Research article

Convergence analysis of general parallel S-iteration process for system of mixed generalized Cayley variational inclusions

  • Received: 17 July 2022 Revised: 29 August 2022 Accepted: 08 September 2022 Published: 16 September 2022
  • MSC : 47H09, 90C33

  • This work is concentrated on the study of a system of mixed generalized Cayley variational inclusions. Parallel Mann iteration process is defined in order to achieve the solution. We define an altering point problem which is equivalent to our system and then we construct general parallel S-iteration process. Finally, we discuss convergence criteria and provide an example.

    Citation: Iqbal Ahmad, Faizan Ahmad Khan, Arvind Kumar Rajpoot, Mohammed Ahmed Osman Tom, Rais Ahmad. Convergence analysis of general parallel S-iteration process for system of mixed generalized Cayley variational inclusions[J]. AIMS Mathematics, 2022, 7(11): 20259-20274. doi: 10.3934/math.20221109

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  • This work is concentrated on the study of a system of mixed generalized Cayley variational inclusions. Parallel Mann iteration process is defined in order to achieve the solution. We define an altering point problem which is equivalent to our system and then we construct general parallel S-iteration process. Finally, we discuss convergence criteria and provide an example.



    Stampacchia[1] initiated the study of variational inequalities in 1964, which evolved in many applications related to nonlinear analysis, economics, physics, operations research, optimization, image recovery, signal processing, control theory, game theory, transportation theory, etc., see for example [2,3,4,5,6,7]. Hassouni and Moudafi[8] originated variational inclusions and proposed an scheme to solve them. System of variational inclusions are the generalized forms of variational inclusions, see [9,10,11,12]. In particular, Pang[13] showed that traffic equilibria, spatial equilibria, Nash equilibria and general equilibria can be transformed into a system of variational inequalities. Cayley operator is defined in terms of a resolvent operator and has many applications in Quaternion homography, Real homography, Complex homography, etc., see for example [14,15]. The S-iteration process was introduced by Agarwal, O'Regan and Sahu [16] gives faster rate of convergence than Mann iteration process[17] as well as Ishikawa iteration process[18].Sahu[19] introduced and studied the parallel S-iteration process and applied it to solve a system of operator equations in Banach space. For more details of the subject and related topics, see [20,21,22,23,24,25,26,27,28,29,30,31,32,33].

    Since variational inclusions, system of variational inclusions, Cayley operator and Yosida approximation operator all have useful applications in applicable sciences, by combining all these concepts, we consider a system of mixed genearlized Cayley variational inclusions. We define parallel Mann iteration process with an equivalent altering point problem and general parallel S-iteration process to obtain the solution. Convergence criteria is also discussed with a numerical example.

    We denote a real Banach space by ˆE and its dual by ˆE. We denote norm by and duality pairing by ,. The normalized duality mapping ˆJ:ˆE2ˆE is defined by

    ˆJ(x)={fˆE:x,f=xf,f=x},xˆE.

    The space ˆE is called uniformly smooth if

    limt0τˆE(t)t=0,

    where τˆE(t) is the modulus of smoothness.

    Definition 2.1. For any x,yˆE and ˆj(xy)ˆJ(xy), a single-valued mapping A:ˆEˆE is called

    (i) accretive, if

    A(x)A(y),ˆj(xy)0,

    (ii) strictly accretive, if

    A(x)A(y),ˆj(xy)>0,

    and the equality holds if and only if x=y,

    (iii) strongly accretive, if there exist a constant r>0 such that

    A(x)A(y),ˆj(xy)rxy2,

    (iv) Lipschitz continuous, if there exist a constant δA>0 such that

    A(x)A(y)δAxy,

    Definition 2.2. [34] Let D1(ϕ)ˆE and D2(ϕ)ˆE. Then xD1 and yD2 are altering points of mappings S1:D1D2 and S2:D2D1, if S1(x)=y and S2(y)=x.

    Alt(S1,S2) means the set of altering points of mappings S1 and S2 such that

    Alt(S1,S2)={(x,y)D1×D2:S1(x)=y,S2(y)=x}.

