This study focuses on developing efficient numerical techniques for solving the fractional Keller-Segel (KS) model, which is critical in explaining chemotaxis events. Within the Caputo operator framework, the study applied two unique methodologies: The Aboodh residual power series method (ARPSM) and the Aboodh transform iteration method (ATIM). These approaches were used to find precise solutions to the fractional KS equation, resulting in a better understanding of chemotactic behavior in biological systems. The comparative examination of the ARPSM and ATIM revealed their distinct strengths and applications in solving complicated fractional models. The work advances numerical approaches for fractional differential equations and improves our understanding of chemotaxis dynamics using a precise modeling approach.
Citation: Nader Al-Rashidi. Innovative approaches to fractional modeling: Aboodh transform for the Keller-Segel equation[J]. AIMS Mathematics, 2024, 9(6): 14949-14981. doi: 10.3934/math.2024724
[1] | Ahmad Mohammed Alghamdi, