆ, π΅1 ). In the meantime, we have πΊπ₯π = ΠπΆ (πΌ − π1 π΅1 ) ΠπΆ (πΌ − π2 π΅2 ) π₯π = ΠπΆ (πΌ − π1 π΅1 ) π₯π = ΠπΆ [(1 − π) π₯π + πππ₯π ] (96) = π₯π − π (πΌ − π) π₯π . In the same way, we get πΊπ¦π = π¦π − π(πΌ − π)π¦π . In this case, it is easy to see that (91) reduces to (93). We claim that Fix(π) = VI(πΆ, π΅1 ). As a matter of fact, we have, for π > 0, π’ ∈ VI (πΆ, π΅1 ) ⇐⇒ β¨π΅1 π’, π½ (π¦ − π’)β© ≥ 0 ∀π¦ ∈ πΆ iterative scheme of [2, Theorem 3.1] and the mapping πππΆ(πΌ − π π π΄) in the iterative scheme of [5, Theorem 3.1] are replaced by the same composite mapping ππ πΊ in the iterative scheme (27) of Theorem 14. (iv) The proof in [2, Theorem 3.1] depends on the argument techniques in [3], the inequality in 2-uniformly smooth Banach spaces ([9]), and the inequality in smooth and uniform convex Banach spaces ([14, Proposition 1]). Because the composite mapping ππ πΊ appears in the iterative scheme (27) of Theorem 14, the proof of Theorem 14 depends on the argument techniques in [3], the inequality in 2-uniformly smooth Banach spaces, the inequality in smooth and uniform convex Banach spaces, and the inequality in uniform convex Banach spaces (Lemma 6). (v) The iterative scheme in [2, Corollary 3.2] is extended to develop the new iterative scheme in Corollary 15 because the mappings π and πΊ are replaced by the same composite mapping ππΊ in Corollary 15. 4. Explicit Iterative Schemes ⇐⇒ β¨π’ − ππ΅1 π’ − π’, π½ (π’ − π¦)β© ≥ 0 ∀π¦ ∈ πΆ In this section, we introduce our explicit iterative schemes and show the strong convergence theorems. First, we give several useful lemmas. ⇐⇒ π’ = ΠπΆ (π’ − ππ΅1 π’) ⇐⇒ π’ = ΠπΆ (π’ − ππ’ + πππ’) ⇐⇒ β¨π’ − ππ’ + πππ’ − π’, π½ (π’ − π¦)β© ≥ 0 ∀π¦ ∈ πΆ ⇐⇒ β¨π’ − ππ’, π½ (π’ − π¦)β© ≤ 0 ∀π¦ ∈ πΆ ⇐⇒ π’ = ππ’ Lemma 18. Let πΆ be a nonempty, closed, and convex subset of a smooth Banach space π, and let the mapping π΅π : πΆ → π be π π -strictly pseudocontractive and πΌπ -strongly accretive with πΌπ + π π ≥ 1 for π = 1, 2. Then, for ππ ∈ (0, 1], we have σ΅©σ΅© σ΅© σ΅©σ΅©(πΌ − ππ π΅π ) π₯ − (πΌ − ππ π΅π ) π¦σ΅©σ΅©σ΅© ⇐⇒ π’ ∈ Fix (π) . (97) So, we conclude that πΉ = Fix(π) ∩ Ω = Fix(π) ∩ Fix(π). Therefore, the desired result follows from Corollary 15. Remark 17. Theorem 14 improves, extends, supplements, and develops Cai and Bu [2, Theorem 3.1 and Corollary 3.2] and Jung [5, Theorem 3.1] in the following aspects. (i) The problem of finding a point π ∈ βπ Fix(ππ ) ∩ Ω in Theorem 14 is more general and more subtle than the problem of finding a point π ∈ Fix(π) ∩ VI(πΆ, π΄) in Jung [5, Theorem 3.1]. (ii) The iterative scheme in [2, Theorem 3.1] is extended to develop the iterative scheme (27) of Theorem 14 by virtue of the iterative scheme of [5, Theorem 3.1]. The iterative scheme (27) of Theorem 14 is more advantageous and more flexible than the iterative scheme of [2, Theorem 3.1] because it involves several parameter sequences {πΌπ }, {π½π }, {πΎπ }, and {πΏπ }. (iii) The iterative scheme (27) in Theorem 14 is very different from everyone in both [2, Theorem 3.1] and [5, Theorem 3.1] because the mappings ππ and πΊ in the ≤ {√ 1 − πΌπ 1 σ΅© σ΅© + (1 − ππ ) (1 + )} σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅© , ππ ππ (98) ∀π₯, π¦ ∈ πΆ, for π = 1, 2. In particular, if 1−(π π /(1+π π ))(1−√(1 − πΌπ )/π π ) ≤ ππ ≤ 1, then πΌ − ππ π΅π is nonexpansive for π = 1, 2. Proof. Taking into account the π π -strict pseudocontractivity of π΅π , we derive for every π₯, π¦ ∈ πΆ σ΅© σ΅©2 π π σ΅©σ΅©σ΅©(πΌ − π΅π ) π₯ − (πΌ − π΅π ) π¦σ΅©σ΅©σ΅© ≤ β¨(πΌ − π΅π ) π₯ − (πΌ − π΅π ) π¦, π½ (π₯ − π¦)β© (99) σ΅© σ΅©σ΅© σ΅© ≤ σ΅©σ΅©σ΅©(πΌ − π΅π ) π₯ − (πΌ − π΅π ) π¦σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅© , which implies that σ΅©σ΅© σ΅© σ΅© 1 σ΅©σ΅© σ΅©σ΅©(πΌ − π΅π ) π₯ − (πΌ − π΅π ) π¦σ΅©σ΅©σ΅© ≤ σ΅©π₯ − π¦σ΅©σ΅©σ΅© . ππ σ΅© (100) Journal of Applied Mathematics 13 Proof. According to Lemma 10, we know that πΌ − ππ π΅π is nonexpansive for π = 1, 2. Hence, for all π₯, π¦ ∈ πΆ, we have Hence, σ΅©σ΅© σ΅© σ΅©σ΅©π΅π π₯ − π΅π π¦σ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© ≤ σ΅©σ΅©σ΅©(πΌ − π΅π ) π₯ − (πΌ − π΅π ) π¦σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅© (101) 1 σ΅© σ΅© ≤ (1 + ) σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅© . ππ σ΅© − ΠπΆ [ΠπΆ (π¦ − π2 π΅2 π¦) − π1 π΅1 ΠπΆ (π¦ − π2 π΅2 π¦)]σ΅©σ΅©σ΅© Utilizing the πΌπ -strong accretivity and π π -strict pseudocontractivity of π΅π , we get σ΅©2 σ΅© ≤ σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅© − β¨π΅π π₯ − π΅π π¦, π½ (π₯ − π¦)β© (102) σ΅© − ΠπΆ (πΌ − π1 π΅1 ) ΠπΆ (πΌ − π2 π΅2 ) π¦σ΅©σ΅©σ΅© σ΅© − (πΌ − π1 π΅1 ) ΠπΆ (πΌ − π2 π΅2 ) π¦σ΅©σ΅©σ΅© σ΅© σ΅© ≤ σ΅©σ΅©σ΅©ΠπΆ (πΌ − π2 π΅2 ) π₯ − ΠπΆ (πΌ − π2 π΅2 ) π¦σ΅©σ΅©σ΅© σ΅©2 σ΅© ≤ (1 − πΌπ ) σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅© . σ΅© σ΅© ≤ σ΅©σ΅©σ΅©(πΌ − π2 π΅2 ) π₯ − (πΌ − π2 π΅2 ) π¦σ΅©σ΅©σ΅© So, we have 1 − πΌπ σ΅©σ΅© σ΅© σ΅©σ΅© σ΅© σ΅©σ΅©(πΌ − π΅π ) π₯ − (πΌ − π΅π ) π¦σ΅©σ΅©σ΅© ≤ √ σ΅©π₯ − π¦σ΅©σ΅©σ΅© . π σ΅© σ΅© σ΅© ≤ σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅© . This shows that πΊ : πΆ → πΆ is nonexpansive. This completes the proof. Therefore, for ππ ∈ (0, 1], we have σ΅© σ΅©σ΅© σ΅©σ΅©(πΌ − ππ π΅π ) π₯ − (πΌ − ππ π΅π ) π¦σ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© ≤ σ΅©σ΅©σ΅©(πΌ − π΅π ) π₯ − (πΌ − π΅π ) π¦σ΅©σ΅©σ΅© + (1 − ππ ) σ΅©σ΅©σ΅©π΅π π₯ − π΅π π¦σ΅©σ΅©σ΅© 1 − πΌπ σ΅©σ΅© 1 σ΅© σ΅© σ΅© σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅© + (1 − ππ ) (1 + ) σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅© ππ ππ 1 − πΌπ 1 σ΅© σ΅© + (1 − ππ ) (1 + )} σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅© . ππ ππ Lemma 20. Let πΆ be a nonempty, closed, and convex subset of a smooth Banach space π. Let ΠπΆ be a sunny nonexpansive retraction from π onto πΆ, and let the mapping π΅π : πΆ → π be π π -strictly pseudocontractive and πΌπ -strongly accretive for π = 1, 2. For given π₯∗ , π¦∗ ∈ πΆ, (π₯∗ , π¦∗ ) is a solution of GSVI (9) if and only if π₯∗ = ΠπΆ(π¦∗ − π1 π΅1 π¦∗ ) where π¦∗ = ΠπΆ(π₯∗ − π2 π΅2 π₯∗ ). Proof. We can rewrite GSVI (9) as (104) Since 1 − (π π /(1 + π π ))(1 − √(1 − πΌi )/π π ) ≤ ππ ≤ 1, it follows immediately that 1 − πΌπ 1 √ + (1 − ππ ) (1 + ) ≤ 1. ππ ππ (107) (103) π = {√ σ΅© = σ΅©σ΅©σ΅©ΠπΆ (πΌ − π1 π΅1 ) ΠπΆ (πΌ − π2 π΅2 ) π₯ σ΅© ≤ σ΅©σ΅©σ΅©(πΌ − π1 π΅1 ) ΠπΆ (πΌ − π2 π΅2 ) π₯ σ΅© σ΅©2 π π σ΅©σ΅©σ΅©(πΌ − π΅π ) π₯ − (πΌ − π΅π ) π¦σ΅©σ΅©σ΅© ≤√ σ΅© σ΅©σ΅© σ΅©σ΅©πΊ (π₯) − πΊ (π¦)σ΅©σ΅©σ΅© σ΅© = σ΅©σ΅©σ΅©ΠπΆ [ΠπΆ (π₯ − π2 π΅2 π₯) − π1 π΅1 ΠπΆ (π₯ − π2 π΅2 π₯)] β¨π₯∗ − (π¦∗ − π1 π΅1 π¦∗ ) , π½ (π₯ − π₯∗ )β© ≥ 0, ∀π₯ ∈ πΆ, β¨π¦∗ − (π₯∗ − π2 π΅2 π₯∗ ) , π½ (π₯ − π¦∗ )β© ≥ 0, ∀π₯ ∈ πΆ, which is obviously equivalent to π₯∗ = ΠπΆ (π¦∗ − π1 π΅1 π¦∗ ) , (105) π¦∗ = ΠπΆ (π₯∗ − π2 π΅2 π₯∗ ) , This implies that πΌ − ππ π΅π is nonexpansive for π = 1, 2. because of Lemma 5. This completes the proof. Lemma 19. Let πΆ be a nonempty, closed, and convex subset of a smooth Banach space π. Let ΠπΆ be a sunny nonexpansive retraction from π onto πΆ, and let the mapping π΅π : πΆ → π be π π -strictly pseudocontractive and πΌπ -strongly accretive with πΌπ + π π ≥ 1 for π = 1, 2. Let πΊ : πΆ → πΆ be the mapping defined by Remark 21. By Lemma 20, we observe that πΊ (π₯) = ΠπΆ [ΠπΆ (π₯ − π2 π΅2 π₯) (108) (109) π₯∗ = ΠπΆ [ΠπΆ (π₯∗ − π2 π΅2 π₯∗ ) − π1 π΅1 ΠπΆ (π₯∗ − π2 π΅2 π₯∗ )] , (110) which implies that π₯∗ is a fixed point of the mapping πΊ. Throughout this paper, the set of fixed points of the mapping πΊ is denoted by Ω. (106) We are now in a position to state and prove our result on the explicit iterative scheme. If 1−(π π /(1+π π ))(1−√(1 − πΌπ )/π π ) ≤ ππ ≤ 1, then πΊ : πΆ → πΆ is nonexpansive. Theorem 22. Let πΆ be a nonempty, closed, and convex subset of a uniformly convex Banach space π which has a uniformly − π1 π΅1 ΠπΆ (π₯ − π2 π΅2 π₯)] , ∀π₯ ∈ πΆ. 14 Journal of Applied Mathematics GaΜteaux differentiable norm. Let ΠπΆ be a sunny nonexpansive retraction from π onto πΆ. Let the mapping π΅π : πΆ → π be π π strictly pseudocontractive and πΌπ -strongly accretive with πΌπ + π π ≥ 1 for π = 1, 2. Let π : πΆ → πΆ be a contraction with coefficient π ∈ (0, 1). Let {ππ }∞ π=0 be an infinite family of nonexpansive mappings of πΆ into itself such that πΉ = β∞ π=0 Fix(ππ ) ∩ Ω =ΜΈ 0, where Ω is the fixed point set of the mapping πΊ = ΠπΆ(πΌ − π1 π΅1 )ΠπΆ(πΌ − π2 π΅2 ). For arbitrarily given π₯0 ∈ πΆ, let {π₯π } be the sequence generated by π¦π = πΌπ πΊ (π₯π ) + (1 − πΌπ ) ππ πΊ (π₯π ) , π₯π+1 = π½π π (π₯π ) + πΎπ π¦π + πΏπ ππ πΊ (π¦π ) , ∀π ≥ 0, (111) where 1 − (π π /(1 + π π ))(1 − √(1 − πΌπ )/π π ) ≤ ππ ≤ 1 for π = 1, 2 and {πΌπ }, {π½π }, {πΎπ }, and {πΏπ } are the sequences in (0, 1) such that π½π + πΎπ + πΏπ = 1, ∀π ≥ 0. Suppose that the following conditions hold: (i) 0 < lim inf π → ∞ πΌπ ≤ lim supπ → ∞ πΌπ < 1, (ii) limπ → ∞ π½π = 0 and ∑∞ π=0 π½π = ∞, (iii) ∑∞ π=1 |πΌπ − πΌπ−1 | < ∞ or limπ → ∞ |πΌπ − πΌπ−1 |/π½π = 0, (iv) ∑∞ π=1 |π½π − π½π−1 | < ∞ or limπ → ∞ π½π−1 /π½π = 1, (v) ∑∞ π=1 |(πΎπ /(1 − π½π )) − (πΎπ−1 /(1 − π½π−1 ))| < ∞ or limπ → ∞ (1/π½π )|(πΎπ /(1 − π½π )) − (πΎπ−1 /(1 − π½π−1 ))| = 0, (vi) 0 < lim inf π → ∞ πΎπ ≤ lim supπ → ∞ πΎπ < 1. ∀π ∈ πΉ. (112) Proof. Take a fixed π ∈ πΉ arbitrarily. Then by Lemma 20, we know that π = πΊ(π) and π = ππ π for all π ≥ 0. Moreover, by Lemma 19, we have σ΅© σ΅©σ΅© σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© ≤ πΌπ σ΅©σ΅©σ΅©πΊ (π₯π ) − πσ΅©σ΅©σ΅© + (1 − πΌπ ) σ΅©σ΅©σ΅©ππ πΊ (π₯π ) − πσ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© ≤ πΌπ σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + (1 − πΌπ ) σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© σ΅© σ΅© = σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© . σ΅© σ΅©σ΅© σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© ≤ π½π σ΅©σ΅©σ΅©π (π₯π ) − πσ΅©σ΅©σ΅© + πΎπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© σ΅© σ΅© + πΏπ σ΅©σ΅©σ΅©ππ πΊ (π¦π ) − πσ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© ≤ π½π (σ΅©σ΅©σ΅©π (π₯π ) − π (π)σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©π (π) − πσ΅©σ΅©σ΅©) σ΅© σ΅© σ΅© σ΅© + πΎπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© + πΏπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© ≤ π½π π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + π½π σ΅©σ΅©σ΅©π (π) − πσ΅©σ΅©σ΅© σ΅© σ΅© + (1 − π½π ) σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© ≤ π½π π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + π½π σ΅©σ΅©σ΅©π (π) − πσ΅©σ΅©σ΅© σ΅© σ΅© + (1 − π½π ) σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© σ΅© σ΅© = (1 − π½π (1 − π)) σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© σ΅© σ΅© + π½π σ΅©σ΅©σ΅©π (π) − πσ΅©σ΅©σ΅© σ΅© σ΅© = (1 − π½π (1 − π)) σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© σ΅© σ΅©σ΅© σ΅©π (π) − πσ΅©σ΅©σ΅© + π½π (1 − π) ⋅ σ΅© 1−π σ΅© σ΅©σ΅© σ΅© σ΅©π (π) − πσ΅©σ΅©σ΅© σ΅© ≤ max {σ΅©σ΅©σ΅©π₯0 − πσ΅©σ΅©σ΅© , σ΅© }, 1−π (114) which implies that {π₯π } is bounded. By Lemma 19 we know from (113) that {π¦π }, {πΊ(π₯π )}, and {πΊ(π¦π )} are bounded. Let us show that β π₯π+1 − π₯π β → 0 and β π₯π − π¦π β → 0 as π → ∞. As a matter of fact, from (113), we have π¦π = πΌπ πΊ (π₯π ) + (1 − πΌπ ) ππ πΊ (π₯π ) , Assume that ∑∞ π=1 supπ₯∈π· β ππ π₯−ππ−1 π₯ β< ∞ for any bounded subset π· of πΆ, and let π be a mapping of πΆ into itself defined by ππ₯ = limπ → ∞ ππ π₯ for all π₯ ∈ πΆ. Suppose that Fix(π) = β∞ π=0 Fix(ππ ). Then {π₯π } converges strongly to π ∈ πΉ, which solves the following VIP: β¨π − π (π) , π½ (π − π)β© ≤ 0, From (113) we obtain (113) π¦π−1 = πΌπ−1 πΊ (π₯π−1 ) + (1 − πΌπ−1 ) ππ−1 πΊ (π₯π−1 ) , ∀π ≥ 1. (115) Simple calculations show that π¦π − π¦π−1 = πΌπ (πΊ (π₯π ) − πΊ (π₯π−1 )) + (πΌπ − πΌπ−1 ) (πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )) (116) + (1 − πΌπ ) (ππ πΊ (π₯n ) − ππ−1 πΊ (π₯π−1 )) . It follows that σ΅©σ΅© σ΅© σ΅©σ΅©π¦π − π¦π−1 σ΅©σ΅©σ΅© σ΅© σ΅© ≤ πΌπ σ΅©σ΅©σ΅©πΊ (π₯π ) − πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅¨ σ΅¨σ΅© σ΅© + σ΅¨σ΅¨σ΅¨πΌπ − πΌπ−1 σ΅¨σ΅¨σ΅¨ σ΅©σ΅©σ΅©πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + (1 − πΌπ ) σ΅©σ΅©σ΅©ππ πΊ (π₯π ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© Journal of Applied Mathematics 15 σ΅© σ΅© ≤ πΌπ σ΅©σ΅©σ΅©πΊ (π₯π ) − πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© ≤ (πΎπ σ΅©σ΅©σ΅©π¦π − π¦π−1 σ΅©σ΅©σ΅© σ΅¨ σ΅¨σ΅© σ΅© + σ΅¨σ΅¨σ΅¨πΌπ − πΌπ−1 σ΅¨σ΅¨σ΅¨ σ΅©σ΅©σ΅©πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + πΏπ ( σ΅©σ΅©σ΅©ππ πΊ (π¦π ) − ππ πΊ (π¦π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π¦π−1 ) − ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅©)) σ΅© σ΅© + (1 − πΌπ ) (σ΅©σ΅©σ΅©ππ πΊ (π₯π ) − ππ πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅©) σ΅© σ΅© ≤ πΌπ σ΅©σ΅©σ΅©πΊ (π₯π ) − πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅¨ σ΅¨σ΅© σ΅© + σ΅¨σ΅¨σ΅¨πΌπ − πΌπ−1 σ΅¨σ΅¨σ΅¨ σ΅©σ΅©σ΅©πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + (1 − πΌπ ) (σ΅©σ΅©σ΅©πΊ (π₯π ) − πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅©) σ΅© σ΅© ≤ σ΅©σ΅©σ΅©πΊ (π₯π ) − πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅¨ σ΅¨σ΅© σ΅© + σ΅¨σ΅¨σ΅¨πΌπ − πΌπ−1 σ΅¨σ΅¨σ΅¨ σ΅©σ΅©σ΅©πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© σ΅¨ σ΅¨ ≤ σ΅©σ΅©σ΅©π₯π − π₯π−1 σ΅©σ΅©σ΅© + σ΅¨σ΅¨σ΅¨πΌπ − πΌπ−1 σ΅¨σ΅¨σ΅¨ σ΅© σ΅© × σ΅©σ΅©σ΅©πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© . −1 × (1 − π½π ) σ΅¨σ΅¨ πΎ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σ΅¨ σ΅© + σ΅¨σ΅¨σ΅¨ π − σ΅¨ σ΅©π¦ σ΅©σ΅© σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨σ΅¨ σ΅© π−1 σ΅© σ΅¨σ΅¨ πΎ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σ΅¨ σ΅© + σ΅¨σ΅¨σ΅¨ π − σ΅¨σ΅¨ σ΅©σ΅©ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅© σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨ σ΅© σ΅© σ΅© σ΅© πΎπ σ΅©σ΅©σ΅©π¦π − π¦π−1 σ΅©σ΅©σ΅© + πΏπ σ΅©σ΅©σ΅©π¦π − π¦π−1 σ΅©σ΅©σ΅© ≤ πΎπ + πΏπ (117) Now, we write π₯π = π½π−1 π(π₯π−1 ) + (1 − π½π−1 )Vπ−1 , ∀π ≥ 1, where Vπ−1 = (π₯π − π½π−1 π(π₯π−1 ))/(1 − π½π−1 ). It follows that, for all π ≥ 1, Vπ − Vπ−1 = π₯π+1 − π½π π (π₯π ) π₯π − π½π−1 π (π₯π−1 ) − 1 − π½π 1 − π½π−1 = πΎπ−1 π¦π−1 + πΏπ−1 ππ−1 πΊ (π¦π−1 ) 1 − π½π−1 πΎπ (π¦π − π¦π−1 ) + πΏπ (ππ πΊ (π¦π ) − ππ−1 πΊ (π¦π−1 )) 1 − π½π +( πΎπ πΎπ−1 − )π¦ 1 − π½π 1 − π½π−1 π−1 πΏπ−1 πΏ +( π − ) π πΊ (π¦π−1 ) . 1 − π½π 1 − π½π−1 π−1 This together with (117) implies that σ΅©σ΅© σ΅© σ΅©σ΅©Vπ − Vπ−1 σ΅©σ΅©σ΅© σ΅©σ΅© σ΅© σ΅©πΎ (π¦ − π¦π−1 ) + πΏπ (ππ πΊ (π¦π ) − ππ−1 πΊ (π¦π−1 ))σ΅©σ΅©σ΅© ≤σ΅© π π 1 − π½π σ΅¨σ΅¨ πΎ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σ΅¨ σ΅© + σ΅¨σ΅¨σ΅¨ π − σ΅¨σ΅¨ σ΅©σ΅©π¦π−1 σ΅©σ΅©σ΅© σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨ σ΅¨σ΅¨σ΅¨ πΏ πΏπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σ΅© + σ΅¨σ΅¨σ΅¨ π − σ΅¨σ΅¨ σ΅©σ΅©ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅© σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨ σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π¦π−1 ) − ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅© σ΅¨σ΅¨ πΎ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σ΅¨ σ΅© σ΅© σ΅© + σ΅¨σ΅¨σ΅¨ π − σ΅¨ (σ΅©π¦ σ΅©σ΅© + σ΅©σ΅©π πΊ (π¦π−1 )σ΅©σ΅©σ΅©) . σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨σ΅¨ σ΅© π−1 σ΅© σ΅© π−1 (119) πΎ π¦ + πΏπ ππ πΊ (π¦π ) = π π 1 − π½π − πΏπ σ΅©σ΅© σ΅© σ΅©π πΊ (π¦π−1 ) − ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅© πΎπ + πΏπ σ΅© π σ΅¨σ΅¨ πΎ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨ + σ΅¨σ΅¨σ΅¨ π − σ΅¨ σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨σ΅¨ σ΅© σ΅© σ΅© σ΅© × (σ΅©σ΅©σ΅©π¦π−1 σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅©) σ΅© σ΅© σ΅© σ΅© ≤ σ΅©σ΅©σ΅©π¦π − π¦π−1 σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π¦π−1 ) − ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅© σ΅¨σ΅¨ πΎ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σ΅¨ σ΅© σ΅© σ΅© + σ΅¨σ΅¨σ΅¨ π − σ΅¨ (σ΅©π¦ σ΅©σ΅© + σ΅©σ΅©π πΊ (π¦π−1 )σ΅©σ΅©σ΅©) σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨σ΅¨ σ΅© π−1 σ΅© σ΅© π−1 σ΅© σ΅© σ΅¨ σ΅¨σ΅© σ΅© ≤ σ΅©σ΅©σ΅©π₯π − π₯π−1 σ΅©σ΅©σ΅© + σ΅¨σ΅¨σ΅¨πΌπ − πΌπ−1 σ΅¨σ΅¨σ΅¨ σ΅©σ΅©σ΅©πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© + (118) Furthermore, we note that π₯π+1 = π½π π (π₯π ) + (1 − π½π ) Vπ , π₯π = π½π−1 π (π₯π−1 ) + (1 − π½π−1 ) Vπ−1 , ∀π ≥ 1. (120) Also, simple calculations show that π₯π+1 − π₯π = π½π (π (π₯π ) − π (π₯π−1 )) + (π½π − π½π−1 ) × (π (π₯π−1 ) − Vπ−1 ) + (1 − π½π ) (Vπ − Vπ−1 ) . (121) This together with (119) implies that σ΅©σ΅© σ΅© σ΅©σ΅©π₯π+1 − π₯π σ΅©σ΅©σ΅© σ΅© σ΅¨ σ΅© σ΅¨ ≤ π½π σ΅©σ΅©σ΅©π (π₯π ) − π (π₯π−1 )σ΅©σ΅©σ΅© + σ΅¨σ΅¨σ΅¨π½π − π½π−1 σ΅¨σ΅¨σ΅¨ σ΅© σ΅© σ΅© σ΅© × σ΅©σ΅©σ΅©π (π₯π−1 ) − Vπ−1 σ΅©σ΅©σ΅© + (1 − π½π ) σ΅©σ΅©σ΅©Vπ − Vπ−1 σ΅©σ΅©σ΅© 16 Journal of Applied Mathematics σ΅© σ΅© ≤ π½π π σ΅©σ΅©σ΅©π₯π − π₯π−1 σ΅©σ΅©σ΅© Taking into account the boundedness of {πΊ(π₯π )} and {ππ πΊ(π₯π )}, by Lemma 6, we know that there exists a continuous strictly increasing function π1 : [0, ∞) → [0, ∞), π1 (0) = 0 such that for π ∈ πΉ σ΅¨ σ΅¨σ΅© σ΅© + σ΅¨σ΅¨σ΅¨π½π − π½π−1 σ΅¨σ΅¨σ΅¨ σ΅©σ΅©σ΅©π (π₯π−1 ) − Vπ−1 σ΅©σ΅©σ΅© + (1 − π½π ) σ΅© σ΅© × [ σ΅©σ΅©σ΅©π₯π − π₯π−1 σ΅©σ΅©σ΅© σ΅©σ΅© σ΅©2 σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© σ΅¨ σ΅¨σ΅© σ΅© + σ΅¨σ΅¨σ΅¨πΌπ − πΌπ−1 σ΅¨σ΅¨σ΅¨ σ΅©σ΅©σ΅©πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π¦π−1 ) − ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅© σ΅¨σ΅¨ πΎ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨ + σ΅¨σ΅¨σ΅¨ π − σ΅¨ σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨σ΅¨ σ΅© σ΅©2 σ΅© σ΅©2 ≤ πΌπ σ΅©σ΅©σ΅©πΊ (π₯π ) − πσ΅©σ΅©σ΅© + (1 − πΌπ ) σ΅©σ΅©σ΅©ππ πΊ (π₯π ) − πσ΅©σ΅©σ΅© σ΅© σ΅© − πΌπ (1 − πΌπ ) π1 (σ΅©σ΅©σ΅©πΊ (π₯π ) − ππ πΊ (π₯π )σ΅©σ΅©σ΅©) σ΅© σ΅©2 σ΅© σ΅©2 ≤ πΌπ σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + (1 − πΌπ ) σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© σ΅© σ΅© − πΌπ (1 − πΌπ ) π1 (σ΅©σ΅©σ΅©πΊ (π₯π ) − ππ πΊ (π₯π )σ΅©σ΅©σ΅©) σ΅© σ΅© σ΅© σ΅© × (σ΅©σ΅©σ΅©π¦π−1 σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅©) ] σ΅© σ΅©2 σ΅© σ΅© = σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© − πΌπ (1 − πΌπ ) π1 (σ΅©σ΅©σ΅©πΊ (π₯π ) − ππ πΊ (π₯π )σ΅©σ΅©σ΅©) . (124) σ΅© σ΅© ≤ (1 − π½π (1 − π)) σ΅©σ΅©σ΅©π₯π − π₯π−1 σ΅©σ΅©σ΅© σ΅¨ σ΅¨σ΅© σ΅© + σ΅¨σ΅¨σ΅¨π½π − π½π−1 σ΅¨σ΅¨σ΅¨ σ΅©σ΅©σ΅©π (π₯π−1 ) − Vπ−1 σ΅©σ΅©σ΅© Since {π¦π } and {ππ πΊ(π¦π )} are bounded, by Lemma 6, there exists a continuous strictly increasing function π2 : [0, ∞) → [0, ∞), π2 (0) = 0 such that for π ∈ πΉ σ΅¨ σ΅¨σ΅© σ΅© + σ΅¨σ΅¨σ΅¨πΌπ − πΌπ−1 σ΅¨σ΅¨σ΅¨ σ΅©σ΅©σ΅©πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π¦π−1 ) − ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅© σ΅¨σ΅¨ πΎ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σ΅¨ σ΅© σ΅© σ΅© + σ΅¨σ΅¨σ΅¨ π − σ΅¨ (σ΅©π¦ σ΅©σ΅© + σ΅©σ΅©π πΊ (π¦π−1 )σ΅©σ΅©σ΅©) σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨σ΅¨ σ΅© π−1 σ΅© σ΅© π−1 σ΅© σ΅© ≤ (1 − π½π (1 − π)) σ΅©σ΅©σ΅©π₯π − π₯π−1 σ΅©σ΅©σ΅© σ΅¨ σ΅¨ σ΅¨ σ΅¨ + σ΅¨σ΅¨σ΅¨π½π − π½π−1 σ΅¨σ΅¨σ΅¨ π + σ΅¨σ΅¨σ΅¨πΌπ − πΌπ−1 σ΅¨σ΅¨σ΅¨ π σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π¦π−1 ) − ππ−1 πΊ (π¦π−1 )σ΅©σ΅©σ΅© σ΅¨σ΅¨ πΎ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨ + σ΅¨σ΅¨σ΅¨ π − σ΅¨π σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨σ΅¨ σ΅© σ΅© = (1 − π½π (1 − π)) σ΅©σ΅©σ΅©π₯π − π₯π−1 σ΅©σ΅©σ΅© σ΅¨ σ΅¨ + π ( σ΅¨σ΅¨σ΅¨πΌπ − πΌπ−1 σ΅¨σ΅¨σ΅¨ σ΅¨ πΎπ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨ σ΅¨σ΅¨ πΎ + σ΅¨σ΅¨σ΅¨π½π − π½π−1 σ΅¨σ΅¨σ΅¨ + σ΅¨σ΅¨σ΅¨ π − σ΅¨) σ΅¨σ΅¨ 1 − π½π 1 − π½π−1 σ΅¨σ΅¨σ΅¨ σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π₯π−1 ) − ππ−1 πΊ (π₯π−1 )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π¦π−1 ) − ππ−1 πΊ (yπ−1 )σ΅©σ΅©σ΅© , ×[ πΎπ (π¦ − π) πΎπ + πΏπ π + πΏπ (π πΊ (π¦π ) − π)] πΎπ + πΏπ π σ΅©σ΅©2 σ΅© + π½π (π (π₯π ) − π) σ΅©σ΅©σ΅© σ΅©σ΅© σ΅© πΎ 2σ΅© σ΅© π ≤ (πΎπ + πΏπ ) σ΅©σ΅©σ΅© (π¦π − π) σ΅©σ΅© πΎπ + πΏπ + σ΅©σ΅©2 πΏπ σ΅© (ππ πΊ (π¦π ) − π)σ΅©σ΅©σ΅© σ΅©σ΅© πΎπ + πΏπ + 2π½π β¨π (π₯π ) − π, π½ (π₯π+1 − π)β© 2 (122) where supπ≥0 {β π(π₯π ) β + β Vπ β + β πΊ(π₯π ) β + β ππ πΊ(π₯π ) β + β π¦π β + β ππ πΊ(π¦π ) β} ≤ π for some π > 0. Utilizing Lemma 2, from conditions (ii)–(v) and the assumption on {ππ }, we deduce that σ΅© σ΅© lim σ΅©σ΅©π₯ − π₯π σ΅©σ΅©σ΅© = 0. π → ∞ σ΅© π+1 σ΅©σ΅© σ΅©2 σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© σ΅© = σ΅©σ΅©σ΅©π½π (π (π₯π ) − π) + πΎπ (π¦π − π) σ΅©2 + πΏπ (ππ πΊ (π¦π ) − π)σ΅©σ΅©σ΅© σ΅©σ΅© σ΅© = σ΅©σ΅©σ΅© (πΎπ + πΏπ ) σ΅©σ΅© (123) ≤ (πΎπ + πΏπ ) [ πΎπ σ΅©σ΅© σ΅©2 σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© πΎπ + πΏπ + − πΏπ σ΅©σ΅© σ΅©2 σ΅©π πΊ (π¦π ) − πσ΅©σ΅©σ΅© πΎπ + πΏπ σ΅© π πΎπ πΏπ 2 σ΅© σ΅© π2 (σ΅©σ΅©σ΅©π¦π − ππ πΊ (π¦π )σ΅©σ΅©σ΅©)] (πΎπ + πΏπ ) σ΅©σ΅© σ΅©σ΅© σ΅© + 2π½π σ΅©σ΅©π (π₯π ) − πσ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© Journal of Applied Mathematics 17 σ΅© σ΅© σ΅©2 σ΅©2 ≤ πΎπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© + πΏπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© Thus, from (123), (130), and π½π → 0, it follows that σ΅© σ΅© − πΎπ πΏπ π2 (σ΅©σ΅©σ΅©π¦π − ππ πΊ (π¦π )σ΅©σ΅©σ΅©) σ΅©σ΅© lim σ΅©π¦ π→∞ σ΅© π σ΅© σ΅©σ΅© σ΅© + 2π½π σ΅©σ΅©σ΅©π (π₯π ) − πσ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© σ΅© σ΅©2 σ΅© σ΅© ≤ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© − πΎπ πΏπ π2 (σ΅©σ΅©σ΅©π¦π − ππ πΊ (π¦π )σ΅©σ΅©σ΅©) σ΅©σ΅© lim σ΅©π¦ π→∞ σ΅© π σ΅© − πΊ (π₯π )σ΅©σ΅©σ΅© = lim (1 − πΌπ ) π→∞ σ΅© σ΅© × σ΅©σ΅©σ΅©ππ πΊ (π₯π ) − πΊ (π₯π )σ΅©σ΅©σ΅© = 0. (125) σ΅©σ΅© σ΅©2 σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© σ΅© σ΅©2 σ΅© σ΅© ≤ σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© − πΌπ (1 − πΌπ ) π1 (σ΅©σ΅©σ΅©πΊ (π₯π ) − ππ πΊ (π₯π )σ΅©σ΅©σ΅©) σ΅© σ΅© − πΎπ πΏπ π2 (σ΅©σ΅©σ΅©π¦π − ππ πΊ (π¦π )σ΅©σ΅©σ΅©) σ΅© σ΅©σ΅© σ΅© + 2π½π σ΅©σ΅©σ΅©π (π₯π ) − πσ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© . It immediately follows that σ΅© σ΅© πΌπ (1 − πΌπ ) π1 (σ΅©σ΅©σ΅©πΊ (π₯π ) − ππ πΊ (π₯π )σ΅©σ΅©σ΅©) σ΅© σ΅© + πΎπ πΏπ π2 (σ΅©σ΅©σ΅©π¦π − ππ πΊ (π¦π )σ΅©σ΅©σ΅©) σ΅© σ΅©2 σ΅© σ΅©2 ≤ σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© − σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© σ΅© σ΅©σ΅© σ΅© + 2π½π σ΅©σ΅©σ΅©π (π₯π ) − πσ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© σ΅© σ΅© ≤ (σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅©) σ΅©σ΅©σ΅©π₯π − π₯π+1 σ΅©σ΅©σ΅© σ΅© σ΅©σ΅© σ΅© + 2π½π σ΅©σ΅©σ΅©π (π₯π ) − πσ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© . (126) (127) π→∞ (128) Since π½π → 0 and β π₯π+1 − π₯π β → 0, we conclude from conditions (i) and (vi) that (πΊ (π₯π ) − ππ πΊ (π₯π )) = 0, Utilizing the properties of π1 and π2 , we have σ΅© σ΅© lim σ΅©σ΅©πΊ (π₯π ) − ππ πΊ (π₯π )σ΅©σ΅©σ΅© = 0, π→∞ σ΅© σ΅© σ΅© lim σ΅©σ΅©π¦ − ππ πΊ (π¦π )σ΅©σ΅©σ΅© = 0. π→∞ σ΅© π Note that σ΅©σ΅© σ΅© σ΅©σ΅©π¦π − π₯π σ΅©σ΅©σ΅© σ΅© = σ΅©σ΅©σ΅©π₯π+1 − π₯π − π½π (π (π₯π ) − π¦π ) σ΅© − πΏπ (ππ πΊ (π¦π ) − π¦π )σ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© ≤ σ΅©σ΅©σ΅©π₯π+1 − π₯π σ΅©σ΅©σ΅© + π½π σ΅©σ΅©σ΅©π (π₯π ) − π¦π σ΅©σ΅©σ΅© σ΅© σ΅© + πΏπ σ΅©σ΅©σ΅©ππ πΊ (π¦π ) − π¦π σ΅©σ΅©σ΅© . σ΅© − πΊ (π₯π )σ΅©σ΅©σ΅© = 0. (134) By (130) and Lemma 7, we have σ΅© σ΅© ≤ σ΅©σ΅©σ΅©ππΊ (π₯π ) − ππ πΊ (π₯π )σ΅©σ΅©σ΅© (135) σ΅© σ΅© + σ΅©σ΅©σ΅©ππ πΊ (π₯π ) − πΊ (π₯π )σ΅©σ΅©σ΅© σ³¨→ 0 as π σ³¨→ ∞. In terms of (134) and (135), we have lim inf πΏπ = lim inf (1 − π½π − πΎπ ) = 1 − lim sup (π½π + πΎπ ) > 0. σ΅© σ΅© lim π (σ΅©σ΅©π¦ − ππ πΊ (π¦π )σ΅©σ΅©σ΅©) = 0. π→∞ 2 σ΅© π σ΅©σ΅© lim σ΅©π₯ π→∞ σ΅© π σ΅©σ΅© σ΅© σ΅©σ΅©ππΊ (π₯π ) − πΊ (π₯π )σ΅©σ΅©σ΅© According to condition (vi), we get lim π π→∞ 1 (133) This together with (132) implies that which together with (124) implies that π→∞ (132) On the other hand, from (130), we get σ΅© σ΅©σ΅© σ΅© + 2π½π σ΅©σ΅©σ΅©π (π₯π ) − πσ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© , π→∞ σ΅© − π₯π σ΅©σ΅©σ΅© = 0. (129) σ΅©σ΅© σ΅© σ΅©σ΅©π₯π − ππ₯π σ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© ≤ σ΅©σ΅©σ΅©π₯π − πΊ (π₯π )σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©πΊ (π₯π ) − ππΊ (π₯π )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©ππΊ (π₯π ) − ππ₯π σ΅©σ΅©σ΅© σ΅© σ΅© ≤ 2 σ΅©σ΅©σ΅©π₯π − πΊ (π₯π )σ΅©σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©πΊ (π₯π ) − ππΊ (π₯π )σ΅©σ΅©σ΅© σ³¨→ 0 as π σ³¨→ ∞. (136) Define a mapping ππ₯ = (1 − π)ππ₯ + ππΊ(π₯), where π ∈ (0, 1) is a constant. Then by Lemma 9, we have that Fix(π) = Fix(π)∩ Fix(πΊ) = πΉ. We observe that σ΅© σ΅©σ΅© σ΅©σ΅©π₯π − ππ₯π σ΅©σ΅©σ΅© σ΅© σ΅© = σ΅©σ΅©σ΅©(1 − π) (π₯π − ππ₯π ) + π (π₯π − πΊ (π₯π ))σ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© ≤ (1 − π) σ΅©σ΅©σ΅©π₯π − ππ₯π σ΅©σ΅©σ΅© + π σ΅©σ΅©σ΅©π₯π − πΊ (π₯π )σ΅©σ΅©σ΅© . (137) From (134) and (136), we obtain lim β π₯π − ππ₯π β= 0. π→∞ (130) (138) Now, we claim that lim sup β¨π (π) − π, π½ (π₯π − π)β© ≤ 0, π→∞ (139) where π = π − limπ‘ → 0 π₯π‘ with π₯π‘ being the fixed point of the contraction π₯ σ³¨σ³¨→ π‘π (π₯) + (1 − π‘) ππ₯. (131) (140) Then π₯π‘ solves the fixed point equation π₯π‘ = π‘π(π₯π‘ ) + (1 − π‘)ππ₯π‘ . Thus we have σ΅©σ΅© σ΅© σ΅© σ΅© σ΅©σ΅©π₯π‘ − π₯π σ΅©σ΅©σ΅© = σ΅©σ΅©σ΅©(1 − π‘) (ππ₯π‘ − π₯π ) + π‘ (π (π₯π‘ ) − π₯π )σ΅©σ΅©σ΅© . (141) 18 Journal of Applied Mathematics By Lemma 3, we conclude that Hence it follows that σ΅©σ΅© σ΅©2 σ΅©σ΅©π₯π‘ − π₯π σ΅©σ΅©σ΅© lim sup β¨π (π) − π, π½ (π₯π − π)β© π→∞ 2σ΅© σ΅© σ΅©2 ≤ (1 − π‘) σ΅©σ΅©ππ₯π‘ − π₯π σ΅©σ΅©σ΅© ≤ lim sup β¨π (π) − π, π½ (π₯π − π) − π½ (π₯π − π₯π‘ )β© π→∞ + 2π‘ β¨π (π₯π‘ ) − π₯π , π½ (π₯π‘ − π₯π )β© σ΅© σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©π₯π‘ − πσ΅©σ΅©σ΅© lim sup σ΅©σ΅©σ΅©π₯π − π₯π‘ σ΅©σ΅©σ΅© σ΅© σ΅© σ΅©2 σ΅© ≤ (1 − π‘) (σ΅©σ΅©σ΅©ππ₯π‘ − ππ₯π σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©ππ₯π − π₯π σ΅©σ΅©σ΅©) 2 π→∞ (148) σ΅© σ΅© σ΅© σ΅© + π σ΅©σ΅©σ΅©π − π₯π‘ σ΅©σ΅©σ΅© lim sup σ΅©σ΅©σ΅©π₯π − π₯π‘ σ΅©σ΅©σ΅© + 2π‘ β¨π (π₯π‘ ) − π₯π , π½ (π₯π‘ − π₯π )β© π→∞ σ΅© σ΅© σ΅© ≤ (1 − π‘)2 [σ΅©σ΅©σ΅©π₯π‘ − π₯π σ΅©σ΅© + 2 σ΅©σ΅©σ΅©π₯π‘ − π₯π σ΅©σ΅©σ΅© σ΅©σ΅©2 + lim sup β¨π (π₯π‘ ) − π₯π‘ , π½ (π₯π − π₯π‘ )β© . (142) σ΅© σ΅© σ΅© σ΅©2 × σ΅©σ΅©σ΅©ππ₯π − π₯π σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©ππ₯π − π₯π σ΅©σ΅©σ΅© ] π→∞ Taking into account that π₯π‘ → π as π‘ → 0, we have from (146) + 2π‘ β¨π (π₯π‘ ) − π₯π‘ , π½ (π₯π‘ − π₯π )β© + 2π‘ β¨π₯π‘ − π₯π , π½ (π₯π‘ − π₯π )β© σ΅©2 σ΅© = (1 − 2π‘ + π‘2 ) σ΅©σ΅©σ΅©π₯π‘ − π₯π σ΅©σ΅©σ΅© + ππ (π‘) lim sup β¨π (π) − π, π½ (π₯π − π)β© π→∞ σ΅©2 σ΅© + 2π‘ β¨π (π₯π‘ ) − π₯π‘ , π½ (π₯π‘ − π₯π )β© + 2π‘σ΅©σ΅©σ΅©π₯π‘ − π₯π σ΅©σ΅©σ΅© , = lim sup lim sup β¨π (π) − π, π½ (π₯π − π)β© π‘→0 π→∞ ≤ lim sup lim sup β¨π (π) − π, π½ (π₯π − π) − π½ (π₯π − π₯π‘ )β© . where σ΅© σ΅© σ΅© σ΅© ππ (π‘) = (1 − π‘) (2 σ΅©σ΅©σ΅©π₯π‘ − π₯π σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©π₯π − ππ₯π σ΅©σ΅©σ΅©) σ΅© σ΅© × σ΅©σ΅©σ΅©π₯π − ππ₯π σ΅©σ΅©σ΅© σ³¨→ 0 as π σ³¨→ ∞. π‘→0 π→∞ (149) 2 (143) It follows from (142) that π‘σ΅© σ΅©2 1 β¨π₯π‘ − π (π₯π‘ ) , π½ (π₯π‘ − π₯π )β© ≤ σ΅©σ΅©σ΅©π₯π‘ − π₯π σ΅©σ΅©σ΅© + ππ (π‘) . 