
We focused on the analytical solution of strong nonlinearity and complicated time-fractional evolution equations, including the Sawada-Kotera equation, Ito equation, and Kaup-Kupershmidt equation, using an effective and accurate method known as the Aboodh residual power series method (ARPSM) in the framework of the Caputo operator. Therefore, the Caputo operator and the ARPSM are practical for figuring out a linear or nonlinear system with a fractional derivative. This technique was effectively proposed to obtain a set of analytical solutions for various types of fractional differential equations. The derived solutions enabled us to understand the mechanisms behind the propagation and generation of numerous nonlinear phenomena observed in diverse scientific domains, including plasma physics, fluid physics, and optical fibers. The fractional property also revealed some ambiguity that may be observed in many natural phenomena, and this is one of the most important distinguishing factors between fractional differential equations and non-fractional ones. We also helped clarify fractional calculus in nonlinear dynamics, motivating researchers to work in mathematical physics.
Citation: Humaira Yasmin, Aljawhara H. Almuqrin. Efficient solutions for time fractional Sawada-Kotera, Ito, and Kaup-Kupershmidt equations using an analytical technique[J]. AIMS Mathematics, 2024, 9(8): 20441-20466. doi: 10.3934/math.2024994
[1] | Tatjana Došenović, Dušan Rakić, Stojan Radenović, Biljana Carić . Ćirić type nonunique fixed point theorems in the frame of fuzzy metric spaces. AIMS Mathematics, 2023, 8(1): 2154-2167. doi: 10.3934/math.2023111 |
[2] | Ying Chang, Hongyan Guan . Generalized (αs,ξ,ℏ,τ)-Geraghty contractive mappings and common fixed point results in partial b-metric spaces. AIMS Mathematics, 2024, 9(7): 19299-19331. doi: 10.3934/math.2024940 |
[3] | Shaoyuan Xu, Yan Han, Suzana Aleksić, Stojan Radenović . Fixed point results for nonlinear contractions of Perov type in abstract metric spaces with applications. AIMS Mathematics, 2022, 7(8): 14895-14921. doi: 10.3934/math.2022817 |
[4] | Nihal Taş, Irshad Ayoob, Nabil Mlaiki . Some common fixed-point and fixed-figure results with a function family on Sb-metric spaces. AIMS Mathematics, 2023, 8(6): 13050-13065. doi: 10.3934/math.2023657 |
[5] | Sourav Shil, Hemant Kumar Nashine . Positive definite solution of non-linear matrix equations through fixed point technique. AIMS Mathematics, 2022, 7(4): 6259-6281. doi: 10.3934/math.2022348 |
[6] | Umar Ishtiaq, Fahad Jahangeer, Doha A. Kattan, Manuel De la Sen . Generalized common best proximity point results in fuzzy multiplicative metric spaces. AIMS Mathematics, 2023, 8(11): 25454-25476. doi: 10.3934/math.20231299 |
[7] | Mi Zhou, Naeem Saleem, Xiao-lan Liu, Nihal Özgür . On two new contractions and discontinuity on fixed points. AIMS Mathematics, 2022, 7(2): 1628-1663. doi: 10.3934/math.2022095 |
[8] | Nosheen Zikria, Aiman Mukheimer, Maria Samreen, Tayyab Kamran, Hassen Aydi, Kamal Abodayeh . Periodic and fixed points for F-type contractions in b-gauge spaces. AIMS Mathematics, 2022, 7(10): 18393-18415. doi: 10.3934/math.20221013 |
[9] | Aftab Hussain . Fractional convex type contraction with solution of fractional differential equation. AIMS Mathematics, 2020, 5(5): 5364-5380. doi: 10.3934/math.2020344 |
[10] | Fatima M. Azmi . New fixed point results in double controlled metric type spaces with applications. AIMS Mathematics, 2023, 8(1): 1592-1609. doi: 10.3934/math.2023080 |
We focused on the analytical solution of strong nonlinearity and complicated time-fractional evolution equations, including the Sawada-Kotera equation, Ito equation, and Kaup-Kupershmidt equation, using an effective and accurate method known as the Aboodh residual power series method (ARPSM) in the framework of the Caputo operator. Therefore, the Caputo operator and the ARPSM are practical for figuring out a linear or nonlinear system with a fractional derivative. This technique was effectively proposed to obtain a set of analytical solutions for various types of fractional differential equations. The derived solutions enabled us to understand the mechanisms behind the propagation and generation of numerous nonlinear phenomena observed in diverse scientific domains, including plasma physics, fluid physics, and optical fibers. The fractional property also revealed some ambiguity that may be observed in many natural phenomena, and this is one of the most important distinguishing factors between fractional differential equations and non-fractional ones. We also helped clarify fractional calculus in nonlinear dynamics, motivating researchers to work in mathematical physics.
Many real-world problems have a need to find a distance connecting two or more items that may not be easy to measure accurately. Consequently, to model distinct problems of practical nature, we require an appropriate metric. There exist several approaches to measure the distance more precisely which are being utilized to widen the extent of the investigation of fixed point theory. Non-unique and unique fixed point conclusions have been widely investigated with a different outlook via distinct metrics in the theory of fixed points (for instance, [1,2,7,8,9,10,24,36,42,43,44,45,46] and so on). Recently, the geometry of the collection of fixed points has been considered in various forms, such as the fixed circle problem, fixed disc problem, fixed ellipse problem, fixed elliptic disc problem and so on. The most general form of these problems is the "fixed figure problem."
In the current work, we introduce an M−class function to establish a unique fixed point and fixed circle via the S−metric introduced by Sedghi et al. [37]. Further, we investigate the notion of a fixed ellipse (elliptic disc) in an S−metric space to conclude that the set of fixed points incorporates an ellipse (elliptic disc) under appropriate conditions and verify this by illustrative examples. In the sequel, we explore some conditions which eliminate the possibility of the identity map in the existence of an ellipse (elliptic disc) in an S−metric space. Further, we give propositions for the existence of a self-map that fixes the given ellipse (elliptic disc) and demonstrate that an ellipse (elliptic disc) contains all the points of space except its foci. It is fascinating to mention that the uniqueness of a fixed ellipse, as well as the existence of the greatest fixed elliptic disc, may be established using celebrated contractive conditions like Banach contraction [4], Ćirić contraction [8], Quasi contraction [9], Rhoades contraction [35] and so on. These fixed ellipse (elliptic disc) conclusions encourage further investigations and implementations in S−metric spaces. It is significant to mention that the collection of fixed points carries out a significant role in the theory of fixed points and may form some geometrical shapes like circles, discs, ellipses or elliptic discs. In particular, the ellipse has numerous applications in Physics, Astronomy, Neural Networks, Biology, Artificial Intelligence, Economics and so on.
Definition 2.1. [37] An S−metric on a non-empty set U is a function S:U×U×U⟶R+ so that
(S1) S(ω,υ,u)≥0;
(S2) S(ω,υ,u)=0 iff ω=υ=u;
(S3) S(ω,υ,u)≤S(ω,ω,α)+S(υ,υ,α)+S(u,u,α),ω,υ,u,α∈U.
Geometrically, we connect three points ω,υ and u to get a triangle, and if α is a point mediating this triangle, then (S3) holds.
Remark 2.1. [37] In an S−metric space S(ω,ω,υ)=S(υ,υ,ω).
Definition 2.2. [37] Let {ωn} be a sequence in an S−metric space (U,S). Then,
(1) {ωn} is convergent to ω∈U if limn→∞S(ωn,ωn,ω)=0;
(2) {ωn} is a Cauchy sequence if limn,m→∞S(ωn,ωn,ωm)=0,n,m>N;
(3) (S,U) is complete if every Cauchy sequence in U converges to a point in U.
Definition 2.3. [26] Let (S,U) be an S−metric space, and C(ω0,r)={ω∈U:S(ω,ω,ω0)=r,r>0} is a circle centered on ω0 with a radius r. For a self-map A:U→U, if Aω=ω,ω∈C(ω0,r), then C(ω0,r) is called a fixed circle of A.
First, we introduce an M−class function in an S−metric space which may be used as a tool to find a fixed point of contraction maps as well as explore its geometry. These functions also give the assurance of a fixed point, fixed circle (disc) and fixed ellipse (elliptic disc), and they unify, improve, extend and generalize numerous existing conclusions in the literature to S−metric spaces.
We denote a set of continuous functions f:[0,∞)5→[0,∞) by M, satisfying the following:
(f1) f(1,1,0,3,1)∈[0,1);
(f2) f is a linear homogeneous function, that is,
f(λω)=λf(ω)orf(λω1,λω2,λω3,λω4,λω5)=λf(ω1,ω2,ω3,ω4,ω5), |
where ω=(ω1,ω2,ω3,ω4,ω5)∈[0,∞)5, λ≥0;
(f3) f is a non-decreasing function, that is,
ω≤ν⇒fω≤fνorωi≤νi,i=1,2,…,5⇒f(ω1,ω2,ω3,ω4,ω5)≤f(υ1,υ2,υ3,υ4,υ5), |
where ω=(ω1,ω2,ω3,ω4,ω5) and υ=(υ1,υ2,υ3,υ4,υ5)∈[0,∞)5.
Then, function f is said to be an M-class function.
Example 3.1. Define f1:[0,∞)5→[0,∞) by f1(ω1,ω2,ω3,ω4,ω5)=αω1,α∈[0,1). Then, f1∈M.
Example 3.2. Define f2:[0,∞)5→[0,∞) by f2(ω1,ω2,ω3,ω4,ω5)=α(ω2+ω5),α∈[0,13). Then, f2∈M.
Example 3.3. Define f3:[0,∞)5→[0,∞) by f3(ω1,ω2,ω3,ω4,ω5)=αmax{ω2,ω5},α∈[0,13). Then, f3∈M.
Example 3.4. Define f4:[0,∞)5→[0,∞) by f4(ω1,ω2,ω3,ω4,ω5)=αω1+βω2+γω5,α+β+γ∈[0,1). Then, f4∈M.
Example 3.5. Define f5:[0,∞)5→[0,∞) by f4(ω1,ω2,ω3,ω4,ω5)=max{ω1,ω2,ω5}. Then, f5∈M.
Example 3.6. Define f6:[0,∞)5→[0,∞) by f4(ω1,ω2,ω3,ω4,ω5)=α(ω3+ω4),α∈[0,13). Then, f6∈M.
Example 3.7. Define f7:[0,∞)5→[0,∞) by f7(ω1,ω2,ω3,ω4,ω5)=αmax{ω3,ω4},α∈[0,13). Then, f7∈M.
Example 3.8. Define f8:[0,∞)5→[0,∞) by
f8(ω1,ω2,ω3,ω4,ω5)=αω1+βω2+γ(ω3+ω4)+δω5,α+β+3γ+δ∈[0,1). |
Then, f8∈M.
Example 3.9. Define f9:[0,∞)5→[0,∞) by
f9(ω1,ω2,ω3,ω4,ω5)=αmax{ω1,ω2,ω3,ω4,ω5},α∈[0,13). |
Then, f9∈M.
Lemma 3.10. If f∈M and ω,υ∈[0,∞) are such that
ω≤max{f(υ,ω,0,υ+2ω,ω),f(υ+2ω,ω,0,υ,υ),f(υ,υ+2ω,0,υ,ω),f(ω,υ,0,ω,υ+2ω)}, | (3.1) |
then ω≤ηυ, where η=f(1,1,0,3,1)∈[0,1).
Proof. We may presume without loss of generality that ω≤f(υ,ω,0,υ+2ω,ω). If υ<ω,
ω≤f(υ,ω,0,υ+2ω,ω)<f(ω,ω,0,3ω,ω)=ωf(1,1,0,3,1)≤ω, |
a contradiction. Thus, ω≤υ. Also,
ω≤f(υ,ω,0,υ+2ω,ω)<f(υ,υ,0,3υ,υ)=υf(1,1,0,3,1)=ηυ. |
Theorem 3.11. Let (U,S) be a complete S−metric space. For all ω≠υ∈U, f∈M and A:U→U, if S(Aω,Aω,Aυ)>0 implies
S(Aω,Aω,Aυ)≤f(S(ω,ω,υ),S(Aω,Aω,ω),S(Aω,Aω,υ),S(Aυ,Aυ,ω),S(Aυ,Aυ,υ)), | (3.2) |
then A has a unique fixed point.
Proof. For arbitrary ω0∈U, let ω1=Aω0. If ω1=Aω1, ω1 is a fixed point of A, and the proof is concluded. So, consider ω1≠Aω1 and ω2=Aω1. Consequently, S(Aω0,Aω0,Aω1)>0, and then, using inequality (3.2) for ω=ω0, υ=ω1 and properties of M−class function,
S(ω1,ω1,ω2)=S(Aω0,Aω0,Aω1)≤f(S(ω0,ω0,ω1),S(Aω0,Aω0,ω0),S(Aω0,Aω0,ω1),S(Aω1,Aω1,ω0),S(Aω1,Aω1,ω1))=f(S(ω0,ω0,ω1),S(ω1,ω1,ω0),S(ω1,ω1,ω1),S(ω2,ω2,ω0),S(ω2,ω2,ω1))=f(S(ω0,ω0,ω1),S(ω0,ω0,ω1),0,S(ω0,ω0,ω2),S(ω1,ω1,ω2))≤f(S(ω0,ω0,ω1),S(ω0,ω0,ω1),0,2S(ω0,ω0,ω1)+S(ω1,ω1,ω2),S(ω1,ω1,ω2)). |
Now, using Lemma 3.10, we have
S(ω1,ω1,ω2)≤ηS(ω0,ω0,ω1). | (3.3) |
Repeatedly, we get S(ω2,ω2,ω3)≤ηS(ω1,ω1,ω2)≤η2S(ω0,ω0,ω1).
