Regarding the Hausdorff measure of noncompactness, we provide and demonstrate a generalization of Petryshyn's fixed point theorem in Banach algebras. Comparing this theorem to Schauder and Darbo's fixed point theorems, we can skip demonstrating closed, convex and compactness properties of the investigated operators. We employ our fixed point theorem to provide the existence findings for the product of n-nonlinear integral equations in the Banach algebra of continuous functions C(Ia), which is a generalization of various types of integral equations in the literature. Lastly, a few specific instances and informative examples are provided. Our findings can successfully be extended to several Banach algebras, including AC,C1 or BV-spaces.
Citation: Ateq Alsaadi, Manochehr Kazemi, Mohamed M. A. Metwali. On generalization of Petryshyn's fixed point theorem and its application to the product of n-nonlinear integral equations[J]. AIMS Mathematics, 2023, 8(12): 30562-30573. doi: 10.3934/math.20231562
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Regarding the Hausdorff measure of noncompactness, we provide and demonstrate a generalization of Petryshyn's fixed point theorem in Banach algebras. Comparing this theorem to Schauder and Darbo's fixed point theorems, we can skip demonstrating closed, convex and compactness properties of the investigated operators. We employ our fixed point theorem to provide the existence findings for the product of n-nonlinear integral equations in the Banach algebra of continuous functions C(Ia), which is a generalization of various types of integral equations in the literature. Lastly, a few specific instances and informative examples are provided. Our findings can successfully be extended to several Banach algebras, including AC,C1 or BV-spaces.
Different types of integral equations are crucial to the study of economics, biology, mechanics, mathematical physics, control theory, vehicular traffic, population dynamics and other fields (cf. [1,2]).
Recent years have seen some successful attempts to examine the qualitative behavior of solutions for many different types of nonlinear differential or integral equations employing the notion of the measure of noncompactness (M.N.C.) connected to the fixed point approach (F.P.T.) (cf. [3,4,5,6,7,8,9,10]).
Based on this methodology, we first offer and demonstrate a generalization of Petryshyn's F.P.T. connected with the Hausdorff M.N.C., which is a generalization of numerous F.P.T. types, including Darbo's, Schauder's and traditional Petryshyn's F.P.T.s [11]. The benefit of the proposed F.P.T. is that it enables us to skip demonstrating closed, convex and compactness properties of the investigated operators. These enable us to investigate various varieties of differential and integral equations under a weaker and more general set of presumptions.
Second, we employ the presented F.P.T. to solve the product of n-nonlinear Volterra integral equations, which are a generalization of the classical and quadratic integral equations of the form
z(v)=n∏i=1fi(v,z(αi(v)),z(βi(v)),∫φi(v)0hi(v,s,z(γi(s)))ds),v∈Ia=[0,a] | (1.1) |
for n≥2, in the Banach algebra C(Ia).
In particular, for n=2,fi(v,z1,z2,z3)=gi+z3,hi=li(v−s)z3(s), equation (1.1) yields a Gripenberg equation
z(v)=k(g1(v)+∫v0l1(v−s)z(s)ds)(g2(v)+∫v0l2(φ−s)z(s)ds), |
that has significant applications in biology (SI models, cf. [12]).
In [13] the authors utilized the F.P.T. approach to establish the existence of C[a,b]-solutions of the equation
z(v)=n∏i=1(hi(v)+∫vaKi(v,s,z(s))ds),v∈[a,b]. |
The authors in [14] presented an extension of Darbo F.P.T. in Banach algebra to solve the q-integral equation
z(v)=n∏i=1(hi(v)+gi(v,z(v))Γq(αi)∫va(v−qs)αi−1ui(s,z(s))ds),v∈[0,1]. |
A generalization of Darbo F.P.T. was used to investigate the existence results for the equation
z(v)=n∏i=1(hi(v)+λi⋅∫baKi(v,s)fi(s,z(s))ds),v∈[a,b] |
in ideal spaces (not be Banach algebras) in [15] see also [16,17,18].
We focus on applying a generalization of Petryshyn's F.P.T. to solve a general form of product-type integral problems in the Banach algebra C(Ia).