    Definition 2.3. [35] Let A:ˆEˆE be single-valued mapping. A multi-valued mapping M:ˆE2ˆE is said to be A-accretive if M is accretive and [A+λM](ˆE)=ˆE, for all λ>0.

    Definition 2.4. [35] Let A:ˆEˆE be single-valued mapping and M:ˆE2ˆE be A-accretive multi-valued mapping. The generalized resolvent operator RMA,λ:ˆEˆE is defined by

    RMA,λ(x)=[A+λM]1(x), for all xˆE. (2.1)

    Definition 2.5. The generalized Yosida approximation operator ˆJMA,λ:ˆEˆE is defined by

    ˆJMA,λ(x)=1λ[ARMA,λ](x), for all xˆEandλ>0. (2.2)

    Definition 2.6. The generalized Cayley operator CMA,λ:ˆEˆE is defined by

    CMA,λ(x)=[2RMA,λA](x), for all xˆEandλ>0. (2.3)

    Lemma 2.1. [36] Consider ˆE to be uniformly smooth Banach space and ˆJ:ˆE2ˆE to be normalized duality mapping. Then, following (i) and (ii) hold:

    (i) x+y2x2+2y,ˆj(x+y), for all ˆj(x+y)ˆJ(x+y),

    (ii) xy,ˆj(x)ˆj(y)2d2ρˆE(4xyd), where d=(x2+y2)2.

    Proposition 2.1. [35] Let A:ˆEˆE be strongly accretive mapping with constant r and M:ˆE2ˆE be A-accretive multi-valued mapping. Then generalized resolvent operator RMA,λ:ˆEˆE satisfy,

    RMA,λ(x)RMA,λ(y)1rxy, for all x,yˆE.

    Proposition 2.2. [35] The generalized Yosida approximation operator is

    (i) θ1-Lipschitz continuous, where θ1=δAr+1λr; δA, r, λ>0, if A:ˆEˆE is Lipschitz continuous with constant δA,

    (ii) θ2-strongly accretive, where θ2=r21λr; r>1, λ>0, if A:ˆEˆE is strongly accretive with constant r.

    Proposition 2.3. [35] The generalized Cayley operator is θ3-Lipschitz continuous, where θ3=2+δArr; δA,r>0, if A:ˆEˆE is Lipschitz continuous with constant δA.

    Let A,B:ˆEˆE be single-valued mappings and M,N:ˆE2ˆE be multi-valued mappings. Let RMA,λ:ˆEˆE and CMA,λ:ˆEˆE be generalized resolvent operator and generalized Cayley operator, respectively. We study the following problem:

    For each λ,ρ>0, find (x,y)ˆE׈E satisfying

    {0A(x)B(y)+λ(CMA,λ(RMA,λ(y))+M(x))0B(y)A(x)+ρ(CNB,ρ(RNB,ρ(x))+N(y)). (3.1)

    The following lemma is fixed point formulation for system (3.1).

    Lemma 3.1. Let A,B:ˆEˆE be single-valued mappings and M,N:ˆE2ˆE be multi-valued mappings such that A is δA-Lipschitz continuous and r1-strongly accretive maaping, B is δB-Lipschitz continuous and r2-strongly accretive maaping, M and N are A-accretive and B-accretive multi-valued mappings, respectively. Let RMA,λ,ˆJMA,λ,CMA,λ:ˆEˆE be generalized resolvent operator, generalized Yosida approximation operator and Cayley operator, respectively. Then, system of mixed generalized Cayley variational inclusions (3.1) admits a solution (x,y)ˆE׈E, if and only if it satisfies the following equations:

    x=RMA,λ[RNB,ρ(y)+(ρˆJNB,ρ(y)λCMA,λ(RMA,λ(y)))]y=RNB,ρ[RMA,λ(x)+(λˆJMA,λ(x)ρCNB,ρ(RNB,ρ(x)))], (3.2)

    where λ,ρ>0 are constants.

    Proof. Proof is easy and hence omitted.

    Using Lemma 3.1, we suggest following parallel Mann iteration process to solve system of mixed generalized Cayley variational inclusions (3.1).