Continuing like this,
S(ωn,ωn,ωn+1)≤ηS(ωn−1,ωn−1,ωn)≤⋯≤ηnS(ω0,ω0,ω1). |
Now, define a Picard sequence ωn+1=Aωn,n∈N∪{0}, with initial point ωo∈U. If for some n∈N, ωn=ωn+1=Aωn, then ωn is a fixed point of A, and the proof is complete. So, presume that ωn≠ωn+1, for all n∈N∪{0}. By using (S3),
S(ωn,ωn,ωn+m)≤2S(ωn,ωn,ωn+1)+S(ωn+m,ωn+m,ωn+1)=2S(ωn,ωn,ωn+1)+S(ωn+1,ωn+1,ωn+m)≤2S(ωn,ωn,ωn+1)+2S(ωn+1,ωn+1,ωn+2)+S(ωn+m,ωn+m,ωn+2)≤2S(ωn,ωn,ωn+1)+2S(ωn+1,ωn+1,ωn+2)+⋯+S(ωn+m,ωn+m,ωn+m−1)≤2[S(ωn,ωn,ωn+1)+S(ωn+1,ωn+1,ωn+2)+⋯+S(ωn+m−1,ωn+m−1,ωn+m)]≤2(ηn+ηn+1+⋯+ηn+m−1)S(ω0,ω0,ω1)=2ηn(1−ηm)1−ηS(ω0,ω0,ω1)→0,asn→∞, |
and hence {ωn} is a Cauchy sequence. Since (S,U) is complete, {ωn} converges to ω∈U, that is, limn→∞S(ωn,ωn,ω)=0. We assert that ω is a fixed point of A. If not, ω≠Aω, that is, S(ω,ω,Aω)>0. Now,
S(ω,ω,Aω)≤2S(ω,ω,ωn+1)+S(Aω,Aω,ωn+1)=2S(ω,ω,ωn+1)+S(Aω,Aω,Aωn)≤2S(ω,ω,ωn+1)+f(S(ω,ω,ωn),S(Aω,Aω,ω),S(Aω,Aω,ωn),S(Aωn,Aωn,ω),S(Aωn,Aωn,ωn))≤2S(ω,ω,ωn+1)+f(S(ω,ω,ωn),S(Aω,Aω,ω),S(Aω,Aω,ω)+S(ωn,ωn,ω),S(Aωn,Aωn,ω),S(Aωn,Aωn,ωn))=2S(ω,ω,ωn+1)+f(S(ω,ω,ωn),S(ω,ω,Aω),S(ω,ω,Aω)+S(ωn,ωn,ω),S(ωn+1,ωn+1,ω),S(ωn+1,ωn+1,ωn)). |
Since f is continuous, as n→∞, using Lemma 3.10, we obtain
S(ω,ω,Aω)≤f(0,S(ω,ω,Aω),S(ω,ω,Aω)+0,0,0). |
Consequently, S(ω,ω,Aω)=0, that is, Aω=ω.
Now, suppose ω∗ is another fixed point of A, that is, S(Aω,Aω,Aω∗)>0, and
S(Aω,Aω,Aω∗)≤f(S(ω,ω,ω∗),S(Aω,Aω,ω),S(Aω,Aω,ω∗),S(Aω∗,Aω∗,ω),S(Aω∗,Aω∗,ω∗))S(ω,ω,ω∗)≤f(S(ω,ω,ω∗),S(ω,ω,ω),S(ω,ω,ω∗),S(ω∗,ω∗,ω),S(ω∗,ω∗,ω∗))S(ω,ω,ω∗)≤f(S(ω,ω,ω∗),0,S(ω,ω,ω∗),S(ω,ω,ω∗),0). |
Again by Lemma 3.10, S(ω,ω,ω∗)=0, that is, ω=ω∗. Hence, A has a unique fixed point in U.
Example 3.12. Let U=[0,1] and an S metric S:U×U×U→R+ be
S(ω,υ,u)=|ω−υ|+|ω+υ−2u|,ω,υ,u∈U. |
Then, (S,U) is a complete S−metric space. Define maps f:[0,∞)5→[0,∞) and A:U→U as
f(ω1,ω2,ω3,ω4,ω5)=α(ω1+ω2+ω5),α∈[0,13) |
and Aω=ω4ω+1, respectively. Then, f∈M. Since
S(Aω,Aω,Aυ)=2|Aω−Aυ|>0, |
S(Aω,Aω,Aυ)=2|ω1+4ω−υ1+4υ|=2|ω−υ(1+4ω)(1+4υ)|≤14(|ω−υ|+8ω24ω+1+8υ24υ+1)=α(S(ω,ω,υ)+S(Aω,Aω,ω)+S(Aυ,Aυ,υ)),α=14, |
that is, A satisfies contraction condition (3.2), and 0 is a unique fixed point of A.
Corollary 3.13. Theorem 3.11 also continues to be true if (3.2) is replaced by
S(Aω,Aω,Aυ)≤αS(ω,ω,υ). |
Proof. Define f:[0,∞)5→[0,∞) by f(ω1,ω2,ω3,ω4,ω5)=αω1,α∈[0,1). Then, f∈M and the proof complies with Theorem 3.11.
Remark 3.1. Corollary 3.13 is an enhancement of the Banach contraction theorem [4] in S−metric space, which is the result of Sedghi et al. [37].
Corollary 3.14. Theorem 3.11 also continues to be true if (3.2) is replaced by
S(Aω,Aω,Aυ)≤α(S(Aω,Aω,ω)+S(Aυ,Aυ,υ)),α∈[0,13). |
Proof. Define f:[0,∞)5→[0,∞) by f(ω1,ω2,ω3,ω4,ω5)=α(ω2+ω5),α∈[0,13). Then, f∈M, and the proof complies with Theorem 3.11.
Remark 3.2. Corollary 3.14 is an enhancement of the Kannan contraction theorem [20] in S−metric space, which is the result of Phaneendra [33].
Corollary 3.15. Theorem 3.11 also continues to be true if (3.2) is replaced by
S(Aω,Aω,Aυ)≤α(S(Aω,Aω,υ)+S(Aυ,Aυ,ω)),α∈[0,13). |
Proof. Define f:[0,∞)5→[0,∞) by f(ω1,ω2,ω3,ω4,ω5)=α(ω3+ω4),α∈[0,13). Then, f∈M, and the proof complies with Theorem 3.11.
Remark 3.3. Corollary 3.15 is an enhancement of the Chatterjee contraction theorem [7] in S−metric space, which is the result of Phaneendra and Swamy [31].
Corollary 3.16. Theorem 3.11 also continues to be true if (3.2) is replaced by
S(Aω,Aω,Aυ)≤αmax{S(ω,ω,υ),S(Aω,Aω,ω),S(Aω,Aω,υ),S(Aυ,Aυ,ω),S(Aυ,Aυ,υ)},α∈[0,13). |
Proof. Define f:[0,∞)5→[0,∞) by f(ω1,ω2,ω3,ω4,ω5)=α{ω1,ω2,ω3,ω4,ω5}α∈[0,13). Then, f∈M, and the proof complies with Theorem 3.11.
Remark 3.4. Corollary 3.16 is an enhancement of the Ćirić type contraction theorem [9] in S−metric space, which is the result of Phaneendra and Swamy [31].
Corollary 3.17. Theorem 3.11 also continues to be true if (3.2) is replaced by
S(Aω,Aω,Aυ)≤αS(ω,ω,υ)+βS(Aω,Aω,ω)+γ(S(Aω,Aω,υ)+S(Aυ,Aυ,ω)+δS(Aυ,Aυ,υ)}, |
where α+β+3γ+δ∈[0,1).
Proof. Define f:[0,∞)5→[0,∞) by
f(ω1,ω2,ω3,ω4,ω5)=αω1+βω2+γ(ω3+ω4)+δω5,α+β+3γ+δ∈[0,1). |
Then, f∈M, and the proof complies with Theorem 3.11.
Remark 3.5. Corollary 3.17 is an enhancement of the Hardy-Roger type contraction theorem [11] in S−metric space.
Corollary 3.18. Theorem 3.11 also continues to be true if (3.2) is replaced by
S(Aω,Aω,Aυ)≤αS(ω,ω,υ)+βS(Aω,Aω,ω)+δS(Aυ,Aυ,υ)},whereα+β+δ∈[0,1). |
Proof. Define f:[0,∞)5→[0,∞) by f(ω1,ω2,ω3,ω4,ω5)=αω1+βω2+δω5,α+β+δ∈[0,1). Then, f∈M, and the proof complies with Theorem 3.11.
Remark 3.6. Corollary 3.18 is an enhancement of the Reich-type contraction theorem [34] in S−metric space.
On suitably varying the elements of an M−class function, distinct existing well-known conclusions in the literature may be deduced. In all the above results, we have generalized, extended, unified and improved some well-known results wherein the fixed point is always unique. However, there may arise some situations where the fixed point is not unique, and the collection of fixed points may include some geometrical shape. So, now we review the geometry of the collection of fixed points in S−metric space via an M−class function. It is significant to notice that the S−metric is not in general created by any metric.
Now, define a set
(f4) M∗={f∈M:f(0,1,1,1,1)∈[0,1)}.
Clearly, M∗⊆M.
Theorem 3.19. Let (S,U) be an S−metric space, f∈M∗. For self-map A:U→U, if S(Aω,Aω,ω)>0 implies
S(Aω,Aω,ω)≤f(S(ω,ω,ω0),S(Aω,Aω,ω),S(Aω0,Aω0,ω0),S(Aω,Aω,ω0),S(Aω0,Aω0,ω)), | (3.4) |
then, C(ω0,r) is a fixed circle of A centered on ω0 with radius r=inf{S(Aω,Aω,ω):Aω≠ω,ω∈U}.
Proof. Let C(ω0,r) be any circle centered on ω0 with radius r and Aω0≠ω0, that is, S(Aω0,Aω0,ω0)>0. So, by using inequality (3.4), (f2) and (f4), we have
S(Aω0,Aω0,ω0)≤f(S(ω0,ω0,ω0),S(Aω0,Aω0,ω0),S(Aω0,Aω0,ω0),S(Aω0,Aω0,ω0),S(Aω0,Aω0,ω0))=f(0,S(Aω0,Aω0,ω0),S(Aω0,Aω0,ω0),S(Aω0,Aω0,ω0),S(Aω0,Aω0,ω0))=S(Aω0,Aω0,ω0)f(0,1,1,1,1)<S(Aω0,Aω0,ω0), |
a contradiction, which implies Aω0=ω0.
Now, consider ω∈C(ω0,r) and Aω≠ω, that is, S(Aω,Aω,ω)>0. Also, by definition of r, S(Aω,Aω,ω)≥r.
Now, by using inequality (3.4), properties of the M−class function and Lemma 3.10,
S(Aω,Aω,ω)≤f(S(ω,ω,ω0),S(Aω,Aω,ω),S(Aω0,Aω0,ω0),S(Aω,Aω,ω0),S(Aω0,Aω0,ω))=f(S(ω,ω,ω0),S(Aω,Aω,ω),S(ω0,ω0,ω0),S(Aω,Aω,ω0),S(ω0,ω0,ω))≤f(S(ω,ω,ω0),S(Aω,Aω,ω),0,2S(Aω,Aω,ω)+S(ω0,ω0,ω),S(ω,ω,ω0))=f(r,S(Aω,Aω,ω),0,2S(Aω,Aω,ω)+r,r)≤f(S(Aω,Aω,ω),S(Aω,Aω,ω),0,3S(Aω,Aω,ω),S(Aω,Aω,ω))=S(Aω,Aω,ω)f(1,1,0,3,1)≤ηS(Aω,Aω,Aω)<S(Aω,Aω,Aω), |
a contradiction. Thus, S(Aω,Aω,Aω)=0, that is, Aω=ω. Hence, C(ω0,r) is a fixed circle of A.
Example 3.20. Let an S−metric S:U×U×U⟶R+ be
S(ω,ω,υ)=|w1−u1|+|w1+u1−2v1|+|w2−u2|+|w2+u2−2v2|+|w3−u3|+|w3+u3−2v3|, |
where ω=(w1,w2,w3),υ=(v1,v2,v3),u=(u1,u2,u3)∈U=R3. Then,
C(ω0,8)={ω∈U:S(ω0,ω0,ω)=8}, |
where ω0=(1,2,3)∈U and r=8, that is, a circle centered at (1,2,3) with radius 8 is given by
|1−w1|+|1+w1−2|+|2−w2|+|2+w2−4|+|3−w3|+|3+w3−6|=8|1−w1|+|2−w2|+|3−w3|=4. | (3.5) |
Define A:U⟶U as A(a,b,c)={(a,b,c),(a,b,c)∈C(ω0,8)(1,0,2),otherwise.
Then, map A validates all the hypotheses of Theorem 3.19 and fixes the unique circle C(ω0,8), that is, the set of fixed points of a self-map A contains a unique circle C(ω0,8) (see Figure 1).
Following Joshi et al. [16,17], now, we define an ellipse (elliptic disc) in an S−metric space and discuss their shapes in different S−metric spaces for different lengths of semi-major axes and different foci. Next, we describe a fixed ellipse (elliptic disc) in an S−metric space and exploit an S−metric variant of a celebrated Caristi type map [6] to conclude that the collection of fixed points incorporates an ellipse (elliptic disc). It is well known that an ellipse is the locus of a point for which the sum of the Euclidean distances from the two foci is uniform, and the circle is the ellipse of diminishing eccentricity wherein both the focal points are identical. In fact, ellipses emerge naturally in numerous areas, such as planetary orbits.
Definition 3.1. We define an ellipse having foci at c1 and c2 in an S−metric space (U,S) as
E(c1,c2,a)={ω∈U:S(c1,c1,ω)+S(c2,c2,ω)=2a,c1,c2∈U,a∈[0,∞)}. |
If S(c1,c1,ω)+S(c2,c2,ω)≤2a, then the above definition reduces to the definition of an elliptic disc, and we denote it by ED(c1,c2,a). For the formation of ellipse, S(c1,c1,c2)<2a.
The distance 2f=S(c1,c1,c2) is the linear eccentricity. It is well known that eccentricity is the degree of the deflection of the curve from the roundness of a specific shape. The midpoint of line c1c2 is said to be a center of an ellipse (elliptic disc). The portion of length 2a passing through the foci c1 and c2 is the major axis, and the line through the center, perpendicular to the major axis, is the minor axis.