We employ the following symbols in the sequel:
● E: Banach space;
● ¯Br: A ball of radius r and center at 0;
● ∂ˉBr: Sphere in E with radius r>0 around 0;
● C(Ia): Space of continuous and real-valued functions on Ia=[0,a];
● (F.P.T.): Fixed point theorem;
● (M.N.C.): Measure of noncompactness.
We recall some theorems & definitions that are required for the sequel.
Definition 2.1. [19] Let Z⊂E be a bounded set, then
α(Z)=inf{ρ>0:∃afinitenumberofsetsofdiameter≤ρthatcancoverZ} |
is said to be the Kuratowski M.N.C.
Definition 2.2. [20] Let Z⊂E be a bounded set, then
μ(Z)=inf{ρ>0:Zhasafiniteρ−netinE} |
is said to be the Hausdorff M.N.C.
Theorem 2.3. [20] For a bounded set Z⊂E, the M.N.C.s α and μ fulfill
μ(Z)≤α(Z)≤2μ(Z). |
For more information about the properties of the M.N.C. see [11,20].
The space C[0,a] yields to a Banach space under the norm ‖z‖=sup{|z(v)|:v∈Ia} and we shall write the modulus of continuity of a function z∈C(Ia) as
ω(z,ρ)=sup{|z(v)−z(s)|:|v−s|≤ρ}. |
Theorem 2.4. [20] For a bounded set Z⊂C(Ia), the M.N.C. in C(Ia) is denoted by
μ(Z)=limρ→0supz∈Zω(z,ρ). | (2.1) |
Definition 2.5. [21] Let P:E→E be a continuous map. P is said to be a contraction map if for all Z⊂C(Ia) be bounded, P(Z) be bounded and
α(PZ)≤kα(Z),0<k<1. |
Moreover, P is said to be condensing (densifying) map if
α(PZ)<α(Z). |
Note that a contraction map yields condensing (densifying) but not vice versa.
Remark 2.6. In C(Ia), the M.N.C. μ fulfills condition (m) (cf. [22]) and its generalization for a finite sequence of bounded sets {Ni}i=1,...,n, n≥2 (cf. [14]) i.e.
μ(n∏i=1Ni)≤n∑i=1n∏j=1,j≠i‖Nj‖⋅μ(Ni). |
In order to solve Eq (1.1), we first give a fixed point z∈ˉBr of the problem
z=Pz=n∏i=1Piz, | (3.1) |
where Pi:ˉBr→E,i=1,⋯,n,n≥2 are known operators.
Definition 2.5 should be rewritten in view of the M.N.C. μ in C(Ia).
Definition 3.1. The operator P:C(Ia)→C(Ia) is said to be a contraction map if for all Z⊂C(Ia) be bounded set, P(Z) be bounded set and
μ(PZ)≤2kμ(Z),0<k<12. |
Moreover, P is said to be condensing (densifying) map if
μ(PZ)<μ(Z). |
Proof. Since Z and P(Z) are bounded sets in C(Ia) and by using Theorem 2.3, we have
μ(PZ)≤α(PZ)≤kα(Z)≤2kμ(Z)⇒μ(PZ)≤2kμ(Z). |
The above inequality with 0<k<12 finishes the proof.
Note that a contraction map related to the M.N.C. μ yields condensing (densifying) with 0<k<12 but not vice versa.
The following Proposition can be presented and proven by us.
Proposition 3.2. Suppose that the operators Pi:ˉBr→E,i=1,⋯n and that:
(B1) Pi are continuous on ˉBr,i=1,⋯n.
(B2) There exist ki>0 such that Pi fulfill:
μ(Pi(Z))≤ki μ(Z),i=1,⋯n |
for arbitrary bounded Z⊂E,
(B3) K=∑ni=1ki∏nj=1,j≠i‖PjˉBr‖<12,
(B4) P(z)=kz, for some z∈∂ˉBr then k≤1,
then the set Fix(P) of fixed points of P in ˉBr is nonempty.
Proof. Let ∅≠Z⊂ˉBr. By utilizing the above assumptions, we obtain
μ(PZ)=μ(n∏i=1PiZ)≤n∑i=1n∏j=1,j≠i‖PjZ‖⋅μ(PiZ)≤n∑i=1kin∏j=1,j≠i‖PjZ‖⋅μ(Z)≤(n∑i=1kin∏j=1,j≠i‖PjˉBr‖)⋅μ(Z)=K⋅μ(Z). |
By using Petryshyn's F.P.T., we have finished.