    Parallel Mann iteration process 3.1. Let x1,y1ˆE, then compute {xn} and {yn} by the iterative process:

    {xn+1=(1αn)xn+αnRMA,λ[RNB,ρ(yn)+(ρˆJNB,ρ(yn)λCMA,λ(RMA,λ(yn)))]yn+1=(1βn)yn+βnRNB,ρ[RMA,λ(xn)+(λˆJMA,λ(xn)ρCNB,ρ(RNB,ρ(xn)))], (3.3)

    where {αn} and {βn} are sequences in [0,1] and n=1,2,.

    Theorem 3.1. Let ˆE be real uniformly smooth Banach space with modulus of smoothness τˆE(t)Ct2 for some C>0. Let A,B:ˆEˆE be single-valued mappings and M,N:ˆE2ˆE be multi-valued mappings such that A is δA-Lipschitz continuous and r1-strongly accretive maaping, B is δB-Lipschitz continuous and r2-strongly accretive maaping, M and N are A-accretive and B-accretive multi-valued mappings, respectively. Suppose that generalized resolvent operators RMA,λ and RNB,ρ are Lipschitz continuous with constants 1r1 and 1r2; generalized Yosida approximation operators ˆJMA,λ and ˆJNB,ρ are Lipschitz continuous with constant θ1 and θ1, and strongly accretive with constants θ2 and θ2, and generalized Cayley operators CMA,λ and CNB,ρ are Lipschitz continuous with constant θ3 and θ3, respectively. Let for some λ,ρ>0, the following conditions are satisfied:

    {|λr1r2(r1ρ)r1θ3r2|<ρ2r21(12θ2+64Cθ12)θ23,|ρr1r2(r2λ)r2θ3r1|<λ2r22(12θ2+64Cθ12)θ32,2θ2<1+64Cθ12and2θ2<1+64Cθ21, (3.4)

    where θ1=δAr1+1λr1,θ1=δBr2+1ρr2, θ2=r211λr1,θ2=r221ρr2,θ3=2+δAr1r1 and θ3=2+δBr2r2.

    Then, the iterative sequences {xn} and {yn} generated by process 3.1 strongly converge to the solution (x,y)ˆE׈E of our system (3.1).

    Proof. Applying parallel Mann iteration process 3.1, Propositions 2.1–2.3, we have

    xn+1x=((1αn)xn+αnRMA,λ[RNB,ρ(yn)+(ρˆJNB,ρ(yn)λCMA,λ(RMA,λ(yn)))])((1αn)x+αnRMA,λ[RNB,ρ(y)+(ρˆJNB,ρ(y)λCMA,λ(RMA,λ(y)))])(1αn)xnx+αnRMA,λ[RNB,ρ(yn)+(ρˆJNB,ρ(yn)λCMA,λ(RMA,λ(yn)))]RMA,λ[RNB,ρ(y)+(ρˆJNB,ρ(y)λCMA,λ(RMA,λ(y)))](1αn)xnx+αn1r1[RNB,ρ(yn)+(ρˆJNB,ρ(yn)λCMA,λ(RMA,λ(yn)))][RNB,ρ(y)+(ρˆJNB,ρ(y)λCMA,λ(RMA,λ(y)))](1αn)xnx+αn1r1(RNB,ρ(yn)RNB,ρ(y)+ρˆJNB,ρ(yn)ˆJNB,ρ(y)+λCMA,λ(RMA,λ(yn))CMA,λ(RMA,λ(y)))(1αn)xnx+αn(1r1r2+ρr1+λθ3r21)yny+αnρr1(yny)(ˆJNB,ρ(yn)ˆJNB,ρ(y)). (3.5)

    Using Lemma 2.1, we evaluate

    (yny)(ˆJNB,ρ(yn)ˆJNB,ρ(y))2yny2+2(ˆJNB,ρ(yn)ˆJMA,λ(y)),ˆj((yny)(ˆJNB,ρ(yn)ˆJNB,ρ(y)))=yny2+2(ˆJNB,ρ(yn)ˆJNB,ρ(y)),ˆj(yny)+2(ˆJNB,ρ(yn)ˆJNB,ρ(y)),ˆj((yny)(ˆJNB,ρ(yn)ˆJNB,ρ(y)))ˆj(yny)yny22θ2yny2+4d2τˆE(4ˆJNB,ρ(yn)ˆJNB,ρ(y)d)yny22θ2yny2+64CˆJNB,ρ(yn)ˆJNB,ρ(y)2(12θ2+64Cθ12)yny2. (3.6)

    Using (3.6), (3.5) becomes

    xn+1x(1αn)xnx+αn(1r1r2+ρr1+λθ3r21)yny+αnρ(12θ2+64Cθ21)r1yny=(1αn)xnx+αnΩyny, (3.7)

    where

    Ω=(1r1r2+ρr1+λθ3r21)+ρ(12θ2+64Cθ21)r1.