Example 3.21. Let an S−metric S:U×U×U⟶R+ be
S(ω,υ,u)=|ω−u|+|ω+u−2υ|,ω,υ,u∈U=R, |
that is, S(−5,−5,5)=20. Then,
E(−5,5,11)={ω∈U:S(−5,−5,ω)+S(5,5,ω)=22}={ω∈U:|5+ω|+|−5+ω+10|+|5−ω|+|5+ω−10|=22}={ω∈U:2|5+ω|+2|5−ω|=22}={−5.5,5.5}, |
and
ED(−5,5,11)={ω∈U:S(−5,−5,ω)+S(5,5,ω)≤22}=[−5.5,5.5], |
that is, an ellipse and elliptic disc centered at the origin having foci at −5 and 5 are {−5.5,5.5} and [−5.5,5.5], respectively.
Example 3.22. Let an S−metric S1:U×U×U⟶R+ be S1(ω,υ,u)=Σ2i=1(|ωi−ui|+|ωi+ui−2νi|), where ω=(w1,w2),υ=(v1,v2),u=(u1,u2)∈U=R2, and S1(c1,c1,c2)=8, where c1=(2,0) and c2=(0,2). Then,
E(c1,c2,5)={ω∈U:S1(c1,c1,ω)+S1(c2,c2,ω)=10}={ω∈U:|2−ω1|+|2+ω1−4|+|0−ω2|+|0+ω2−0|+|0−ω1|+|0+ω1−0|+|2−ω2|+|2+ω2−4|=10}={ω∈U:2|2−ω1|+2|ω2|+2|ω1|+2|2−ω2|=10}={ω∈U:|2−ω1|+|2−ω2|+|ω1|+|ω2|=5}, | (3.6) |
that is, an ellipse centered at (1,1) with foci (2,0) and (0,2) is shown as the blue line in Figure 2.
If an S−metric S2:U×U×U⟶R+ is
S2(ω,υ,u)=√(ω1−υ1)2+(ω2−υ2)2+(υ1−u1)2+(υ2−u2)2+(u1−ω1)2+(u2−ω2)2, |
ω=(ω1,ω2),υ=(υ1,υ2),u=(u1,u2)∈U=R2, |
and S2(c1,c1,c2)=4, then an ellipse having the same center and the same foci as above is √2(2−ω1)2+2ω22+√2ω21+2(2−ω2)2=6 and is shown as the blue line in Figure 3.
Let S3:U×U×U⟶R+ be S3(ω,υ,u)=max{|ω1−υ1|,|ω2−υ2|,|υ1−u1|,|υ2−u2|,|u1−ω1|,|u2−ω2|}, ω=(ω1,ω2),υ=(υ1,υ2), u=(u1,u2)∈U=R2, and S3(c1,c1,c2)=2. Then, again, an ellipse with the same center and the same foci is max{|2−w1|,|w2|}+max{|w1|,|2−w2|}=2 and is shown as the blue line in Figure 4.
The shapes of ellipses corresponding to an S1 metric, as used in Figure 2, corresponding to different foci and different values of semi major axes are shown in Figure 5.
Example 3.23. Let an S−metric S1:U×U×U⟶R+ be S1(ω,υ,u)=Σ3i=1(|ωi−υi|+|ωi−ui|), where ω=(ω1,ω2,ω3),υ=(υ1,υ2,υ3),u=(u1,u2,u3)∈U=R3. Then,
E(c1,c2,2)={ω∈U:S1(c1,c1,ω)+S1(c2,c2,ω)=12}={ω∈U:2|ω1|+2|ω2|+2|ω3|+2|ω1−1|+2|ω2−1|+2|ω3−1|=12}={ω∈U:|ω1|+|ω2|+|ω3|+|ω1−1|+|ω2−1|+|ω3−1|=6, | (3.7) |
where c1=(0,0,0) and c2=(1,1,1), that is, an ellipse centered at (0.5,0.5,0.5) with foci (0,0,0) and (1,1,1) is shown in Figure 6.
If an S−metric S2:U×U×U⟶R+ is
S2(ω,υ,u)=√Σ3i=1(ωi−υi)2+√Σ3i=1(ωi−ui)2, |
ω=(ω1,ω2,ω3),υ=(υ1,υ2,υ3),u=(u1,u2,u3)∈U=R3, |
then an ellipse having the same center and the same foci as above is
√ω21+ω22+ω23+√(ω1−1)2+(ω2−1)2+(ω3−1)2=6 |
and is shown in Figure 7.
If S3:U×U×U⟶R+ is
S3(ω,υ,u)=max{|ω1−u1|,|ω2−u2|,|ω3−u3|}+max{|υ1−u1|,|υ2−u2|,|υ3−u3|}, |
ω=(ω1,ω2,ω3),υ=(υ1,υ2,υ3),u=(u1,u2,u3)∈U=R3, |
then again an ellipse with the same center and the same foci is
max{|ω1|,|ω2|,|ω3|}+max{|ω1−1|,|ω2−1|,|ω3−1|}=6 |
and is shown in Figure 8.
It is fascinating to see that the shapes of some ellipses may change by changing the length of the semi-major axis (see Figures 1–3) or foci (see Figure 4), or involved metric (see Figures 2–4 and 6–8).
Remark 3.7. The interior of Figures 2–8 is the corresponding elliptic disc with the same center, foci and length of the semi-major axis as those of the ellipse.
Following Caristi [6], we introduce the Caristi map in an S−metric space.
Definition 3.2. A self-map A of an S−metric space (U,S) is a Caristi map on U if ς:U⟶[0,∞) is a lower semi-continuous function for (U,S) and
S(ω,ω,Aω)≤ς(ω)−ς(Aω),ω∈U. |
Following Joshi et al. [16], we introduce fixed ellipse and elliptic disc in S−metric space to explore the geometry of the collection of non-unique fixed points.
Definition 3.3. Let A:U⟶U be a self-map of an S−metric space (U,S). If Aω=ω,ω∈E(c1,c2,a),c1,c2∈U,a∈[0,∞), then E(c1,c2,a) is said to be the fixed ellipse of A.
Definition 3.4. Let A:U⟶U be a self-map of an S−metric space (U,S). If Aω=ω,ω∈ED(c1,c2,a),c1,c2∈U,a∈[0,∞), then ED(c1,c2,a) is said to be the fixed elliptic disc of A.
Theorem 3.24. Let E(c1,c2,a) be an ellipse in an S−metric space (U,S). Define ς:U⟶[0,∞) as
ς(ω)=S(c1,c1,ω)+S(c2,c2,ω),c1,c2,ω∈U. | (3.8) |
If self-map A:U⟶U satisfies the hypotheses
(E1) S(ω,ω,Aω)≤ς(ω)−ς(Aω),
(E2) S(c1,c1,Aω)+S(c2,c2,Aω)≥2a,
(E3) if S(Aω,Aω,Aυ)≤σS(ω,ω,υ),ω∈E(c1,c2,a),υ∈U∖E(c1,c2,a),σ∈[0,1),
then E(c1,c2,a) is a unique fixed ellipse of A.
Proof. Let ω∈E(c1,c2,a) be an arbitrary point. Utilizing (E1) and Eq (3.8),
S(ω,ω,Aω)≤S(c1,c1,ω)+S(c2,c2,ω)−S(c1,c1,Aω)−S(c2,c2,Aω)=2a−S(c1,c1,Aω)−S(c2,c2,Aω)≤2a−2a,(using(E2)) |
that is,
S(ω,ω,Aω)=0⟹Aω=ω, | (3.9) |
that is, ω is a fixed point of A,∀ω∈E(c1,c2,a).
So, a self-map A fixes an ellipse E(c1,c2,a), that is, the set of fixed points of a self-map A contains an ellipse.
Let E(c1,c2,a) and E(c′1,c′2,a′) be two fixed ellipses of A, that is, A satisfies both conditions (E1) and (E2) for each of the ellipses E(c1,c2,a) and E(c′1,c′2,a′). Let ω∈E(c1,c2,a) and υ∈E(c′1,c′2,a′). Using (E3), S(ω,ω,υ)=S(Aω,Aω,Aυ)≤σS(ω,ω,υ), a contradiction. Hence, E(c1,c2,a) is a unique fixed ellipse of A.
The subsequent explanatory example with pictographic validation substantiates Theorem 3.24.
Example 3.25. Let an S−metric S:U×U×U⟶R+ be
S(ω,υ,u)=√(w1−v1)2+(w2−v2)2+(υ1−u1)2+(υ2−u2)2+(ω1−u1)2+(ω2−u2)2, |
where ω=(w1,w2),υ=(v1,v2),u=(u1,u2)∈U=R2. Then,
E(c1,c2,5)={ω∈U:S(c1,c2,ω)+S(c2,c2,ω)=15}, |
where c1=(4,5) and c2=(−2,−3)∈U, that is, the equation of an ellipse centered at (1,1) with foci at (4,5) and (−2,−3) is
√2(4−ω1)2+2(5−ω2)2+√2(2+ω1)2+2(3+ω2)2=15. | (3.10) |
Define A:U⟶U as A(a,b)={(a,b),(a,b)∈E(c1,c2,7.5)(2.47,0),otherwise.
Then, map A validates all the hypotheses of Theorem 3.24 and fixes the unique ellipse E(c1,c2,5), that is, the set of fixed points of a self-map A contains a unique ellipse E(c1,c2,5) (see Figure 9).
Geometrically, condition (E1) states that Aω is in the exterior of an ellipse, and condition (E2) states that Aω is in the interior of an ellipse.
The following examples depict the importance of hypotheses (E1)–(E3) in the existence of a fixed ellipse or a unique fixed ellipse in Theorem 3.24.
Example 3.26. Let an S−metric S:U×U×U⟶R+ be
S(ω,υ,u)=|ω−υ|+|ω+u−2υ|,ω,υ,u∈U=R. |
The ellipse
E(2,4,6)={ω∈U:S(2,2,ω)+S(4,4,ω)=12}={ω∈U:|2−ω|+|2+ω−4|+|4−ω|+|4+ω−8|=12}={ω∈U:2|2−ω|+2|4−ω|=12}={ω∈U:|2−ω|+|4−ω|=6}={0,6}. |
Define A:U⟶U as Aω={ω,ω=0orωisanoddnumber6,otherwise.
Then, a self-map A validates all the hypotheses of Theorem 3.24 except (E3). Hence, a self-map A fixes the ellipse E(2,4,6). However, it is not unique, and there may exist infinitely many ellipses which are fixed by a self-map A.
Example 3.27. Let an S−metric S:U×U×U⟶R+ be
S(ω,υ,u)=Σ2i=1(|ωi−ui|+|ωi+ui−2νi|), |
where ω=(w1,w2),υ=(v1,v2),u=(u1,u2)∈U=R2. Then,
E(c1,c2,6)={ω∈U:S(c1,c1,ω)+S(c2,c2,ω)=12}, | (3.11) |
where c1=(2,0) and c2=(0,2)∈U, that is, the equation of an ellipse centered at (1,1) with foci at (2,0) and (0,2) is
|2−ω1|+|2+ω1−4|+|0−ω2|+|0+ω2−0| |
+|0−ω1|+|0+ω2−0|+|2−ω2|+|2+ω2−4|=12, |
that is,
2[|2−ω1|+|ω2|+|ω1|+|2−ω2|]=12, |
that is,
|2−ω1|+|ω2|+|ω1|+|2−ω2|=6. |
Define A:U⟶U as A(ω,υ)={(ω,υ),ω∈{−1,0,1,2,3}(3,0),otherwise.
Then, a self-map A validates hypothesis (E2) and does not validate hypotheses (E1) and (E3) of Theorem 3.24. Hence, A does not fix the ellipse E(c1,c2,6) but fixes the points (0,−1),(0,3),(2,−1),(2,3),(−1,y) and (3,y)∈U,0≤y≤2 of an ellipse (3.11).
Theorem 3.28. The conclusion of Theorem 3.24 continues to be true even if we replace (E1) and (E2) by
(E′1) S(ω,ω,Aω)≤ς(ω)+ς(Aω)−4a,
(E′2) S(c1,c1,Aω)+S(c2,c2,Aω)≤2a.
Proof. Let ω∈E(c1,c2,a) be any arbitrary point. Using (E′1) and Equation (3.8),
S(ω,ω,Aω)≤S(c1,c1,ω)+S(c2,c2,ω)+S(c1,c1,Aω)+S(c2,c2,Aω)−4a=2a+S(c1,c1,Aω,)+S(c2,c2,Aω)−4a=S(c1,c1,Aω,)+S(c2,c2,Aω)−2a≤0(using(E′2)), |
a contradiction, that is, S(ω,ω,Aω)=0⟹Aω=ω,ω∈E(c1,c2,a).
The uniqueness of a fixed ellipse may be established as in Theorem 3.24.
It is clear that geometrically the condition (E′1) states that Aω is in the exterior of an ellipse, and the condition (E′2) states that Aω is in the interior of an ellipse.
The relationships among the "if"s and "then"s in this theorem are unclear. Currently, it appears that the first "if" ("If self-map …") does not have a conclusion, that is, a corresponding "then" clause. Meanwhile, hypothesis (E2D) appears to lack an expected "if" preceding its "then". Lastly, (E3D) appears to be its own complete conditional.
Theorem 3.29. Let ED(c1,c2,a) be an elliptic disc in an S−metric space (U,S). Define ς:U⟶[0,∞) as in (3.8). If self-map A:U⟶U satisfies the hypotheses
(E1D) S(ω,ω,Aω)≤ς(ω)+ς(Aω)−4a,
(E2D) S(c1,c1,Aω)+S(c2,c2,Aω)≤2a,ω∈ED(c1,c2,a).
Then, ED(c1,c2,a) is a fixed elliptic disc of A.
(E3D) In addition to the above hypotheses, if S(Aω,Aω,Aυ)≤σS(ω,ω,υ),ω∈ED(c1,c2,a), υ∈U∖ED(c1,c2,a),σ∈[0,1), then ED(c1,c2,a) is a fixed elliptic disc of maximum semi-major axis a, that is, there is no fixed elliptic disc ED(c1,c2,a) of A having a semi-major axis greater than a.