Remark 3.3. ● If n=1, Proposition 3.2 reduces to classical Petryshyn's F.P.T. [11], which is a generalization of classical Darbo and Schauder F.P.Ts.
● If n=2, Proposition 3.2 reduces to the F.P.T. presented in [11,21], which is a generalization of the results presented in [22].
● If n≥2, Proposition 3.2 is a general form of the F.P.T. presented in [14,15].
Now, we will apply Proposition 3.2 to check the solvability of Eq. (1.1) under the assumptions:
(A1) Assume that αi,βi,γi:Ia→Ia and φi:Ia→R+ are continuous s.t. φi(v)≤B, for i=1,⋯,n and B≥0,v∈Ia.
(A2) The functions hi∈C(Ia×[0,B]×R,R) and fi∈C(Ia×R×R×R,R), where there exist constants ki>0, s.t.
|fi(v,Ω1,Ω2,Ω3)−fi(v,ˉΩ1,ˉΩ2,ˉΩ3)|≤ki(|Ω1−ˉΩ1|+|Ω2−ˉΩ2|+|Ω3−ˉΩ3|),i=1,⋯,n. |
(A3) There exists Mi≥0 and r0≥0 such that
sup{|n∏i=1fi(v,Ω1,Ω2,Ω3)|:v∈Ia,|Ωj|≤r0,j=1,2,|Ω3|≤n∏i=1BMi,i=1,⋯,n}≤r0, |
where
Mi=sup{|hi(v,s,z)|;∀v∈Ia,s∈[0,B],z∈[−r0,r0]}. |
(A4) K=∑ni=12ki∏nj=1,j≠i‖fj‖<12.
Theorem 3.4. Under the tacit assumption (A1)–(A4) above, Eq. (1.1) has at least one solution in C(Ia).
Proof. First, let us define the operators Pi:Br0→C(Ia), as follows
Pz(v)=n∏i=1Piz(v)=n∏i=1fi(v,z(αi(v)),z(βi(v)),∫φi(v)0hi(v,s,z(γi(s)))ds),v∈Ia. | (3.2) |
Next, we will divide the proof into some steps according to Proposition 3.2. Step 1. The operator P is well defined on C(Ia). Obviously from assumptions (A1) and (A2), we have P:C(Ia)→C(Ia).
Step 2. We will demonstrate that the operators P,Pi,i=1,⋯,n are continuous on the ball Br0.
Take arbitrary z,y∈Br0 and ε>0 s.t. ‖z−y‖≤ε, then for v∈Ia, we obtain
|(Piz)(v)−(Piy)(v)|=|fi(v,z(αi(v)),z(βi(v)),∫φi(v)0hi(v,s,z(γi(s)))ds)−fi(v,y(αi(v)),y(βi(v)),∫φi(v)0hi(v,s,y(γi(s)))ds)|≤|fi(v,z(αi(v)),z(βi(v)),∫φi(v)0hi(v,s,z(γi(s)))ds)−fi(v,y(αi(v)),z(βi(v)),∫φi(v)0hi(v,s,z(γi(s)))ds)|+|fi(v,y(αi(v)),z(βi(v)),∫φi(v)0hi(v,s,z(γi(s)))ds)−fi(v,y(αi(v)),y(βi(v)),∫φi(v)0hi(v,s,z(γi(s)))ds)|+|fi(v,y(αi(v)),y(βi(v)),∫φi(v)0hi(v,s,z(γi(s)))ds)−fi(v,y(αi(v)),y(βi(v)),∫φi(v)0hi(v,s,y(γi(s)))ds)|≤ki|z(αi(v))−y(αi(v))|+ki|z(βi(v))−y(βi(v))|+ki∫φi(v)0|hi(v,s,z(γi(s)))−hi(v,s,y(γ1(s)))|ds≤2ki‖z−y‖+kiB⋅ω(hi,ε), |
where ω(hi,ε)=sup{|hi(v,s,z)−hi(v,s,y)|:v∈Ia,s∈[0,B],z,y∈[−r0,r0],‖z−y‖≤ε}.
From assumption (A2), the functions hi=hi(v,s,z) are uniformly continuous on [0,a]×[0,B]×R, we indicate that ω(hi,ε)→0 as ε→0. Thus, the operators Pi,i=1,⋯,n are continuous on Br0 and consequently, the operator P=∏ni=1Pi is continuous on Br0.
Step 3. We will demonstrate that the operator P fulfills the densifying condition in view of μ.
Take arbitrary ρ>0 and z∈M⊂C(Ia) is bounded set and for v1,v2∈Ia s.t. v1≤v2 with v2−v1≤ρ, we obtain
|(Piz)(v2)−(Piz)(v1)|=|fi(v2,z(αi(v2)),z(βi(v2)),∫φi(v2)0hi(v2,s,z(γi(s)))ds)−fi(v1,z(αi(v1)),z(βi(v1)),∫φi(v1)0hi(v1,s,z(γi(s)))ds)|≤|fi(v2,z(αi(v2)),z(βi(v2)),∫φi(v2)0hi(v2,s,z(γi(s)))ds)−fi(v2,z(αi(v2)),z(βi(v2)),∫φi(v1)0hi(v1,s,z(γi(s)))ds)|+|fi(v2,z(αi(v2)),z(βi(v2)),∫φi(v1)0hi(ti,s,z(γi(s)))ds)−fi(v2,z(αi(v2)),z(βi(v1)),∫φi(v1)0hi(v1,s,z(γi(s)))ds)|+|fi(v2,z(αi(v2)),z(βi(v1)),∫φi(v1)0hi(v1,s,z(γi(s)))ds)−fi(v2,z(αi(v1)),z(βi(v1)),∫φi(v1)0hi(v1,s,z(γi(s)))ds)|+|fi(v2,z(αi(v1)),z(βi(v1)),∫φi(v1)0hi(v1,s,z(γi(s)))ds)−fi(v1,z(αi(v1)),z(βi(v1)),∫φi(v1)0hi(v1,s,z(γi(s)))ds)|≤ki|∫φi(v2)0hi(v2,s,z(γi(s)))ds−∫φi(v1)0hi(v1,s,z(γi(s)))ds|+ki|z(βi(v2))−z(βi(v1))|+ki|z(αi(v2))−z(αi(v1))|+ωifi(Ia,ρ)≤ki|∫φi(v1)0ωihi(Ia,ρ)ds+∫φi(v2)φi(v1)hi(v2,s,z(γi(s)))ds|+kiω(z,ω(βi,ρ))+kiω(z,ω(αi,ρ))+ωifi(Ia,ρ), |
where
ωihi(Ia,ρ)=sup{|hi(v,s,z)−hi(ˉv,s,z)|:|v−ˉv|≤ρ,v∈Ia,s∈[0,B],z∈[−r0,r0]}, |
ωifi(Ia,ρ)=sup{|fi(v,z1,z2,z3)−fi(ˉv,z1,z2,z3)|:|v−ˉv|≤ρ,v∈Ia,z1,z2∈[−r0,r0],z3∈[−BMi,BMi]} |
and
Mi=sup{|hi(v,s,z)|:v∈Ia,s∈[0,B],z∈[−r0,r0]}. |
From the above relations we get
|(Piz)(v)−(Piy)(v)|≤kiBωihi(Ia,ρ)+kiMiω(φi,ρ)+kiω(z,ω(βi,ρ))+kiω(z,ω(αi,ρ))+ωifi(Ia,ρ). |
Let ρ→0, we get
ω(Piz,ρ)≤2kiω(z,ρ). |
This yields the following estimation:
μ(PiM)≤2kiμ(M). |
Therefore,
μ(PM)=μ(n∏i=1PiM)≤K=(n∑i=12kin∏j=1,j≠i‖fj‖)μ(M). |
From assumption (A4), we get P is a condensing map with K<12.
Step 4. We will demonstrate assumption (B4) of Proposition 3.2.