    Using the similar arguments as for (3.5)–(3.7), we compute

    yn+1y(1αn)yny+αn(1r1r2+λr2+ρθ3r22)xnx+αnλ(12θ1+64Cθ22)r2xnx=(1αn)yny+αnΩxnx, (3.8)

    where

    Ω=(1r1r2+λr2+ρθ3r22)+λ(12θ2+64Cθ21)r2.

    Combining (3.7) and (3.8), we get

    xn+1x+yn+1y(1αn)xnx+αnΩyny+(1αn)yny+αnΩxnx(1αn)(xnx+yny)+αnmax{Ω,Ω}(xnx+yny),

    which implies that

    xn+1x+yn+1y(1αn(1Ω))(xnx+yny), (3.9)

    where Ω=max{Ω,Ω}. Now, we define the norm . on ˆE׈E by (x,y)=x+y, for all (x,y)ˆE׈E. Using (3.9), we have

    (xn+1,yn+1)(x,y)=(xn+1x,yn+1y)=xn+1x+yn+1y(1αn(1Ω))(xnx+yny)=(1αn(1Ω))(xn,yn)(x,y).

    From condition (3.4), it is clear that Ω<1 and consequently {(xn,yn)} is a Cauchy sequence which strongly converges to (x,y)ˆE׈E. As A,B,M,N,RMA,λ,ˆJMA,λ,CMA,λ are all continuous, the conclusion follows from Lemma 3.1. Hence, (x,y)ˆE׈E is the solution of our system (3.1).

    By using the altering points problem we obtain strong convergence of system of mixed generalized Cayley variational inclusions (3.1). We suggest general parallel S-iteration process for altering points problem associated with the system (3.1).

    Let D1(ϕ)ˆE and D2(ϕ)ˆE such that D1 and D2 are closed and convex. Let S1:D1D2, S2:D2D1 be mappings such that

    S1=RNB,ρ[RMA,λ+(λˆJMA,λρCNB,ρ(RNB,ρ))] (4.1)
    S2=RMA,λ[RNB,ρ+(ρˆJNB,ρλCMA,λ(RMA,λ))], (4.2)

    where λ,ρ>0 are constants. Using Lemma 3.1, it is clear that the system (3.1) is equivalent to following altering point problem:

    Find (x,y)D1×D2 satisfying

    {x=S2(y)=RNB,ρ[RMA,λ+(λˆJMA,λρCNB,ρ(RNB,ρ))](y)y=S1(x)=RMA,λ[RNB,ρ+(ρˆJNB,ρλCMA,λ(RMA,λ))](x). (4.3)

    We construct the general parallel S-iteration process to solve system (3.1).

    Parallel S-iteration process 4.1. For any given (x1,y1)D1×D2, let {(xn,yn)} be an iterative sequence in D1×D2 defined by

    xn+1=S2[(1αn)yn+αnS1(xn)]yn+1=S1[(1αn)xn+αnS2(yn)], (4.4)

    where {αn} is a sequence in [0,1]. The following result is needed in continuation.