Proof. The existence of a fixed elliptic disc may be shown as in Theorem 3.28.
Let there exist two fixed elliptic discs ED(c1,c2,a) and ED(c′1,c′2,a′) of A,a<a′, that is, A satisfies both the conditions (E1D) and (E2D) for each of the elliptic discs E(c1,c2,a) and E(c′1,c′2,a′). Let ω∈ED(c1,c2,a) and υ∈ED(c′1,c′2,a′). Using (E3D), S(ω,ω,υ)=S(Aω,Aω,Aυ)≤σS(ω,ω,υ), a contradiction. Hence, ED(c1,c2,a) is a fixed elliptic disc of maximum semi-major axis a.
The subsequent explanatory example with pictographic validation substantiates Theorems 3.28 and 3.29.
Example 3.30. Let an S−metric S:U×U×U⟶R+ be
S(ω,υ,u)=Σ2i=1(|eωi−eui|+|eωi+eui−2eυi|), |
ω=(ω1,ω2),υ=(υ1,υ2),u=(u1,u2)∈U=R2. |
Then,
E(c1,c2,a)={ω∈U:S(c1,c1,ω)+S(c2,c2,ω)=4},ED(c1,c2,a)={ω∈U:S(c1,c1,ω)+S(c2,c2,ω)≤4}, |
where c1=(0,0) and c2=(ln2,0), that is, the equation of an ellipse centered at (0.35,0) with foci at (0,0) and (ln2,0) is
|e0−eω1|+|e0+eω1−2e0|+|e0−eω2|+|e0+eω2−2e0|+|eln2−eω1|+|eln2+eω1−2eln2|+|e0−eω2|+|e0+eω2−2e0|=4, |
that is,
2|1−eω1|+4|1−eω2|+2|2−eω1|=4, |
that is,
|1−eω1|+2|1−eω2|+|2−eω1|=2 | (3.12) |
is an ellipse, and
|1−eω1|+2|1−eω2|+|2−eω1|≤2 | (3.13) |
is an elliptic disc.
Define A:U⟶U as A(a,b)={(a,b),(a,b)∈ED(c1,c2,ln2)(a−ln15,b−ln15),otherwise.
Then, map A validates all the postulates of Theorem 3.28 except (E3) and all postulates of Theorem 3.29. Consequently, a self-map A fixes the ellipse E(c1,c2,2) and elliptic disc ED(c1,c2,2) of maximum semi-major axis 2, that is, the set of fixed points of A contains an ellipse E(c1,c2,2) as well as an elliptic disc ED(c1,c2,2) of maximum semi-major axis 2 (see Figure 10). Nevertheless, a fixed ellipse is not unique, as there exist many fixed ellipses. For example, the ellipses having foci at (0,0) and (ln2,0) with a semi-major axis of less than 2 units are the fixed ellipses of A.
Using Eq (3.8), we give one more result for the existence of a unique fixed ellipse on an S−metric space.
Theorem 3.31. Theorem 3.24 continues to be true even if we replace (E2) by
(E″2) ηS(ω,ω,Aω)+S(c1,c1,Aω)+S(c2,c2,Aω)≥2a.
Proof. Let ω∈E(c1,c2,a) be any arbitrary point. Using (E1) and Eq (3.8),
S(ω,ω,Aω)≤S(c1,c1,ω)+S(c2,c2,ω)−S(c1,c1,Aω)−S(c2,c2,Aω)=2a−S(c1,c1,Aω)−S(c2,c2,Aω)≤ηS(ω,ω,Aω),(using(E″2)), |
a contradiction, that is, S(ω,ω,Aω)=0⟹Aω=ω,ω∈E(c1,c2,a).
Following the pattern of Theorem 3.24, we may establish that E(c1,c2,a) is a unique fixed ellipse of A.
Theorem 3.32. The conclusion of Theorem 3.29 continues to be true even if we replace (E1D) and (E2D) by
(E′1D) S(ω,ω,Aω)≤ς(ω)−ς(Aω);
(E′2D) ηS(ω,ω,Aω)+S(c1,c1,Aω)+S(c2,c2,Aω)≥2a.
Proof. Let ω∈ED(c1,c2,a) be any arbitrary point. Using (E′1D) and Eq (3.8),
S(ω,ω,Aω)≤S(c1,c1,ω)+S(c2,c2,ω)−S(c1,c1,Aω)−S(c2,c2,Aω)≤2a−S(c1,c1,Aω)−S(c2,c2,Aω)≤ηS(ω,ω,Aω),(using(E′2D), |
a contradiction, that is,
S(ω,ω,Aω)=0⟹Aω=ω,ω∈E(c1,c2,a). |
Following Theorem 3.29, we may establish that ED(c1,c2,a) is a fixed elliptic disc of maximum semi-major axis a.
Example 3.33. Let an S−metric S:U×U×U⟶R+ be
S(ω,υ,u)=Σ2i=1(|tan−1ωi−tan−1ui|2+|tan−1υi−tan−1ui|2), |
ω=(ω1,ω2),υ=(υ1,υ2),u=(u1,u2)∈U=R2. |
Then
E(c1,c2,2)={ω∈U:S(c1,c1,ω)+S(c2,c2,ω)=4}, |
where c1=(0,3) and c2=(0,−3), that is, the equation of an ellipse centered at (0,0) with foci at (0,3) and (0,−3) is
|tan−10−tan−1ω1|2+|tan−10−tan−1ω1|2+|tan−13−tan−1ω2|2+|tan−13−tan−1ω2|2+|tan−10−tan−1ω1|2+|tan−10−tan−1ω1|2+|tan−1(−3)−tan−1ω2|2+|tan−1(−3)−tan−1ω2|2=4, |
that is,
|tan−1ω1|2+|tan−13−tan−1ω2|2+|tan−13+tan−1ω2|2=2 | (3.14) |
is an ellipse, and
|tan−1ω1|2+|tan−13−tan−1ω2|2+|tan−13+tan−1ω2|2≤2 | (3.15) |
is an elliptic disc.
Define A:U⟶U as A(a,b)={(a,b),(a,b)∈ED(c1,c2,2)19(tana,tanb),otherwise.
Then, map A validates all the hypotheses of Theorem 3.31 except (E3) and all hypotheses of Theorem 3.32. Consequently, a self-map A fixes the ellipse E(c1,c2,2) and elliptic disc ED(c1,c2,2) of maximum semi-major axis 2, that is, the set of fixed points of A contains an ellipse E(c1,c2,2) as well as an elliptic disc ED(c1,c2,2) of maximum semi-major axis 2 (see Figure 11). However, a fixed ellipse is not unique, as there exist many fixed ellipses. For example, the ellipse having foci at (0,3) and (0,−3) with a semi-major axis less than 2 is also the fixed ellipse of A.
Example 3.34. Let an S−metric S:U×U×U⟶R+ be
S(ω,υ,u)=|ω−u|+|ω+u−2υ|,ω,υ,u∈U=R. |
The ellipse and elliptic disc centered at 3 with foci at 2 and 4 are
E(2,4,9)={ω∈U:S(2,2,ω)+S(4,4,ω)=18}={ω∈U:|2−ω|+|2+ω−4|+|4−ω|+|4+ω−8|=18}={−32,152}, |
and
ED(2,4,9)=[−32,152]. |
Define A:U⟶U as Aω={−32,ω∈(−∞,0]152,ω∈(0,∞).
Then, map A validates all the hypotheses of Theorem 3.31 and fixes the ellipse E(2,4,9), that is, the set of fixed points of a self-map A contains unique ellipse E(2,4,9). The next result is proved by taking a function ζa to be discontinuous.
Theorem 3.35. Let E(c1,c2,a) be an ellipse in an S−metric space (U,S). Define ζa:[0,∞)⟶[0,∞) as
ζa(ω)={ω+2a,ω>00,ω=0,ω∈R+∪{0},a∈[0,∞). | (3.16) |
If there exists A:M⟶M satisfying
(E‴1) S(ω,ω,Aω)≤S(c1,c1,Aω)+S(c2,c2,Aω)−ζa(S(ω,ω,Aω)),
(E‴2) S(c1,c1Aω)+S(c2,c2,Aω)≤2a,
(E‴3) S(Aω,Aω,Aυ)≤σS(ω,ω,υ),ω,υ∈E(c1,c2,a),υ∈U∖E(c1,c2,a),σ∈[0,1), then E(c1,c2,a) is a unique fixed ellipse of A.
Proof. Let ω∈E(c1,c2,a) such that Aω≠ω,ω∈E(c1,c2,a). Using (E‴1) and Eq (3.16),
S(ω,ω,Aω)≤S(c1,c1,Aω)+S(c2,c2Aω)−S(ω,ω,Aω)−2a≤2a−S(ω,ω,Aω)−2a |
⟹2S(ω,ω,Aω)≤0, a contradiction, that is, Aω=ω,ω∈E(c1,c2,a).
Following Theorem 3.24, we may establish that E(c1,c2,a) is a unique fixed ellipse of A.
The subsequent example depicts the significance of condition (E‴3) in the existence of a unique fixed ellipse in Theorem 3.35.
Example 3.36. Let an S−metric S:U×U×U⟶R+ be
S(ω,υ,u)=|ω−u|+|ω+u−2υ|,ω,υ,u∈U=R. |
The ellipse
E(2,4,4)={ω∈U:S(2,2,ω)+S(4,4,ω)=8}={ω∈U:2|2−ω|+2|4−ω|=8}={ω∈U:|2−ω|+|4−ω|=4}={1,5}. |
Define A:U⟶U as Aω={2ω+1ω+3,ω∈(−∞,2)15ω−3ω+1,ω∈[2,∞).
Then, a self-map A validates the hypotheses (E‴1) and (E‴2) of Theorem 3.35 but does not validate the hypothesis (E‴3). Noticeably, A fixes the two ellipses E(2,4,4) and E(2,5,11). It is clear that geometrically the condition (E‴1) states that Aω is in the exterior of an ellipse, and the condition (E‴2) states that Aω is in the interior of an ellipse.
The relationships among the "if"s and "then"s in this theorem are unclear, as in Theorem 3.29.
Theorem 3.37. Let ED(c1,c2,a) be an elliptic disc in an S−metric space (U,S). Define ζa:U⟶[0,∞) as in Eq (3.16). If self-map A:U⟶U satisfies the hypotheses
(E″1D) S(ω,ω,Aω)≤S(c1,c1,Aω)+S(c2,c2Aω)−ζa(S(ω,ω,Aω)),
(E2D) S(c1,c1,Aω)+S(c2,c2,Aω)≤2a,ω∈ED(c1,c2,a).
Then, ED(c1,c2,a) is a fixed elliptic disc of A.
(E3D) In addition to the above hypotheses, if S(Aω,Aω,Aυ)≤σS(ω,ω,υ),ω∈ED(c1,c2,a), υ∈U∖ED(c1,c2,a),σ∈[0,1), then ED(c1,c2,a) is a fixed elliptic disc of maximum semi-major axis a, that is, there is no fixed elliptic disc ED(c1,c2,a) of A having a semi-major axis greater than a.
Proof. The proof is simple and follows Theorem 3.35.
Remark 3.8 (Joshi et al. [14,16] and Joshi and Tomar [17]). (1) Examples 3.21–3.23, 3.26–3.36 (Examples 3.21, 3.22, 3.30–3.33) demonstrate that an ellipse (elliptic disc) in an S−metric space may not be similar to an ellipse (elliptic disc) in a Euclidean space. Further, Examples 3.22, 3.23, 3.30 and 3.33 demonstrate the significant fact that the shape of the ellipse (elliptic disc) may alter by altering the center, the semi-major axis, the foci or the S−metric under consideration. Also, the semi-major axis a of the fixed ellipse (elliptic disc) is not dependent on a center and may not be maximal.
(2) The fixed ellipse and fixed elliptic disc conclusions are comparable to fixed-circle and fixed disc conclusions if both the focuses coincide. Clearly, if c1=c2=u0 (say), E(c1,c2,a)=C(u0,a2) and ED(c1,c2,a)=D(u0,a2), with center u0 and radius a2. Also, AE(c1,c2,a)=E(c1,c2,a) does not imply that E(c1,c2,a) is a fixed ellipse of A, and AED(c1,c2,a)=ED(c1,c2,a) does not imply that ED(c1,c2,a) is a fixed elliptic disc of A.
(3) It is clear from Examples 3.30 and 3.33 that if a self-map fixes an elliptic disc, then it also fixes an ellipse. However, the reverse may not hold (see Examples 3.25–3.27, 3.34, 3.36). The fixed elliptic disc is not unique, that is, all the elliptic discs inside a fixed elliptic disc of a self map in an S−metric space are also fixed elliptic discs (see Examples 3.30 and 3.33). An elliptic disc having a maximum semi-major axis is called the greatest elliptic disc. For details on the collection of non-unique fixed points containing some geometric figures, one may refer to Aydi et al. [3], Beloul et al. [5], Joshi et al. [13,14,15,16,17,18], Joshi and Tomar [17], Mlaiki et al. [22,23], Özgür et al. [27], Özgür and Taş [27,28,29,30], Petwal et al. [32], Taş et al. [38], Tomar and Joshi [39], Tomar et al. [40] and references therein.
Let I:U⟶U be the identity map, that is, Iω=ω∈U. Clearly, I satisfies the first two hypotheses of each of the Theorems 3.24, 3.28, 3.31 and 3.35 for an ellipse. Now, we devise conditions that preclude the possibility of the identity map I from Theorems 3.24, 3.28, 3.31 and 3.35.
Theorem 3.38. Let a self-map A:U⟶U have a fixed ellipse E(c1,c2,a),c1,c2∈U,a∈[0,∞) in an S−metric space (U,S). Let map ς be defined as in Theorems 3.24, 3.28, 3.31 and 3.35, and map A satisfies
(Ⅰ) λS(ω,ω,Aω)≤ς(ω)−2ς(Aω), ω∈U,andλ>2⟺A=I.