Suppose z∈∂ˉBr0. If Tz=kz then we get kr0=k‖z‖=‖Pz‖ and by (H3) we have
|Pz(v)|=|n∏i=1Piz(v)|=|n∏i=1fi(v,z(αi(v)),z(βi(v)),∫φi(v)0hi(v,s,z(γi(s)))ds)|≤r0, |
for all v∈Ia, hence ‖Pz‖≤r0, so this shows k≤1.
Step 5. The proof is completed when Proposition 3.2 is applied.
To demonstrate the value of our results, we provide a few examples and instances of integral equations.
● If n=2,f1(v,Ω1,Ω2,Ω3)=f(v,Ω1)+p(v,Ω1,Ω3),α1(v)=φ1(v)=v,f2(v,Ω1,Ω2,Ω3)=q(v,Ω1,Ω3),φ2(v)=a, then we have
z(v)=(f(v,z(v))+p(v,z(β1(v)),∫v0h1(v,s,z(γ1(s)))ds)×q(v,z(α2(v)),∫a0h2(v,s,z(γ2(s)))ds), |
which was inspected in [23].
● For n=2,fi(v,Ω1,Ω2,Ω3)=pi(v,Ω1,Ω3),γ1(v)=γ2(v)=φ1(v)=v,φ2(v)=a, we have
z(v)=p1(v,z(α1(v)),∫v0h1(v,s,z(s)ds)×p2(v,z(α2(v)),∫a0h2(v,s,z(s))ds), |
which was inspected in [24,25].
● If n=2,fI(v,Ω1,Ω2,Ω3)=pi(v,Ω1,Ω3),φ2(v)=1 then we get
z(v)=p1(v,z(α1(v)),∫φ1(v)0h1(v,s,z(γ1(s)))ds)×p2(v,z(α2(v)),∫10h2(v,s,z(γ2(s)))ds), |
which was inspected in [26,27].
● If n=2,f1(v,Ω1,Ω2,Ω31)=a(v)⋅Ω31,f2(v,Ω1,Ω2,Ω32)=Ω31⋅Ω32,αi(v)=φ1(v)=γi(v)=γ2(v)=v,φ2(v)=a, then we get
z(v)=a(v)∫a0h2(v,s,z(s))ds+(∫v0h1(v,s,z(s))ds)(∫a0h2(v,s,z(s))ds), |
which was inspected in [28].
Example 4.1. Consider the integral equation in C[0,1]
z(v)=(v215(1+v2)sin(|z(v)|)+12ln(1+|z(√v)|)+14∫√v0ssin(z(√s))1+s+evds)×(e−v(z(v)+2z(1−v))6+v+18+v∫12v0v(1+arctan(z(s2)1+z(s2)))2+sds)×(v4e−vz(12v)3+12+ln(1+s)+ev∫v30se−2tz(s)2+|cos(z(s))|ds)v∈[0,1]. | (4.1) |
Equation (4.1) is a particular form of Eq (1.1) such that:
αi(v)=v,i=1,2,α3(v)=v2v,β1(v)=√v,β2(v)=1−v,β3(v)=v,γ1(v)=√v,γ2(v)=v2,γ3=vφ1(v)=√v,φ2(v)=v2,φ3(v)=v3, |
● f1(v,z(α1(v)),z(β1(v)),W1)=v215(1+v2)sin(|z(v)|)+12ln(1+|z(√v)|)+14W1,W1=∫√v0ssin(z(√s))1+s+evds,
● f2(v,z(α2(v)),z(β2(v)),W2)=e−v(z(v)+2z(1−v))6+v+18+vW2,W2=∫12v0v(1+arctan(z(s2)1+z(s2)))2+sds,
● f3(v,z(α2(v)),z(β2(v)),W3)=v4e−vz(12v)3+12+ln(1+s)+evW3,W3=∫v30se−2tz(s)2+|cos(z(s))|ds.