    Theorem 4.1. Let ˆE be real uniformly smooth Banach space with modulus of smoothness τˆE(t)Ct2 for some C>0. Let A,B:ˆEˆE be single-valued mappings and M,N:ˆE2ˆE be multi-valued mappings such that A is δA-Lipschitz continuous and r1-strongly accretive maaping, B is δB-Lipschitz continuous and r2-strongly accretive maaping, M and N are A-accretive and B-accretive multi-valued mappings, respectively. Suppose that generalized resolvent operators RMA,λ and RNB,ρ are Lipschitz continuous with constants 1r1 and 1r2; generalized Yosida approximation operators ˆJMA,λ and ˆJNB,ρ are Lipschitz continuous with constant θ1 and θ1, and strongly accretive with constants θ2 and θ2, and generalized Cayley operators CMA,λ and CNB,ρ are Lipschitz continuous with constant θ3 and θ3 with 2θ2<1+64Cθ12 and 2θ2<1+64Cθ21, where θ1=δAr1+1λr1,θ1=δBr2+1ρr2, θ2=r211λr1,θ2=r221ρr2,θ3=2+δAr1r1 and θ3=2+δBr2r2, respectively. Then mappings S1 and S2 are Lipschitz continuous with constants Ω and Ω, respectively, where Ω=(1r1r2+ρr1+λθ3r21)+ρ(12θ2+64Cθ21)r1 and Ω=(1r1r2+λr2+ρθ3r22)+λ(12θ2+64Cθ21)r2.

    Proof. Let x,yˆE. Then, we have

    S1(x)S1(y)=RMA,λ[RNB,ρ+(ρˆJNB,ρλCMA,λ(RMA,λ))](x)RMA,λ[RNB,ρ+(ρˆJNB,ρλCMA,λ(RMA,λ))](y)1r1[RNB,ρ(x)+(ρˆJNB,ρ(x)λCMA,λ(RMA,λ(x)))][RNB,ρ(y)+(ρˆJNB,ρ(y)λCMA,λ(RMA,λ(y)))]1r1(RNB,ρ(x)RNB,ρ(y)+ρˆJNB,ρ(x)ˆJNB,ρ(y)+λCMA,λ(RMA,λ(x))CMA,λ(RMA,λ(y)))
    1r1(1r2xy+ρ(xy)(ˆJNB,ρ(x)ˆJNB,ρ(y))+ρxy+λθ3r1xy)(1r1r2+ρr1+λθ3r21)xy+ρr1(xy)(ˆJNB,ρ(x)ˆJNB,ρ(y)). (4.5)

    Using same arguments as used for (3.6), we obtain

    (xy)(ˆJNB,ρ(x)ˆJNB,ρ(y))2(12θ2+64Cθ12)xy2.

    Combining (4.5) and (4.6), we obtain

    S1(x)S1(y)[(1r1r2+ρr1+λθ3r21)+ρ(12θ2+64Cθ12)r1]xy.

    Hence S1 is Ω-Lipschitz continuous, where Ω=(1r1r2+ρr1+λθ3r21)+ρ(12θ2+64Cθ12)r1. In the same manner, it follows that S2 is Ω-Lipschitz continuous, where Ω=(1r1r2+λr2+ρθ3r22)+λ(12θ2+64Cθ21)r2.

    The convergence criteria is established for system (3.1) by applying general parallel S-iteration process.

    Theorem 4.2. Let D1 and D2 be same as in parallel S-iteration process (4.1). Let A,B,M,N, RMA,λ,ˆJMA,λ and CMA,λ be same as in Theorem 3.1 such that all the conditions of Theorem 3.1 are satisfied. Let S1 and S2 be same as in Theorem 4.1. Then (I) and (II) hold.

    (I) There exists a point (x,y)D1×D2, which solves altering point problem (4.3) associated with the system (3.1).

    (II) The sequence {(xn,yn)} generated by general parallel S-iteration process (4.4) converges strongly to point (x,y)D1×D2.

    Proof. (I). Applying Lemma 3.1 and (4.3), (I) follows.

    (II). Using parallel S-iteration process 4.1 and Theorem 4.1, we have

    yn+1y=S1[(1αn)xn+αnS2(yn)]S1(x)Ω[(1αn)xn+αnS2(yn)]xΩ((1αn)xnx+αnS2(yn)x)Ω((1αn)xnx+αnS2(yn)S2(y))Ω((1αn)xnx+αnΩyny)(1αn)Ωxnx+αnΩΩyny. (4.6)

    Similarly,

    xn+1x=S2[(1αn)yn+αnS1(xn)]S2(y)Ω[(1αn)yn+αnS1(xn)]yΩ((1αn)yny+αnS1(xn)y)Ω((1αn)yny+αnS1(xn)S1(x))Ω((1αn)yny+αnΩxnx)(1αn)Ωyny+αnΩΩxnx. (4.7)