Proof. Let ω∈U and Aω≠ω. Then,
λS(ω,ω,Aω)≤S(c1,c1,ω)+S(c2,c2,ω)−2S(c1,c1,Aω)−2S(c2,c2,Aω)≤2S(c1,c1,Aω)+S(Aω,Aω,ω)+2S(c2,c2,Aω)+S(Aω,Aω,ω) 2S(c1,c1,Aω)−2S(c2,c2,Aω)=2S(Aω,Aω,ω)=2S(ω,ω,Aω)(usingsymmetryofS), |
(λ−2)S(ω,ω,Aω)≤0, a contradiction, since λ>2. Hence, S(ω,ω,Aω)=0, that is, Aω=ω=Iω,ω∈U.
Conversely, it is straightforward to validate that I satisfies inequality (Ⅰ).
Theorem 3.39. The conclusion of Theorem 3.38 continues to be true if (Ⅰ) is replaced by
(Ⅰ′) S(ω,ω,Aω)≤λ1(ς(ω)−2ς(Aω)), ω∈U,andλ1<12⟺A=I.
Proof. Let ω∈U and Aω≠ω. Then,
S(ω,ω,Aω)≤λ1(S(c1,c1,ω)+S(c2,c2,ω)−2S(c1,c1,Aω)−2S(c2,c2,Aω))≤λ1(2S(c1,c1,Aω)+S(Aω,Aω,ω)+2S(c2,c2,Aω)+S(Aω,Aω,ω)−2S(c1,c1,Aω)−2S(c2,c2,Aω))=2λ1S(Aω,Aω,ω)=2λ1S(ω,ω,Aω)(usingsymmetryofS), |
that is, (1−2λ1)S(ω,ω,Aω)≤0, a contradiction, since λ1<12. Hence, S(ω,ω,Aω)=0, that is, Aω=ω=Iω,ω∈U.
Conversely, it is straightforward to validate that I satisfies inequality (Ⅰ′).
Theorem 3.40. The conclusion of Theorem 3.38 continues to be true if (Ⅰ) is replaced by
(Ⅰ″) S(ω,ω,Aω)≤ζa(S(ω,ω,Aω))+2a.
Proof. Let ω∈U and Aω≠ω, and then S(ω,ω,Aω)≤S(ω,ω,Aω)−2a+2a=S(ω,ω,Aω), a contradiction. Hence, Aω=ω=Iω,ω∈U.
Conversely, it is straightforward to validate that I satisfies inequality (Ⅰ)″.
Remark 3.9. Conclusions of Theorems 3.38–3.40 are also true for fixed elliptic disc ED(c1,c2,a).
It is interesting to see that the fixed ellipse E(c1,c2,a) may not be unique (see Examples 3.26, 3.30 and 3.36) except if a supplementary contraction condition is presumed. In Theorems 3.24, 3.28, 3.31, and 3.35, we have utilized the Banach contraction [4] to prove the uniqueness of a fixed ellipse. In the subsequent result, we determine the uniqueness utilizing quasi-contractive condition [9]. In the same way, we may utilize other classical contractions present in the literature to demonstrate the uniqueness of the fixed ellipse.
Theorem 3.41. Let E(c1,c2,a) be a fixed ellipse of a self-map A:U→U of an S−metric space (U,S). If A satisfies the first two conditions of Theorems 3.24, 3.28, 3.31 and 3.35, along with the contraction condition
S(Aω,Aω,Aυ)≤ηmax{S(ω,ω,υ),S(ω,ω,Aυ),S(υ,υ,Aω),S(ω,ω,Aω),S(υ,υ,Aυ))}, | (3.17) |
ω∈E(c1,c2,a),υ∈U∖E(c1,c2,a), where η∈[0,1), then E(c1,c2,a) is a unique fixed ellipse of A.
Proof. Let E(c1,c2,a) and E(c′1,c′2,a′) be two fixed ellipses of A, that is, A satisfies the first two postulates of Theorems 3.24, 3.28, 3.31 and 3.35 for both the ellipses E(c1,c2,a) and E(c′1,c′2,a′). Let ω∈E(c1,c2,a) and υ∈E(c′1,c′2,a′). Using inequality (3.17),
S(ω,ω,υ)=S(Aω,Aω,Aυ)≤ηmax{S(ω,ω,υ),S(ω,ω,υ),S(υ,υ,ω),S(ω,ω,ω),S(υ,υ,υ)}=ηS(ω,ω,υ)<S(ω,ω,υ), |
a contradiction. Hence, E(c1,c2,a) is a unique fixed ellipse of A.
Remark 3.10. A conclusion almost identical to Theorem 3.41 may also be established for the existence of the greatest fixed elliptic disc using a quasi-contractive condition [9].
Next, we give propositions for the existence of a self-map that fixes the given ellipses.
Proposition 3.1 Let E(c1,c2,a) and E(c′1,c′2,a′) be any two ellipses in an S−metric space (U,S). Then, we have more than one self-map A on U such that a self-map A fixes the ellipses E(c1,c2,a) and E(c′1,c′2,a′).
Proof. Define A:U⟶U as Aω={ω,ω∈E(c1,c2,a)∪E(c′1,c′2,a′)μ,otherwise,ω∈U,
where μ is some constant such that S(c1,c1,μ)+S(c2,c2,μ)≠2a and S(c′1,c′1,μ)+S(c′2,c′2,μ)≠2a′.
Now, define ς1,ς2:U⟶[0,∞) as ς1(ω)=S(c1,c1,ω)+S(c2,c2,ω) and ς2(ω)=S(c′1,c′1,ω)+S(c′2,c′2,ω),ω∈U. Then, a self-map A validates all the hypotheses of Theorems 3.24 and 3.28 (except (E3)) for the ellipses E(c1,c2,a) and E(c′1,c′2,a′). Hence, E(c1,c2,a) and E(c′1,c′2,a′) are fixed ellipses of A.
Following an almost identical pattern, Proposition 3.1 may be extended for n ellipses.
Proposition 3.2 If E(c1,c2,a1),E(c′1,c′2,a′1),…,E(cn1,cn2,an1) are any n ellipses in an S−metric space (U,S), then we have more than one self-map A on U so that a self-map A fixes ellipses E(c1,c2,a1),E(c′1,c′2,a′1),…,E(cn1,cn2,an1).
One may observe that the ellipses E(c1,c2,a1),E(c′1,c′2,a′1),…,E(cn1,cn2,an1) need not be disjoint.
Remark 3.11 Propositions similar to Propositions 3.1 and 3.2 are also true for two and n elliptic discs ED(c1,c2,a1), ED(c′1,c′2,a′1),…, ED(cn1,cn2,an1), respectively.
Next, we give a proposition on an S−metric space in which an ellipse (elliptic disc) includes all the points of space except its foci and validate it by giving an example.
Proposition 3.3 For a∈R+, define the map Sa:U×U×U⟶[0,∞) as
Sa(ω,υ,u)={0,ω=υ=ua,otherwise,ω,υ,u∈U. |
Then, the ellipse E(c1,c2,a) (elliptic disc ED(c1,c2,a)) includes all the points of space U except the foci c1,c2∈U.
Proof. Obviously, the function Sa is an S−metric on U, and consequently, (U,Sa) is an S−metric space. Let the ellipse E(c1,c2,a)={ω∈U:Sa(c1,c1,ω)+Sa(c2,c2,ω)=2a} (elliptic disc ED(c1,c2,a)={ω∈U:Sa(c1,c1,ω)+Sa(c2,c2,ω)≤2a}). Clearly, ellipse E(c1,c2,a) (elliptic disc ED(c1,c2,a)) consists of all of the points ω∈U so that ω∉{c1,c2}.
Example 3.42. Let (U,Sa) be an S−metric space so that the S−metric Sa be as in Proposition 3.3. Consider a set J={ωi:1≤i≤n},n∈N. Obviously, there exists an ellipse E(c1,c2,a) (elliptic disc ED(c1,c2,a)) consisting of the elements of J as follows:
{ω∈U:Sa(c1,c1,ω)+Sa(c2,c2,ω)=2a}={ω1,ω2,…,ωn},c1,c2∈U∖J({ω∈U:Sa(c1,c1,ω)+Sa(c2,c2,ω)≤2a}={ω1,ω2,…,ωn},c1,c2∈U∖J), |
that is, E(c1,c2,a)=ED(c1,c2,a).
First, we discuss the continuity of a self-map on a fixed ellipse in S−metric spaces. This discussion will also be beneficial for providing the answer to the query of continuity of contractive maps (Rhoades [35]) at the fixed ellipse (elliptic disc).
Theorem 4.1. Let E(c1,c2,a),c1,c2∈U,a∈[0,∞), be a fixed ellipse of a self-map A in an S−metric space (U,S) satisfying
(i) \mathcal{S}(\mathcal{A}\omega, \mathcal{A}\omega, \mathcal{A}\upsilon)\leq \eta{\boldsymbol{M}}(\omega, \omega, \upsilon) , where
{\boldsymbol{M}}(\omega,\omega,\upsilon) = \max\{\mathcal{S}(\omega,\omega,\upsilon), \mathcal{S}(\omega,\omega,\mathcal{A}\upsilon),\mathcal{S}(\upsilon,\upsilon,\mathcal{A}\omega), \mathcal{S}(\omega,\omega,\mathcal{A}\omega),\mathcal{S}(\upsilon,\upsilon,\mathcal{A}\upsilon) \}, |
\eta\in[0, 1), \; \omega, \upsilon\in\mathcal{U} ;
(ii) for \varepsilon > 0, there exists a \delta > 0 so that \varepsilon < {\boldsymbol{M}}(\omega, \omega, \upsilon) < \varepsilon+\delta\Longrightarrow d(\mathcal{A}\omega, \mathcal{A}\omega, \mathcal{A}\upsilon) < \varepsilon .
Then, a self-map \mathcal{A} is continuous at u\in\mathcal{E}(\mathfrak{c}_{1}, \mathfrak{c}_{2}, \mathfrak{a}) iff \lim_{\omega_n\longrightarrow u}{\textbf{M}}(\omega_{n}, \omega_{n}, u) = 0, or in other words, \mathcal{A} is discontinuous at u\in\mathcal{E}(\mathfrak{c}_{1}, \mathfrak{c}_{2}, \mathfrak{a}) iff \lim_{\omega_n\longrightarrow u}{\textbf{M}}(\omega_{n}, \omega_{n}, u)\neq 0.
Proof. Let \mathcal{A} be continuous at u\in \mathcal{E}(\mathfrak{c}_{1}, \mathfrak{c}_{2}, \mathfrak{a}) and \omega_{n}\longrightarrow u . So, \mathcal{A}\omega_{n}\longrightarrow\mathcal{A}u = u .
\begin{align*} \lim\limits_{\omega_n\longrightarrow u}{\textbf{M}}(\omega_{n},\omega_{n},u) = &\lim\limits_{\omega_n\longrightarrow u}\max\{\mathcal{S}(\omega_{n},\omega_{n},u), \mathcal{S}(\omega_{n},\omega_{n},\mathcal{A}\omega_{n}),\\ &\mathcal{S}(u,u,\mathcal{A}u), \mathcal{S}(\omega_{n},\omega_{n},\mathcal{A}\omega_{n}),\mathcal{S}(u,u,\mathcal{A}u)) \}\\ = &\max\{\mathcal{S}(u,u,u), \mathcal{S}(u,u,\mathcal{A}u), \mathcal{S}(u,u,\mathcal{A}u), \mathcal{S}(u,u,\mathcal{A}u),\mathcal{S}(u,u,\mathcal{A}u)) \} \\ = &0. \end{align*} |
Conversely, if \lim_{\omega_n\longrightarrow u}{\textbf{M}}(\omega_{n}, \omega_{n}, u) = 0 , that is, \lim_{\omega_n\longrightarrow u}\mathcal{S}(\mathcal{A}\omega_{n}, \mathcal{A}\omega_{n}, \mathcal{A}u) = 0 as \omega_{n}\longrightarrow u , hence \mathcal{A}\omega_{n}\longrightarrow \mathcal{A}u, that is, \mathcal{A} is continuous at u\in\mathcal{E}(\mathfrak{c}_{1}, \mathfrak{c}_{2}, \mathfrak{a}) .
Remark 4.1. Following similar steps, we may determine continuity and discontinuity at the fixed elliptic disc.
Continuity at a fixed ellipse (elliptic disc) may be decided by making use of function {\bf{M}}(\omega, \omega, \upsilon) in \mathcal{S-} metric spaces. Inspired by the reality that the majority of the phenomena appearing in the physical world are discontinuous, now, we discuss Mexican-hat-type [41] and Gaussian-wavelet-type [25] activation functions, which are utilized to examine non-linear properties, local stability and coexistence of several equilibrium points to the neural network.
Example 4.2. Let an \mathcal{S}- metric \mathcal{S:U\times U\times U\to}\mathbb{R}^+ be \mathcal{S}(\omega, \upsilon, u) = |\omega-u|+|\omega+u-2\upsilon|, \omega, \upsilon, u\in\mathcal{U}.
The ellipse
\begin{align*} {E}(-3,4,9)& = \{\omega\in\mathcal{U}:\mathcal{S}(-3,-3,\omega)+\mathcal{S}(4,4,\omega) = 18\}\\& = \{\omega\in\mathcal{U}:2\left|3+\omega\right|+2\left|4-\omega\right| = 18 \}\\ & = \{\omega\in\mathcal{U}:|3+\omega|+|4-\omega| = 9 \}\\& = \{ -4,\; 5\}. \end{align*} |
The Mexican-hat-type activation function is
\begin{equation} \mathcal{A}\omega = \begin{cases} -4,&-\infty < \omega < -1\\2\omega-2,&-1\leq\omega < 1\\-\omega+1,&1\leq\omega < 5\\5,&5\leq\omega < \infty \end{cases}. \end{equation} | (4.1) |
Clearly, \mathcal{A} validates all the hypotheses of Theorems 3.24, 3.28, 3.31 and 3.35. Function \mathcal{A} has two fixed points, -4 and 5 , which are also the elements of the ellipse \mathcal{E}(-3, 4, 9) . Hence, \mathcal{A} fixes the ellipse \mathcal{E}(-3, 4, 9).