2 2π‘ (144) Letting π → ∞ in (144) and noticing (143), we derive π‘ lim sup β¨π₯π‘ − π (π₯π‘ ) , π½ (π₯π‘ − π₯π )β© ≤ π2 , 2 π→∞ Since π has a uniformly GaΜteaux differentiable norm, the duality mapping π½ is norm-to-weak∗ uniformly continuous on bounded subsets of π. Consequently, the two limits are interchangeable, and hence (139) holds. From (123), we get (π₯π+1 − π) − (π₯π − π) → 0. Noticing the norm-to-weak∗ uniform continuity of π½ on bounded subsets of π, we deduce from (139) that lim sup β¨π (π) − π, π½ (π₯π+1 − π)β© π→∞ (145) = lim sup (β¨π (π) − π, π½ (π₯π+1 − π) − π½ (π₯π − π)β© π→∞ 2 where π2 > 0 is a constant such that β π₯π‘ − π₯π β ≤ π2 for all π‘ ∈ (0, 1) and π ≥ 0. Taking π‘ → 0 in (145), we have lim sup lim sup β¨π₯π‘ − π (π₯π‘ ) , π½ (π₯π‘ − π₯π )β© ≤ 0. π‘→0 π→∞ + β¨π (π) − π, π½ (π₯π+1 − π)β©) = lim sup β¨π (π) − π, π½ (π₯π − π)β© ≤ 0. π→∞ (150) (146) Finally, let us show that π₯π → π as π → ∞. We observe that On the other hand, we have β¨π (π) − π, π½ (π₯π − π)β© σ΅©σ΅© σ΅© σ΅© σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© = σ΅©σ΅©σ΅©πΌπ (πΊ (π₯π ) − π) = β¨π (π) − π, π½ (π₯π − π) − π½ (π₯π − π₯π‘ )β© + β¨π₯π‘ − π, π½ (π₯π − π₯π‘ )β© + β¨π (π) − π (π₯π‘ ) , π½ (π₯π − π₯π‘ )β© + β¨π (π₯π‘ ) − π₯π‘ , π½ (xπ − π₯π‘ )β© . (147) σ΅© + (1 − πΌπ ) (ππ πΊ (π₯π ) − π)σ΅©σ΅©σ΅© σ΅© σ΅© σ΅© σ΅© ≤ πΌπ σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + (1 − πΌπ ) σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© σ΅© σ΅© = σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© , (151) Journal of Applied Mathematics 19 σ΅©σ΅© σ΅©2 σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© = π½π β¨π (π₯π ) − π (π) + π (π) − π, π½ (π₯π+1 − π)β© + β¨πΎπ (π¦π − π) + πΏπ (ππ πΊ (π¦π ) − π) , π½ (π₯π+1 − π)β© σ΅© σ΅©σ΅© σ΅© ≤ π½π σ΅©σ΅©σ΅©π (π₯π ) − π (π)σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© + π½π β¨π (π) − π, π½ (π₯π+1 − π)β© σ΅©σ΅© σ΅© σ΅© + σ΅©σ΅©σ΅©πΎπ (π¦π − π) + πΏπ (ππ πΊ (π¦π ) − π)σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© σ΅© σ΅©σ΅© σ΅© ≤ π½π π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© (i) 0 < lim inf π → ∞ πΌπ ≤ lim supπ → ∞ πΌπ < 1, + π½π β¨π (π) − π, π½ (π₯π+1 − π)β© (ii) limπ → ∞ π½π = 0 and ∑∞ π=0 π½π = ∞, σ΅© σ΅©σ΅© σ΅© + (πΎπ + πΏπ ) σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© (iii) ∑∞ π=1 |πΌπ − πΌπ−1 | < ∞ or limπ → ∞ |πΌπ − πΌπ−1 |/π½π = 0, (iv) ∑∞ π=1 |π½π − π½π−1 | < ∞ or limπ → ∞ π½π−1 /π½π = 1, σ΅© σ΅©σ΅© σ΅© ≤ π½π π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© (v) ∑∞ π=1 |(πΎπ /(1 − π½π )) − (πΎπ−1 /(1 − π½π−1 ))| < ∞ or limπ → ∞ (1/π½π )|(πΎπ /(1 − π½π )) − (πΎπ−1 /(1 − π½π−1 ))| = 0, + π½π β¨π (π) − π, π½ (π₯π+1 − π)β© σ΅© σ΅©σ΅© σ΅© + (1 − π½π ) σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© (vi) 0 < lim inf π → ∞ πΎπ ≤ lim supπ → ∞ πΎπ < 1. σ΅© σ΅©σ΅© σ΅© = (1 − π½π (1 − π)) σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© Then {π₯π } converges strongly to π ∈ πΉ, which solves the following VIP: + π½π β¨π (π) − π, π½ (π₯π+1 − π)β© β¨π − π (π) , π½ (π − π)β© ≤ 0, 1 − π½π (1 − π) σ΅©σ΅© σ΅©2 σ΅© σ΅©2 (σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© ) 2 1 σ΅©σ΅© σ΅©2 σ΅©π₯ − πσ΅©σ΅©σ΅© 2 σ΅© π+1 + π½π β¨π (π) − π, π½ (π₯π+1 − π)β© . (152) So, we have σ΅©σ΅© σ΅©2 σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© σ΅© σ΅©2 ≤ (1 − π½π (1 − π)) σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + 2π½π β¨π (π) − π, π½ (π₯π+1 − π)β© σ΅© σ΅©2 = (1 − π½π (1 − π)) σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + π½π (1 − π) ∀π ∈ πΉ. (155) Further, we illustrate Theorem 22 by virtue of an example, that is, the following corollary. + π½π β¨π (π) − π, π½ (π₯π+1 − π)β© 1 − π½π (1 − π) σ΅©σ΅© σ΅©2 σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© + 2 (154) ∀π ≥ 0, where 1 − (π π /(1 + π π ))(1 − √(1 − πΌπ )/π π ) ≤ ππ ≤ 1 for π = 1, 2. Suppose that {πΌπ }, {π½π }, {πΎπ }, and {πΏπ } are the sequences in (0, 1) satisfying the following conditions: σ΅© σ΅© σ΅© σ΅© σ΅© σ΅© + (πΎπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅© + πΏπ σ΅©σ΅©σ΅©π¦π − πσ΅©σ΅©σ΅©) σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© σ΅© σ΅©σ΅© σ΅© = π½π π σ΅©σ΅©σ΅©π₯π − πσ΅©σ΅©σ΅© σ΅©σ΅©σ΅©π₯π+1 − πσ΅©σ΅©σ΅© ≤ π¦π = πΌπ πΊ (π₯π ) + (1 − πΌπ ) ππΊ (π₯π ) , π₯π+1 = π½π π (π₯π ) + πΎπ π¦π + πΏπ ππΊ (π¦π ) , + π½π β¨π (π) − π, π½ (π₯π+1 − π)β© ≤ GaΜteaux differentiable norm. Let ΠπΆ be a sunny nonexpansive retraction from π onto πΆ. Let the