    Combining (4.6) with (4.7), we have

    xn+1x+yn+1y(1αn)Ωxnx+αnΩΩyny+(1αn)Ωyny+αnΩΩxnxΩ{(1αn)xnxαnΩxnx}+Ω{(1αn)ynyαnΩyny}max{Ω,Ω}{(1αn)(xnx+yny)+αnmax{Ω,Ω}(xnx+yny)}Ω(1αn(1Ω))(xnx+yny), (4.8)

    where Ω=max{Ω,Ω}. The norm . on E×E is defined by (x,y)=x+y. Using (4.8), we have

    (xn+1,yn+1)(x,y)=(xn+1x,yn+1y)=(xn+1x+yn+1y)Ω(1αn(1Ω))(xn,yn)(x,y). (4.9)

    Since Ω(1αn(1Ω))Ω<1, we obtain that limn(xn,yn)(x,y)=0. Thus, we get limnxnx=limnyny=0 and hence the sequence {(xn,yn)} converges strongly to point (x,y).

    For illustration, we provide the following example. All codes are written in MATLAB R2019a.

    Example 5.1. Let ˆE=R,D1=[0,20], and D2=[0,23]. Let A,B:ˆEˆE and M,N:ˆE2ˆE be such that

    A(x)=65x,B(x)=43x,M(x)={110x},N(x)={15x}.

    Clearly, A is 1110-strongly accretive and 1310-Lipschtiz continuous mapping and B is 76-strongly accretive and 32-Lipschtiz continuous mapping and M and N are accretive mappings. For λ=1,[A+λM](ˆE)=ˆE and for ρ=1,[B+ρN](ˆE)=ˆE, the multi-valued mappings M and N are A-accretive and B-accretive mappings.

    The generalized resolvent operators, generalized Yosida approximation operators and generalized Cayley operators are defined below:

    RMA,λ(x)=[A+λM]1(x)=1013x,RNB,ρ(x)=[B+ρN]1(x)=1523x,JMA,λ(x)=1λ[ARMA,λ](x)=2865x,JNB,ρ(x)=1ρ[BRNB,ρ](x)=4769x,CMA,λ(x)=2RMA,λ(x)A(x)=2265x,CNB,ρ(x)=2RNB,ρ(x)B(x)=269x, for all xˆE.

    The above defined generalized resolvent operators RMA,λ and RNB,ρ are Lipschitz continuous with constants 1r1=1011 and 1r2=67, respectively, and generalized Yosida approximation operators JMA,λ and JNB,ρ are Lipschitz continuous with constants θ1=δAr1+1λr1=2210 and θ1=δBr2+1ρr2=3314, respectively and strongly accretive with constants θ2=r211λr1=19100 and θ2=r221ρr2=1342, respectively and generalized Cayley operators CMA,λ and CNB,ρ are Lipschitz continuous with constants θ3=2+δAr1r1=3110 and θ3=2+δBr2r2=4514, respectively.

    For λ=1 and ρ=1, we evaluate the mappings S1 and S2 such that

    S1(x)=RMA,λ[RNB,ρ+(ρJNB,ρλCMA,λRMA,λ)](x)=0.8254x,S2(x)=RNB,ρ[RMA,λ+(λJMA,λρCNB,ρRNB,ρ)](x)=0.8308x,

    which are Lipschitz continuous with constants 15 and 19, respectively.

    Also, the conditions considered in Theorem 3.1,

    |λr1r2(r1ρ)r1θ3r2|<ρ2r21(12θ2+64Cθ12)θ23 and |ρr1r2(r2λ)r2θ3r1|<λ2r22(12θ2+64Cθ21)θ23,

    r1,r2>1,2θ2<1+64Cθ12and2θ2<1+64Cθ21 are satisfied for all the values considered above. Thus, Theorem 3.1 is satisfied.

    For arbitrary x1D1 and y1D2, the common terms of {xn} and {yn} produced by process 3.1 are given by

    xn+1=(1αn)xn+αnRMA,λ[RNB,ρ(yn)+(ρJNB,ρ(yn)λCMA,λ(RMA,λ(yn)))]=xnn+1+n(0.8254)ynn+1,yn+1=(1αn)yn+αnRNB,ρ[RMA,λ(xn)+(λJMA,λ(xn)ρCNB,ρ(RNB,ρ(xn)))]=ynn+1+n(0.8308)xnn+1.