Since we have \lim_{\omega_n\longrightarrow -4}{\boldsymbol{M}}(\omega_n, \omega_n, -4) = 0 , and \lim_{\omega_n\longrightarrow 5}{\boldsymbol{M}}(\omega_n, \omega_n, 5) does not exist, hence \mathcal{A} is continuous at the fixed point u = -4\in\mathcal{E}(-3, 4, 9) and discontinuous at u = 5\in\mathcal{E}(-3, 4, 9) . As a result, \mathcal{A} is discontinuous at the fixed ellipse \mathcal{E}(-3, 4, 9) (see Figure 12). Noticeably, \mathcal{A} does not fix any elliptic disc.
Example 4.3. Let an \mathcal{S}- metric \mathcal{S:U\times U\times U\to}\mathbb{R^+} be \mathcal{S}(\omega, \upsilon, u) = |\omega-u|+|\omega+u-2\upsilon|, \omega, \upsilon, u\in\mathcal{U}.
The ellipse
\begin{align*} \mathcal{E}(2,4,16)& = \{\omega\in\mathcal{U}:\mathcal{S}(2,2,\omega)+\mathcal{S}(4,4,\omega) = 32\}\\& = \{\omega\in\mathcal{U}:2\left|2-\omega\right|+2\left|4-\omega\right| = 32 \}\\& = \{\omega\in\mathcal{U}:|2-\omega|+|4-\omega| = 16 \}\\& = \{ -5,11\}. \end{align*} |
The Gaussian-wavelet-type activation function is
\begin{equation} \mathcal{A}\omega = \begin{cases} -5,&-\infty < \omega < -3\\2\omega+4,&-3\leq\omega\leq3\\-\omega+1,&3 < \omega < 6\\3\omega+6,&6\leq\omega\leq10\\11,&10 < \omega < \infty \end{cases}. \end{equation} | (4.2) |
Clearly, \mathcal{A} validates all the hypotheses of Theorems 3.24, 3.28, 3.31 and 3.35. The function \mathcal{A} has two fixed points, -5 and 11 , which are also the elements of the ellipse \mathcal{E}(2, 4, 16), hence \mathcal{A} fixes the ellipse \mathcal{E}(2, 4, 16). Since we have \lim_{\omega_n\longrightarrow -5}{\boldsymbol{M}}(\omega_n, \omega_n, -5) = 0 , and \lim_{\omega_n\longrightarrow 11}{\boldsymbol{M}}(\omega_n, \omega_n, 11) = 0 , \mathcal{A} is continuous at the ellipse \mathcal{E}(2, 4, 16) (see Figure 13). Noticeably, \mathcal{A} does not fix any elliptic disc.
Example 4.4. Let an \mathcal{S}- metric \mathcal{S:U\times U\times U}\to\mathbb{R^+} be \mathcal{S}(\omega, \upsilon, u) = |\omega-u|+|\omega+u-2\upsilon|, \omega, \upsilon, u\in\mathcal{U}.
The ellipse
\begin{align*} \mathcal{E}(-5,15,30)& = \{\omega\in\mathcal{U}:\mathcal{S}(-5,-5,\omega)+\mathcal{S}(15,15,\omega) = 60\}\\&\{\omega\in\mathcal{U}:2\left|5+\omega\right|+2\left|15-\omega\right| = 60\}\\ & = \{\omega\in\mathcal{U}:|5+\omega|+|15-\omega| = 30 \}\\ & = \{-10,20\}. \end{align*} |
The elliptic disc
\begin{align*} \mathcal{E_D}(-8,-4,8)& = \{\omega\in\mathcal{U}:\mathcal{S}(-8,-8,\omega)+\mathcal{S}(-4,-4,\omega)\leq16\}\\ &\{\omega\in\mathcal{U}:2\left|8+\omega\right|+2\left|4+\omega\right|\leq16\}\\ &\{\omega\in\mathcal{U}:|8+\omega|+|4+\omega|\leq8 \}\\ & = [-10,-2]. \end{align*} |
The Mexican-hat-type activation function is
\begin{equation} \mathcal{A}\omega = \begin{cases} -10,&-\infty < \omega\leq-10\\\omega,&-10 < \omega\leq-2\\-2\omega-6,&-2 < \omega < 2\\20,&2\leq\omega < \infty \end{cases}. \end{equation} | (4.3) |
Clearly, \mathcal{A} validates all the hypotheses of Theorems 3.29, 3.32 and 3.37. The function \mathcal{A} has infinitely many fixed points in the set [-10, -2] and at 20 . Hence, \mathcal{A} fixes the ellipse \mathcal{E}(-5, 15, 30) and the elliptic disc \mathcal{E_D}(-8, -4, 8). Since we have \lim_{\omega_n\longrightarrow \omega}{\textbf{M}}(\omega_n, \omega_n, \omega) = 0, \omega\in[-10, -2], and \lim_{\omega_n\longrightarrow 20}{\textbf{M}}(\omega_n, \omega_n, 20) does not exist, hence \mathcal{A} is discontinuous at the ellipse \mathcal{E}(-5, 15, 30) and continuous at the elliptic disc \mathcal{E_D}(-8, -4, 8) (see Figure 14).
Remark 4.2. Utilizing the number {\boldsymbol{M}}(\omega, \omega, \upsilon) , we may decide on the fixed point/ fixed ellipse/ elliptic disc at which the activation function is continuous. The motivation behind using the discontinuous activation function is the fact that its storage capacity is higher than the continuous activation function, and consequently, it can handle diverse spans of input data as diverse segments.
It is worth mentioning that a neural network is a network of neurons that is either biological, made up of real biological neurons or artificial. An artificial neural network is useful in medical diagnosis, non-linear system identification and control, sequence recognition, pattern recognition, decision-making, game-playing, financial applications, e-mail spam filtering, data mining and visualization.
Motivated by the applications of fixed point techniques in diverse real-world problems, we utilize Corollary 3.13 to solve a satellite web coupling boundary value problem [19]. A satellite web coupling may be idealized as a thin sheet connecting two cylindrical satellites. The problem of radiation from the web coupling between two satellites leads to the following non-linear boundary value problem:
\begin{equation} -\frac{d^2\omega}{dt^2} = \mu \omega^4,\; 0 < t < 1,\; \omega(0) = \omega(1) = 0, \end{equation} | (5.1) |
where \omega(t) denotes the temperature of radiation at any point t\in[0, 1], \mu = \frac{2al^2K^3 }{\zeta\mathfrak{h}} > 0 is a non-dimensional positive constant, K is the constant absolute temperature of both satellites, while heat is radiated from the surface of the web into space at 0 absolute temperature, l is the distance between two satellites, a is a positive constant describing the radiation properties of the surface of the web, factor 2 is required because there is radiation from both the top and bottom surfaces, \zeta is thermal conductivity, and \mathfrak{h} is the thickness.
The Green function
\mathcal{G}(t,\xi) = \begin{cases} t(1-\xi),& 0 < t < \xi\\ \xi(1-t),&\xi < t < 1 \end{cases}. |
Problem (5.1) is equivalent to
\omega(t) = 1-\mu \int_{0}^{1}\mathcal{G}(t,\xi)\omega^4(\xi)d\xi. |
Let \mathcal{U = R}[0, 1] be a set of Riemann integrable functions on [0, 1] . Define an \mathcal{S-} metric \mathcal{S:U\times U\times U}\to\mathbb{R}^+ by \mathcal{S}(\omega, \upsilon, u) = |\omega-u|+|\upsilon-u|. Clearly, (\mathcal{U, S}) is a complete \mathcal{S}- metric space, and \|\omega\|_{\infty} = \sup_{t\in[0, 1]}|\omega(t)| .
Theorem 5.1. Let \mathcal{A:U\to U} be a self map in a complete \mathcal{S-} metric space (\mathcal{U, S}) , satisfying
\begin{equation} \| \omega(t)-\upsilon(t)\|_{\infty} > 0\Longrightarrow\| (\omega^2(\xi)+\upsilon^2(\xi))(\omega(\xi)+\upsilon(\xi)) \|_{\infty} \leq \frac{\kappa}{\mu},\; \kappa\in(0,8). \end{equation} | (5.2) |
Then, the satellite web coupling boundary value problem (5.1) has a unique solution.
Proof. Define a self-map \mathcal{A}:\mathcal{U}\to\mathcal{U} by
\begin{equation} \mathcal{A}\omega(t) = 1-\mu \int_{0}^{1}\mathcal{G}(t,\xi)\omega^4(\xi)d\xi,\; \xi\in[0,1]. \end{equation} | (5.3) |
Clearly, a solution to the satellite web coupling problem (5.1) is a fixed point of a self map \mathcal{A} .
However, \|\mathcal{A}\omega(t)-\mathcal{A}\upsilon(t)\|_\infty > 0, so \mathcal{S}(\mathcal{A}\omega(t), \mathcal{A}\omega(t), \mathcal{A}\upsilon(t)) > 0 . Now,
\begin{equation*} \begin{split} \mathcal{S}(\mathcal{A}\omega(t),\mathcal{A}\omega(t),\mathcal{A}\upsilon(t)) & = 2|\mathcal{A}\omega(t)-\mathcal{A}(\upsilon)|\\& = 2\Big|1-\mu \int_{0}^{1}\mathcal{G}(t,\xi)\omega^4(\xi)d\xi-1+\mu \int_{0}^{1}\mathcal{G}(t,\xi)\upsilon^4(\xi)d\xi\Big|\\ & = 2\mu\Big|\int_{0}^{1}(\upsilon^4(\xi)-\omega^4(\xi))\mathcal{G}(t,\xi)d\xi\Big|\\& = 2\mu\Big|\int_{0}^{1}(\upsilon^2(\xi)+\omega^2(\xi))(\upsilon(\xi)+\omega(\xi))(\upsilon(\xi)-\omega(\xi))\mathcal{G}(t,\xi)d\xi\Big|\\& = 2\mu\|\omega(t)-\upsilon(t)\|_{\infty}\|(\omega^2(t)+\upsilon^2(t))(\omega(t)+\upsilon(t))\|_{\infty}\int_{0}^{1}\mathcal{G}(t,\xi)d\xi \\&\leq 2\kappa\|\omega(t)-\upsilon(t)\|_{\infty}\Big[\int_{0}^{t}\xi(1-t)d\xi+\int_{t}^{1}t(1-\xi)d\xi \Big]\\&\leq \frac{\kappa}{8}\|\omega(t)-\upsilon(t)\|_{\infty} \\ & = \alpha \mathcal{S}(\omega,\omega,\upsilon),\; \alpha\in[0,1) \; ({\rm{since,}}\; \kappa\in(0,8)). \end{split} \end{equation*} |
Hence, all the postulates of Corollary 3.13 are validated. As a result, \mathcal{A} has a unique fixed point, and a satellite web coupling problem (5.1) has a unique solution.
Let \mathcal{A:U\to U} be a self-map in a complete \mathcal{S-} metric space (\mathcal{U, S}) and \zeta be the simulation function [21].
(1) If \mathcal{A} is a JS-contraction [12], does \mathcal{A} have a unique fixed point / fixed ellipse/ fixed elliptic disc in \mathcal{U} ? Does the Picard sequence \{u_n\} converge to the unique fixed point u or any point u of a fixed ellipse (elliptic disc)? If not, what additional postulate(s) do we have to include?
(2) If \mathcal{A} is a surjective JS-expanding map, does \mathcal{A} have a unique fixed point/ fixed ellipse/ fixed elliptic disc in \mathcal{U}? Does the Picard sequence \{u_n\} converge to the unique fixed point u or any point u of a fixed ellipse or elliptic disc? If not, what additional postulate(s) do we have to include?
We have established a unique fixed point, fixed circle, fixed ellipse and greatest fixed elliptic disc via an \mathcal{M-} class function while extending, generalizing, unifying and improving some popular results existing in the literature. Motivated by the reflecting property of an ellipse (elliptic disc), which is useful in Medical science, Optics, Astronomy, Whispering Galleries, and so on, we have explored a new direction to the geometry of the collection of fixed points in an \mathcal{S}- metric space. Furthermore, we have discussed continuity at fixed ellipses (elliptic discs) on \mathcal{S-} metric spaces to establish the significance of novel fixed ellipse (elliptic disc) conclusions in a neural network, which permits choosing the appropriate activation function according to the underlying problem of a neural network. In the sequel, we have presented some interesting prepositions and remarks. In this paper, investigations of fixed point and fixed figure problems in metric fixed point theory have been enriched to problems formulated in terms of \mathcal{M-} class contractive conditions on an \mathcal{S-} metric space. Consequently, more general conclusions have been established than those existing in the literature. It has been demonstrated by illustrative examples that these extensions, improvements and generalizations are genuine. Towards the end, the obtained conclusions have been applied to solve the satellite web coupling problem, which is a very significant and relevant field on its own. Our results provide a specific procedure and directions for further investigation in this recently developed space.
The authors are thankful to the anonymous reviewer for his comments that help us to improve the manuscript. The author T. Abdeljawad would like to thank Prince Sultan University for the support through the TAS research lab.
The authors declare that they have no conflicts of interest.