mapping π΅π : πΆ → π be π π strictly pseudocontractive and πΌπ -strongly accretive with πΌπ + π π ≥ 1 for π = 1, 2. Let π : πΆ → πΆ be a contraction with coefficient π ∈ (0, 1). Let π be a nonexpansive mapping of πΆ into itself such that πΉ = Fix(π) ∩ Ω =ΜΈ 0, where Ω is the fixed point set of the mapping πΊ = ΠπΆ(πΌ − π1 π΅1 )ΠπΆ(πΌ − π2 π΅2 ). For arbitrarily given π₯0 ∈ πΆ, let {π₯π } be the sequence generated by Corollary 24. Let πΆ be a nonempty, closed, and convex subset of a uniformly convex Banach space π which has a uniformly GaΜteaux differentiable norm. Let ΠπΆ be a sunny nonexpansive retraction from π onto πΆ. Let π : πΆ → C be a contraction with coefficient π ∈ (0, 1). Let π : πΆ → πΆ be a self-mapping on πΆ such that πΌ − π is π-strictly pseudocontractive and π-strongly accretive with π + π ≥ 1, and let π be a nonexpansive mapping of πΆ into itself such that πΉ = Fix(π) ∩ Fix(T) =ΜΈ 0. For arbitrarily given π₯0 ∈ πΆ, let {π₯π } be the sequence generated by π¦π = πΌπ πΊ (π₯π ) + (1 − πΌπ ) π (πΌ − π (πΌ − π)) π₯π , (153) 2 β¨π (π) − π, π½ (π₯π+1 − π)β© . 1−π Since ∑∞ π=0 π½π = ∞ and lim supπ → ∞ β¨π(π) − π, π½(π₯π+1 − π)β© ≤ 0, by Lemma 2, we conclude from (153) that π₯π → π as π → ∞. This completes the proof. Corollary 23. Let πΆ be a nonempty, closed, and convex subset of a uniformly convex Banach space π which has a uniformly π₯π+1 = π½π π (π₯π ) + πΎπ π¦π + πΏπ π (πΌ − π (πΌ − π)) π¦π , ∀π ≥ 0, (156) where 1 − (π/(1 + π))(1 − √(1 − π)/π) ≤ π ≤ 1. Suppose that {πΌπ }, {π½π }, {πΎπ }, and {πΏπ } are the sequences in (0, 1) satisfying the following conditions: (i) 0 < lim inf π → ∞ πΌπ ≤ lim supπ → ∞ πΌπ < 1, (ii) limπ → ∞ π½π = 0 and ∑∞ π=0 π½π = ∞, (iii) ∑∞ π=1 |πΌπ − πΌπ−1 | < ∞ or limπ → ∞ |πΌπ − πΌπ−1 |/π½π = 0, (iv) ∑∞ π=1 |π½π − π½π−1 | < ∞ or limπ → ∞ π½π−1 /π½π = 1, 20 Journal of Applied Mathematics (v) ∑∞ π=1 |(πΎπ /(1 − π½π )) − (πΎπ−1 /(1 − π½π−1 ))| < ∞ or limπ → ∞ (1/π½π )|(πΎπ /(1 − π½π )) − (πΎπ−1 /(1 − π½π−1 ))| = 0, (vi) 0 < lim inf π → ∞ πΎπ ≤ lim supπ → ∞ πΎπ < 1. Then {π₯π } converges strongly to π ∈ πΉ, which solves the following VIP: β¨π − π (π) , π½ (π − π)β© ≤ 0, ∀π ∈ πΉ. (157) Proof. Utilizing the arguments similar to those in the proof of Corollary 16, we can obtain the desired result. Remark 25. As previous, we emphasize that our composite iterative algorithms (i.e., the iterative schemes (27) and (111)) are based on Korpelevich’s extragradient method and viscosity approximation method. It is well known that the so-called viscosity approximation method must contain a contraction π on πΆ. In the meantime, it is worth pointing out that our proof of Theorems 14 and 22 must make use of Lemma 8 for implicit viscosity approximation method; that is, Lemma 8 plays a key role in our proof of Theorems 14 and 22. Therefore, there is no doubt that the contraction π in Theorems 14 and 22 cannot be replaced by a general πLipschitzian mapping with constant π ≥ 0. Remark 26. Theorem 22 improves, extends, supplements, and develops [2, Theorem 3.1 and Corollary 3.2] and [5, Theorems 3.1] in the following aspects. (i) The problem of finding a point π ∈ βπ Fix(ππ ) ∩ Ω in Theorem 22 is more general and more subtle than the problem of finding a point π ∈ Fix(π) ∩ VI(πΆ, π΄) in Jung [5, Theorem 3.1]. (ii) The iterative scheme in [2, Theorem 3.1] is extended to develop the iterative scheme (111) of Theorem 22 by virtue of the iterative scheme of [5, Theorem 3.1]. The iterative scheme (111) in Theorem 22 is more advantageous and more flexible than the iterative scheme in [2, Theorem 3.1] because it involves several parameter sequences {πΌπ }, {π½π }, {πΎπ }, and {πΏπ }. (iii) The iterative scheme (111) in Theorem 22 is very different from everyone in both [2, Theorem 3.1] and [5, Theorem 3.1] because the mappings ππ and πΊ in the iterative scheme of [2, Theorem 3.1] and the mapping πππΆ(πΌ − π π π΄) in the iterative scheme of [5, Theorem 3.1] are replaced by the same composite mapping ππ πΊ in the iterative scheme (111) of Theorem 22. (iv) The proof in [2, Theorem 3.1] depends on the argument techniques in [3], the inequality in 2-uniformly smooth Banach spaces, and the inequality in smooth and uniform convex Banach spaces. However, the proof of Theorem 22 does not depend on the argument techniques in [3], the inequality in 2-uniformly smooth Banach spaces, and the inequality in smooth and uniform convex Banach spaces. 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