    Hence,

    xn+1=xnn+1+n(0.8254)ynn+1,yn+1=ynn+1+n(0.8308)xnn+1.

    For arbitrary x1D1 and y1D2, the common terms of {xn} and {yn} produced by process 4.1 are given by

    xn+1=S2[(1αn)yn+αnS1(xn)]=(0.8308)ynn+1+n(0.6857)xnn+1,yn+1=S1[(1αn)xn+αnS2(yn)]=(0.8254)xnn+1+n(0.6857)ynn+1.

    Hence,

    xn+1=(0.8308)ynn+1+n(0.6857)xnn+1,yn+1=(0.8254)xnn+1+n(0.6857)ynn+1.

    Taking different initial values x1=3,y1=3,x1=5 and y1=7, the sequences {xn} and {yn} converge to the unique solution (x,y)=(0,0) of system (3.1).

    In Table 1, we compare both the processes under consideration for x=3,x=3. Convergence of parallel Mann iteration process for different initial values of x is shown in Figure 1. In Table 2, comparison of parallel Mann iteration process and parallel S-iteration process for x=5 and x=7 is shown and in Figure 2, convergence of parallel S-iteration process is shown for different initial values of x. In all cases, the iteration process will terminate for xn+1xn105 and yn+1yn105.

    Table 1.  Comparison table: For initial values x1=3 and y1=3.
    No. of iterations Parallel Mann iteration process Parallel S-iteration process
    (n) xn yn xn yn
    1 3 -3 3 -3
    2 2.05722 -2.05722 0.90219 -0.90219
    3 1.41072 -1.41073 0.27131 -0.27131
    4 0.96739 -0.96739 0.08159 -0.08159
    5 0.66338 -0.66338 0.02453 -0.02453
    6 0.45491 -0.45491 0.00737 -0.00737
    7 0.31195 -0.31195 0.00221 -0.00221
    8 0.21391 -0.21391 0.00066 -0.00066
    9 0.14669 -0.14669 0.00020 -0.00020
    10 0.10059 -0.10059 0.00006 -0.00006
    13 0.03244 -0.03243 0 0
    16 0.01046 -0.01046 0 0
    20 0.00231 -0.00231 0 0
    23 0.00074 -0.00074 0 0
    26 0 0 0 0
    27 0 0 0 0

     | Show Table
    DownLoad: CSV
    Figure 1.  Convergence graph of {xn} and {yn} produced by parallel Mann iteration process (3.3) taking different initial values.
    Table 2.  Comparison table: For initial values x1=5 and y1=7.
    No. of iterations Parallel Mann iteration process Parallel S-iteration process
    (n) xn yn xn yn
    1 5 -7 5 -7
    2 3.42871 -4.80019 1.50366 -2.10512
    3 2.35121 -3.29169 0.45219 -0.63307
    4 1.61232 -2.25725 0.13599 -0.19038
    5 1.10564 -1.54789 0.04089 -0.05725
    6 0.75818 -1.06145 0.01229 -0.01721
    7 0.51991 -0.72788 0.00369 -0.00517
    8 0.35653 -0.49914 0.00111 -0.00155
    9 0.24448 -0.34228 0.00033 -0.00046
    10 0.16765 -0.23471 0.00010 -0.00014
    13 0.05406 -0.07568 0 0
    16 0.01743 -0.02441 0 0
    20 0.00385 -0.00539 0 0
    23 0.00124 -0.00174 0 0
    26 0.00040 -0.00056 0 0
    30 0 0 0 0

     | Show Table
    DownLoad: CSV
    Figure 2.  Convergence graph of {xn} and {yn} produced by parallel S-iteration process (4.4) taking different initial values.

    The general parallel S-iteration process is established to discuss the convergence criteria for the problem (3.1). We apply parallel Mann iteration process to obtain the solution of our system. We provide a numerical example applying Matlab program.

    Further, we remark that our result can be extended in other higher dimensional spaces.

    The authors declare that they have no conflict of interest.



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