[1] |
R. Khalil, M. Al Horani, A. Yousef, M. Sababheh, A new definition of fractional derivative, J. Comput. Appl. Math., 264 (2014), 65–70. http://dx.doi.org/10.1016/j.cam.2014.01.002 doi: 10.1016/j.cam.2014.01.002
![]() |
[2] |
R. Mabel Lizzy, K. Balachandran, J. Trujillo, Controllability of nonlinear stochastic fractional neutral systems with multiple time varying delays in control, Chaos Soliton. Fract., 102 (2017), 162–167. http://dx.doi.org/10.1016/j.chaos.2017.04.024 doi: 10.1016/j.chaos.2017.04.024
![]() |
[3] | K. Diethelm, The analysis of fractional differential equations, Berlin: Springer, 2010. http://dx.doi.org/10.1007/978-3-642-14574-2 |
[4] |
H. Yasmin A. Alderremy, R. Shah, A. Hamid Ganie, S. Aly, Iterative solution of the fractional Wu-Zhang equation under Caputo derivative operator, Front. Phys., 12 (2024), 1333990. http://dx.doi.org/10.3389/fphy.2024.1333990 doi: 10.3389/fphy.2024.1333990
![]() |
[5] |
M. Kbiri Alaoui, K. Nonlaopon, A. Zidan, A. Khan, R. Shah, Analytical investigation of fractional-order Cahn-Hilliard and gardner equations using two novel techniques, Mathematics, 10 (2022), 1643. http://dx.doi.org/10.3390/math10101643 doi: 10.3390/math10101643
![]() |
[6] |
T. Botmart, R. Agarwal, M. Naeem, A. Khan, R. Shah, On the solution of fractional modified Boussinesq and approximate long wave equations with non-singular kernel operators, AIMS Mathematics, 7 (2022), 12483–12513. http://dx.doi.org/10.3934/math.2022693 doi: 10.3934/math.2022693
![]() |
[7] |
H. Yasmin, N. Aljahdaly, A. Saeed, R. Shah, Probing families of optical soliton solutions in fractional perturbed radhakrishnan-kundu-akshmanan model with improved versions of extended direct algebraic method, Fractal Fract., 7 (2023), 512. http://dx.doi.org/10.3390/fractalfract7070512 doi: 10.3390/fractalfract7070512
![]() |
[8] |
H. Yasmin, N. Aljahdaly, A. Saeed, R. Shah, Investigating families of soliton solutions for the complex structured coupled fractional biswas-arshed model in birefringent fibers using a novel analytical technique, Fractal Fract., 7 (2023), 491. http://dx.doi.org/10.3390/fractalfract7070491 doi: 10.3390/fractalfract7070491
![]() |
[9] |
L. Barros, M. Lopes, F. Pedro, E. Esmi, J. Santos, D. Sanchez, The memory effect on fractional calculus: an application in the spread of COVID-19, Comp. Appl. Math., 40 (2021), 72. http://dx.doi.org/10.1007/s40314-021-01456-z doi: 10.1007/s40314-021-01456-z
![]() |
[10] |
R. Pakhira, U. Ghosh, S. Sarkar, Study of memory effects in an inventory model using fractional calculus, Applied Mathematical Sciences, 12 (2018), 797–824. http://dx.doi.org/10.12988/ams.2018.8578 doi: 10.12988/ams.2018.8578
![]() |
[11] |
S. Alkhateeb, S. Hussain, W. Albalawi, S. El-Tantawy, E. El-Awady, Dissipative Kawahara ion-acoustic solitary and cnoidal waves in a degenerate magnetorotating plasma, J. Taibah Univ. Sci., 17 (2023), 2187606. http://dx.doi.org/10.1080/16583655.2023.2187606 doi: 10.1080/16583655.2023.2187606
![]() |
[12] |
R. Alharbey, W. Alrefae, H. Malaikah, E. Tag-Eldin, S. El-Tantawy, Novel approximate analytical solutions to the nonplanar modified Kawahara equation and modeling nonlinear structures in electronegative plasmas, Symmetry, 15 (2023), 97. http://dx.doi.org/10.3390/sym15010097 doi: 10.3390/sym15010097
![]() |
[13] |
S. El-Tantawy, A. Salas, H. Alyouse, M. Alharthi, Novel exact and approximate solutions to the family of the forced damped Kawahara equation and modeling strong nonlinear waves in a plasma, Chinese J. Phys., 77 (2022), 2454–2471. http://dx.doi.org/10.1016/j.cjph.2022.04.009 doi: 10.1016/j.cjph.2022.04.009
![]() |
[14] |
H. Alyousef, A. Salas, M. Alharthi, S. El-tantawy, New periodic and localized traveling wave solutions to a Kawahara-type equation: applications to plasma physics, Complexity, 2022 (2022), 9942267. http://dx.doi.org/10.1155/2022/9942267 doi: 10.1155/2022/9942267
![]() |
[15] |
M. Alharthi, R. Alharbey, S. El-Tantawy, Novel analytical approximations to the nonplanar Kawahara equation and its plasma applications, Eur. Phys. J. Plus, 137 (2022), 1172. http://dx.doi.org/10.1140/epjp/s13360-022-03355-6 doi: 10.1140/epjp/s13360-022-03355-6
![]() |
[16] |
S. El-Tantawy, L. El-Sherif, A. Bakry, W. Alhejaili, A. Wazwaz, On the analytical approximations to the nonplanar damped Kawahara equation: cnoidal and solitary waves and their energy, Phys. Fluids, 34 (2022), 113103. http://dx.doi.org/10.1063/5.0119630 doi: 10.1063/5.0119630
![]() |
[17] |
R. Shah, H. Khan, P. Kumam, M. Arif, An analytical technique to solve the system of nonlinear fractional partial differential equations, Mathematics, 7 (2019), 505. http://dx.doi.org/10.3390/math7060505 doi: 10.3390/math7060505
![]() |
[18] |
H. Khan, R. Shah, D. Baleanu, P. Kumam, M. Arif, Analytical solution of fractional-order hyperbolic telegraph equation, using natural transform decomposition method, Electronics, 8 (2019), 1015. http://dx.doi.org/10.3390/electronics8091015 doi: 10.3390/electronics8091015
![]() |
[19] |
X. Li, Y. Sun, Application of RBF neural network optimal segmentation algorithm in credit rating, Neural Comput. Appl., 33 (2021), 8227–8235. http://dx.doi.org/10.1007/s00521-020-04958-9 doi: 10.1007/s00521-020-04958-9
![]() |
[20] |
T. Ali, Z. Xiao, H. Jiang, B. Li, A class of digital integrators based on trigonometric quadrature rules, IEEE T. Ind. Electron., 71 (2024), 6128–6138. http://dx.doi.org/10.1109/TIE.2023.3290247 doi: 10.1109/TIE.2023.3290247
![]() |
[21] |
B. Chen, J. Hu, B. Ghoso, Finite-time observer based tracking control of heterogeneous multi-AUV systems with partial measurements and intermittent communication, Sci. China Inform. Sci., 67 (2024), 152202. http://dx.doi.org/10.1007/s11432-023-3903-6 doi: 10.1007/s11432-023-3903-6
![]() |
[22] |
B. Chen, J. Hu, Y. Zhao, B. Ghosh, Finite-time observer based tracking control of uncertain heterogeneous underwater vehicles using adaptive sliding mode approach, Neurocomputing, 481 (2022), 322–332. http://dx.doi.org/10.1016/j.neucom.2022.01.038 doi: 10.1016/j.neucom.2022.01.038
![]() |
[23] |
C. Guo, J. Hu, Time base generator based practical predefined-time stabilization of high-order systems with unknown disturbance, IEEE T. Circuits-II, 70 (2023), 2670–2674. http://dx.doi.org/10.1109/TCSII.2023.3242856 doi: 10.1109/TCSII.2023.3242856
![]() |
[24] |
S. Lin, J. Zhang, C. Qiu, Asymptotic analysis for one-stage stochastic linear complementarity problems and applications, Mathematics, 11 (2023), 482. http://dx.doi.org/10.3390/math11020482 doi: 10.3390/math11020482
![]() |
[25] |
L. Liu, S. Zhang, L. Zhang, G. Pan, J. Yu, Multi-UUV maneuvering counter-game for dynamic target scenario based on fractional-order recurrent neural network, IEEE T. Cybernetics, 53 (2023), 4015–4028. http://dx.doi.org/10.1109/TCYB.2022.3225106 doi: 10.1109/TCYB.2022.3225106
![]() |
[26] | Y. Kai, S. Chen, K. Zhang, Z. Yin, Exact solutions and dynamic properties of a nonlinear fourth-order time-fractional partial differential equation, Wave. Random Complex, in press. http://dx.doi.org/10.1080/17455030.2022.2044541 |
[27] |
D. Kaup, On the inverse scattering problem for cubic eigenvalue problems of the class \psi_{xxx}+ 6Q \psi_{x}+ 6R_{\psi} = \lambda \psi , Stud. Appl. Math., 62 (1980), 189–216. http://dx.doi.org/10.1002/sapm1980623189 doi: 10.1002/sapm1980623189
![]() |
[28] |
B. Kupershmidt, A super Korteweg-de Vries equation: an integrable system, Phys. Lett. A, 102 (1984), 213–215. http://dx.doi.org/10.1016/0375-9601(84)90693-5 doi: 10.1016/0375-9601(84)90693-5
![]() |
[29] | O. Abdulaziz, I. Hashim, M. Chowdhury, A. Zulkifle, Assessment of decomposition method for linear and nonlinear fractional differential equations, Far East Journal of Applied Mathematics, 28 (2007), 95–112. |
[30] |
J. He, X. Wu, Construction of solitary solution and compacton-like solution by variational iteration method, Chaos Soliton. Fract., 29 (2006), 108–113. http://dx.doi.org/10.1016/j.chaos.2005.10.100 doi: 10.1016/j.chaos.2005.10.100
![]() |
[31] |
Z. Odibat, S. Momani, Application of variational iteration method to nonlinear differential equations of fractional order, Int. J. Nonlin. Sci. Num., 7 (2006), 27–34. http://dx.doi.org/10.1515/IJNSNS.2006.7.1.27 doi: 10.1515/IJNSNS.2006.7.1.27
![]() |
[32] |
J. He, Application of homotopy perturbation method to nonlinear wave equations, Chaos Soliton. Fract., 26 (2005), 695–700. http://dx.doi.org/10.1016/j.chaos.2005.03.006 doi: 10.1016/j.chaos.2005.03.006
![]() |
[33] |
Z. Odibat, Exact solitary solutions for variants of the KdV equations with fractional time derivatives, Chaos Soliton. Fract., 40 (2009), 1264–1270. http://dx.doi.org/10.1016/j.chaos.2007.08.080 doi: 10.1016/j.chaos.2007.08.080
![]() |
[34] |
Q. Wang, Homotopy perturbation method for fractional KdV-Burgers equation, Chaos Soliton. Fract., 35 (2008), 843–850. http://dx.doi.org/10.1016/j.chaos.2006.05.074 doi: 10.1016/j.chaos.2006.05.074
![]() |
[35] |
S. Liao, An approximate solution technique not depending on small parameters: a special example, Int. J. NonLin. Mech., 30 (1995), 371–380. http://dx.doi.org/10.1016/0020-7462(94)00054-E doi: 10.1016/0020-7462(94)00054-E
![]() |
[36] | M. El-Tawil, S. Huseen, The q-homotopy analysis method (q-HAM), Int. J. Appl. Math. Mech., 8 (2012), 51–75. |
[37] | J. Biazar, K. Hosseini, P. Gholamin, Homotopy perturbation method for solving KdV and Sawada-Kotera equations, Journal of Operational Research in its Applications, 6 (2009), 11–16. |
[38] | S. Dinarvand, S. Khosravi, A. Doosthoseini, M. Rashidi, The homotopy analysis method for solving the Sawada-Kotera and Lax's fifth-order KdV equations, Adv. Theor. Appl. Mech., 1 (2008), 327–335. |
[39] |
O. Abu Arqub, Series solution of fuzzy differential equations under strongly generalized differentiability, J. Adv. Res. Appl. Math., 5 (2013), 31–52. http://dx.doi.org/10.5373/jaram.1447.051912 doi: 10.5373/jaram.1447.051912
![]() |
[40] |
O. Abu Arqub, Z. Abo-Hammour, R. Al-Badarneh, S. Momani, A reliable analytical method for solving higher-order initial value problems, Discrete Dyn. Nat. Soc., 2013 (2013), 673829. http://dx.doi.org/10.1155/2013/673829 doi: 10.1155/2013/673829
![]() |
[41] |
O. Abu Arqub, A. El-Ajou, Z. Zhour, S. Momani, Multiple solutions of nonlinear boundary value problems of fractional order: a new analytic iterative technique, Entropy, 16 (2014), 471–493. http://dx.doi.org/10.3390/e16010471 doi: 10.3390/e16010471
![]() |
[42] |
A. El-Ajou, O. Abu Arqub, S. Momani, Approximate analytical solution of the nonlinear fractional KdV-Burgers equation: a new iterative algorithm, J. Comput. Phys., 293 (2015), 81–95. http://dx.doi.org/10.1016/j.jcp.2014.08.004 doi: 10.1016/j.jcp.2014.08.004
![]() |
[43] |
F. Xu, Y. Gao, X. Yang, H. Zhang, Construction of fractional power series solutions to fractional Boussinesq equations using residual power series method, Math. Probl. Eng., 2016 (2016), 5492535. http://dx.doi.org/10.1155/2016/5492535 doi: 10.1155/2016/5492535
![]() |
[44] |
J. Zhang, Z. Wei, L. Li, C. Zhou, Least-squares residual power series method for the time-fractional differential equations, Complexity, 2019 (2019), 6159024. http://dx.doi.org/10.1155/2019/6159024 doi: 10.1155/2019/6159024
![]() |
[45] |
I. Jaradat, M. Alquran, R. Abdel-Muhsen, An analytical framework of 2D diffusion, wave-like, telegraph, and Burgers' models with twofold Caputo derivatives ordering, Nonlinear Dyn., 93 (2018), 1911–1922. http://dx.doi.org/10.1007/s11071-018-4297-8 doi: 10.1007/s11071-018-4297-8
![]() |
[46] |
I. Jaradat, M. Alquran, K. Al-Khaled, An analytical study of physical models with inherited temporal and spatial memory, Eur. Phys. J. Plus, 133 (2018), 162. http://dx.doi.org/10.1140/epjp/i2018-12007-1 doi: 10.1140/epjp/i2018-12007-1