It can be seen that
|f1(v,Ω1,Ω2,Ω3)−f1(v,ˉΩ1,ˉΩ2,ˉΩ3)|≤12(|Ω1−ˉΩ1|+|Ω2−ˉΩ2|+|Ω3−¯3|), |
|f2(v,Ω1,Ω2,Ω3)−f2(v,ˉΩ1,ˉΩ2,ˉΩ3)|≤13(|Ω1−ˉΩ1|+|Ω2−ˉΩ2|+|Ω3−ˉΩ3|), |
|f3(v,Ω1,Ω2,Ω3)−f3(v,ˉΩ1,ˉΩ2,ˉΩ3)|≤13(|Ω1−ˉΩ1|+|Ω2−ˉΩ2|+|Ω3−ˉΩ3|). |
So we can choose
k1=12,k2=13,k3=13 |
and so the conditions (A1) and (A2) hold. Moreover, for ‖z‖≤r0, we get
|z(v)|≤|f1(v,z(α1(v)),z(β1(v)),W1)|⋅|f2(v,z(α2(v)),z(β2(v)),W2)|⋅|f3(v,z(α3(v)),z(β3(v)),W3)|≤(115+12r0+14)(12r0+(1+r0)16)(13r0+14r0)≤r0. |
This shows that r0≤2.1104. Also, for r0∈[0,0.64368]⊂[0,2.1104] we have
K=2k1(‖f2‖⋅‖f3‖)+2k2(‖f1‖⋅‖f3‖)+2k3(‖f1‖⋅‖f2‖)<12. |
Therefore, assumptions (A1)–(A4) be fulfilled and Theorem 3.4 indicates the solution of (4.1) in C[0,1].
Example 4.2. Consider the integral equation in C[0,1]
z(v)=(12ve−v+cos(z(v3))8+18sin(z(√v)2+v)+18+v2∫v0(√1+2|z(√s)|+ts2)cos(s)4+3√sds)×(19vcos(z(v))+tz(√v)9(1+z(√v))+19(ev+3t4)∫√v0(1+cos(√s))(√1+2|z(√s)|)1+stln(1+s)ds). | (4.2) |
● Here α1(v)=v3,α2(v)=√v,β1(v)=β2(v)=√v,γ1(v)=γ2(v)=√v,,φ1(v)=√v,φ2(v)=√v,
● f1(v,z(α1(v)),z(β1(v)),W1)=12ve−v+cos(z(v3))8+18sin(z(√v)2+v)+18+v2W1,
● f2(v,z(α2(v)),z(β2(v)),W2)=19vcos(z(v))+tz(√v)9(1+z(√v))+19(ev+3t4)W2,
● W1=∫v0(√1+2|z(√s)|+ts2)cos(s)4+3√sds,W2=∫√v0(1+cos(√s))(√1+2|z(√s)|)1+stln(1+s)ds.
It can be seen that
|f1(v,Ω1,Ω2,Ω3)−f1(v,ˉΩ1,ˉΩ2,ˉΩ3)|≤18(|Ω1−ˉΩ1|+|Ω2−ˉΩ2|+|Ω3−ˉΩ3|), |
|f2(v,Ω1,Ω2,Ω3)−f2(v,ˉΩ1,ˉΩ2,ˉΩ3)|≤19(|Ω1−ˉΩ1|+|Ω2−ˉΩ2|+|Ω3−ˉΩ3|). |
So we can choose
k1=18,k2=19 |
and so the conditions (A1) and (A2) hold. Moreover, for ‖z‖≤r0, we get
|z(v)|≤|f1(v,z(α1(v)),z(β1(v)),W1)|⋅|f2(v,z(α2(v)),z(β2(v)),W2)|≤(12+18+18+132(√1+2r0))(19+19+29(√1+2r0))≤r0 |
This shows that r0≥0.41410. Also, for r0∈[0.41410,9.3765] we have
K=2k1‖f2‖+2k2‖f1‖<12. |
Therefore, assumptions (A1)–(A4) be fulfilled and Theorem 3.4 indicates the solution of (4.1) in C[0,1].
In this article, a generalization of Petryshyn F.P.T. and the MNC idea were used to analyze the solutions for products of n-nonlinear integral equations in the Banach algebra C(Ia). The presented F.P.T. is a generalization of Darbo, Schauder and the classical Petryshyn F.P.T. Examples are provided to demonstrate the usefulness of our findings. The upcoming work in this field will consider different Banach algebras, including AC,C1 or BV spaces.
The authors declare that they have not used Artificial Intelligence (AI) tools in the creation of this article.
The authors declare that there are no conflicts of interest regarding the publication of this article.
The researchers would like to acknowledge the Deanship of Scientific Research, Taif University for funding this work.
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