![]() |
[47] | M. Alquran, K. Al-Khaled, S. Sivasundaram, H. Jaradat, Mathematical and numerical study of existence of bifurcations of the generalized fractional Burgers-Huxley equation, Nonlinear Stud., 24 (2017), 235–244. |
[48] |
M. Alquran, M. Alsukhour, M. Ali, I. Jaradat, Combination of Laplace transform and residual power series techniques to solve autonomous n-dimensional fractional nonlinear systems, Nonlinear Engineering, 10 (2021), 282–292. http://dx.doi.org/10.1515/nleng-2021-0022 doi: 10.1515/nleng-2021-0022
![]() |
[49] | A. Khan, M. Junaid, I. Khan, F. Ali, K. Shah, D. Khan, Application of homotopy analysis natural transform method to the solution of nonlinear partial differential equations, Sci. Int. (Lahore), 29 (2017), 297–303. |
[50] | M. Zhang, Y. Liu, X. Zhou, Efficient homotopy perturbation method for fractional non-linear equations using Sumudu transform, Therm. Sci., 19 (2015), 1167–1171. |
[51] | R. Al-Deiakeh, M. Ali, M. Alquran, T. Sulaiman, S. Momani, M. Al-Smadi, On finding closed-form solutions to some nonlinear fractional systems via the combination of multi-Laplace transform and the Adomian decomposition method, Rom. Rep. Phys., 74 (2022), 111. |
[52] |
H. Eltayeb, A. Kilicman, A note on double Laplace transform and telegraphic equations, Abstr. Appl. Anal., 2013 (2013), 932578. http://dx.doi.org/10.1155/2013/932578 doi: 10.1155/2013/932578
![]() |
[53] | M. Alquran, K. Al-Khaled, M. Ali, A. Ta'any, The combined Laplace transform-differential transform method for solving linear non-homogeneous PDEs, J. Math. Comput. Sci., 2 (2012), 690–701. |
[54] | K. Aboodh, The new integral transform "Aboodh transform'', Global Journal of Pure and Applied Mathematics, 9 (2013), 35–43. |
[55] | S. Aggarwal, R. Chauhan, A comparative study of Mohand and Aboodh transforms, International Journal of Research in Advent Technology, 7 (2019), 520–529. |
[56] |
M. Benattia, K. Belghaba, Application of the Aboodh transform for solving fractional delay differential equations, Universal Journal of Mathematics and Applications, 3 (2020), 93–101. http://dx.doi.org/10.32323/ujma.702033 doi: 10.32323/ujma.702033
![]() |
[57] |
B. Delgado, J. Macias-Diaz, On the general solutions of some non-homogeneous Div-curl systems with Riemann-Liouville and Caputo fractional derivatives, Fractal Fract., 5 (2021), 117. http://dx.doi.org/10.3390/fractalfract5030117 doi: 10.3390/fractalfract5030117
![]() |
[58] |
S. Alshammari, M. Al-Smadi, I. Hashim, M. Alias, Residual power series technique for simulating fractional Bagley-Torvik problems emerging in applied physics, Appl. Sci., 9 (2019), 5029. http://dx.doi.org/10.3390/app9235029 doi: 10.3390/app9235029
![]() |
[59] |
S. Almutlak, S. Parveen, S. Mahmood, A. Qamar, B. Alotaibi, S. El-Tantawy, On the propagation of cnoidal wave and overtaking collision of slow shear Alfvén solitons in low \beta-magnetized plasmas, Phys. Fluids, 35 (2023), 075130. http://dx.doi.org/10.1063/5.0158292 doi: 10.1063/5.0158292
![]() |
[60] |
W. Albalawi, S. El-Tantawy, A. Salas, On the rogue wave solution in the framework of a Korteweg-de Vries equation, Results Phys., 30 (2021), 104847. http://dx.doi.org/10.1016/j.rinp.2021.104847 doi: 10.1016/j.rinp.2021.104847
![]() |
[61] |
T. Hashmi, R. Jahangir, W. Masood, B. Alotaibi, S. Ismaeel, S. El-Tantawy, Head-on collision of ion-acoustic (modified) Korteweg-de Vries solitons in Saturn's magnetosphere plasmas with two temperature superthermal electrons, Phys. Fluids, 35 (2023), 103104. http://dx.doi.org/10.1063/5.0171220 doi: 10.1063/5.0171220
![]() |
[62] |
A. Wazwaz, W. Alhejaili, S. El-Tantawy, Physical multiple shock solutions to the integrability of linear structures of Burgers hierarchy, Phys. Fluids, 35 (2023), 123101. http://dx.doi.org/10.1063/5.0177366 doi: 10.1063/5.0177366
![]() |
[63] |
S. El-Tantawy, R. Matoog, R. Shah, A. Alrowaily, S. Ismaeel, On the shock wave approximation to fractional generalized Burger-Fisher equations using the residual power series transform method, Phys. Fluids, 36 (2024), 023105. http://dx.doi.org/10.1063/5.0187127 doi: 10.1063/5.0187127
![]() |
[64] |
S. El-Tantawy, A. Salas, H. Alyousef, M. Alharthi, Novel approximations to a nonplanar nonlinear Schrodinger equation and modeling nonplanar rogue waves/breathers in a complex plasma, Chaos Soliton. Fract., 163 (2022), 112612. http://dx.doi.org/10.1016/j.chaos.2022.112612 doi: 10.1016/j.chaos.2022.112612
![]() |
[65] |
S. El-Tantawy, A. Wazwaz, R. Schlickeiser, Solitons collision and freak waves in a plasma with Cairns-Tsallis particle distributions, Plasma Phys. Control. Fusion, 57 (2015), 125012. http://dx.doi.org/10.1088/0741-3335/57/12/125012 doi: 10.1088/0741-3335/57/12/125012
![]() |
1. | Meena Joshi, Shivangi Upadhyay, Anita Tomar, Mohammad Sajid, Geometry and Application in Economics of Fixed Point, 2023, 15, 2073-8994, 704, 10.3390/sym15030704 | |
2. | Nihal Taş, Irshad Ayoob, Nabil Mlaiki, Some common fixed-point and fixed-figure results with a function family on S_{b} -metric spaces, 2023, 8, 2473-6988, 13050, 10.3934/math.2023657 | |
3. | Irshad Ayoob, Ng Zhen Chuan, Nabil Mlaiki, Hardy-Rogers type contraction in double controlled metric-like spaces, 2023, 8, 2473-6988, 13623, 10.3934/math.2023691 | |
4. | Nabil Mlaiki, Nihal Özgür, Nihal Taş, Dania Santina, On the Fixed Circle Problem on Metric Spaces and Related Results, 2023, 12, 2075-1680, 401, 10.3390/axioms12040401 | |
5. | Jamilu Abubakar Jiddah, Mohammed Shehu Shagari, Maha Noorwali, Ahmad Aloqaily, Nabil Mlaiki, Hybrid fixed point theorems of graphic contractions with applications, 2024, 10, 24058440, e31269, 10.1016/j.heliyon.2024.e31269 | |
6. | Meena Joshi, Anita Tomar, 2024, Chapter 23, 978-3-031-57004-9, 221, 10.1007/978-3-031-57005-6_23 | |
7. | Muhammad Tariq, Muhammad Arshad, Eskandar Ameer, Ahmad Aloqaily, Suhad Subhi Aiadi, Nabil Mlaiki, On Relational Weak Fℜm,η-Contractive Mappings and Their Applications, 2023, 15, 2073-8994, 922, 10.3390/sym15040922 | |
8. | Fayyaz Ahmad, Kifayat Ullah, Junaid Ahmad, Ahmad Aloqaily, Nabil Mlaiki, Computational Analysis of a Novel Iterative Scheme with an Application, 2024, 12, 2079-3197, 192, 10.3390/computation12090192 | |
9. | Meena Joshi, Anita Tomar, On set-valued fixed points, their geometry and solution of boundary value problem for a differential inclusion, 2024, 0019-5588, 10.1007/s13226-024-00688-z | |
10. | Reham Qaralleh, Abdalla Tallafha, Wasfi Shatanawi, Some Fixed-Point Results in Extended S-Metric Space of Type (α,β), 2023, 15, 2073-8994, 1790, 10.3390/sym15091790 | |
11. | Jamshaid Ahmad, Abdullah Shoaib, Irshad Ayoob, Nabil Mlaiki, Common fixed points for ( \kappa _{G_{m}} )-contractions with applications, 2024, 9, 2473-6988, 15949, 10.3934/math.2024772 | |
12. | Koti N. V. V. Vara Prasad, Vinay Mishra, Zoran D. Mitrović, Dania Santina, Nabil Mlaiki, Unified interpolative of a Reich-Rus-Ćirić-type contraction in relational metric space with an application, 2024, 2024, 1029-242X, 10.1186/s13660-024-03176-4 | |
13. | Ivan D. Aranđelović, Zoran D. Mitrović, Ahmad Aloqaily, Nabil Mlaiki, The Results of Common Fixed Points in b-Metric Spaces, 2023, 15, 2073-8994, 1344, 10.3390/sym15071344 | |
14. | Mohammad Nazrul Islam Khan, Nahid Fatima, Novel theorems for the cotangent bundle endowed with metallic structures on a differentiable manifold, 2024, 10, 24058440, e32144, 10.1016/j.heliyon.2024.e32144 | |
15. | Syed Shah Khayyam, Muhammad Sarwar, Asad Khan, Nabil Mlaiki, Fatima M. Azmi, Solving Integral Equations via Fixed Point Results Involving Rational-Type Inequalities, 2023, 12, 2075-1680, 685, 10.3390/axioms12070685 | |
16. | Muhammad Sarwar, Syed Khayyam Shah, Zoran D. Mitrović, Aiman Mukheimer, Nabil Mlaiki, Almost Ćirić Type Contractions and Their Applications in Complex Valued b-Metric Spaces, 2023, 12, 2075-1680, 794, 10.3390/axioms12080794 | |
17. | Seema Mehra, Renu Chugh, Dania Santina, Nabil Mlaiki, An iterative approach for addressing monotone inclusion and fixed point problems with generalized demimetric mappings, 2024, 12, 26668181, 100953, 10.1016/j.padiff.2024.100953 | |
18. | Muhammad Din, Umar Ishtiaq, Muzammil Mukhtar, Salvatore Sessa, Hassan Ali Ghazwani, On Generalized Sehgal–Guseman-Like Contractions and Their Fixed-Point Results with Applications to Nonlinear Fractional Differential Equations and Boundary Value Problems for Homogeneous Transverse Bars, 2024, 12, 2227-7390, 541, 10.3390/math12040541 | |
19. | Seema Mehra, Renu Chugh, Salma Haque, Nabil Mlaiki, Iterative algorithm for solving monotone inclusion and fixed point problem of a finite family of demimetric mappings, 2023, 8, 2473-6988, 19334, 10.3934/math.2023986 | |
20. | Zeynep Kalkan, Aynur Şahin, Ahmad Aloqaily, Nabil Mlaiki, Some fixed point and stability results in b -metric-like spaces with an application to integral equations on time scales, 2024, 9, 2473-6988, 11335, 10.3934/math.2024556 | |
21. | Maliha Rashid, Lariab Shahid, Fatima Dar, Irshad Ayoob, Nabil Mlaiki, Existence of solution of a system of non-linear differential inclusions with non-local, integral boundary conditions via fixed points of hybrid contractions, 2024, 2024, 1687-2770, 10.1186/s13661-024-01902-x | |
22. | Sudipta Kumar Ghosh, Ozgur Ege, Junaid Ahmad, Ahmad Aloqaily, Nabil Mlaiki, On elliptic valued b-metric spaces and some new fixed point results with an application, 2024, 9, 2473-6988, 17184, 10.3934/math.2024835 | |
23. | Nilay Ekiz Yazici, Ozgur Ege, Nabil Mlaiki, Aiman Mukheimer, Controlled S-Metric-Type Spaces and Applications to Fractional Integrals, 2023, 15, 2073-8994, 1100, 10.3390/sym15051100 | |
24. | N. Seshagiri Rao, Ahmad Aloqaily, Nabil Mlaiki, Results pertaining to fixed points in ordered metric spaces with auxiliary functions and application to integral equation, 2024, 9, 2473-6988, 10832, 10.3934/math.2024528 | |
25. | Amna Naz, Samina Batul, Dur-e-Shehwar Sagheer, Irshad Ayoob, Nabil Mlaiki, F-Contractions Endowed with Mann’s Iterative Scheme in Convex Gb-Metric Spaces, 2023, 12, 2075-1680, 937, 10.3390/axioms12100937 | |
26. | Khairul Habib Alam, Yumnam Rohen, Anita Tomar, Mohammad Sajid, On geometry of fixed figures via φ−interpolative contractions and application of activation functions in neural networks and machine learning models, 2025, 16, 20904479, 103182, 10.1016/j.asej.2024.103182 | |
27. | Neeraj Kumar, Seema Mehra, Dania Santina, Nabil Mlaiki, Some fixed point results concerning various contractions in extended b- metric space endowed with a graph, 2025, 25, 25900374, 100524, 10.1016/j.rinam.2024.100524 | |
28. | Mohammed Shehu Shagari, Rosemary O. Ogbumba, Maha Noorwali, Trad Alotaibi, Afis Saliu, Fixed Point Results of F F ‐Contractive–Type Operators With Applications, 2025, 0170-4214, 10.1002/mma.10735 | |
29. | Amna Naz, Samina Batul, Sarah Aljohani, Nabil Mlaiki, Results for cyclic contractive mappings of Kannan and Chatterjea type equipped with Mann’s iterative scheme, 2025, 26668181, 101145, 10.1016/j.padiff.2025.101145 | |
30. | R. P. Pant, Anita Tomar, Meena Joshi, Non-contractive mappings and application to a drug diffusion problem, 2025, 26, 1989-4147, 221, 10.4995/agt.2025.21595 | |
31. | Elif Kaplan, Nihal Taş, Salma Haque, Nabil Mlaiki, Multiplicative modular metric spaces and some fixed point results, 2025, 2025, 1029-242X, 10.1186/s13660-025-03303-9 | |
32. | Usman Shehzad, Samina Batul, Dur-e-Shehwar Sagheer, Irshad Ayoob, Nabil Mlaiki, Fixed point results via fuzzy mappings in b-metric spaces and an application to differential equations, 2025, 2025, 1029-242X, 10.1186/s13660-025-03317-3 |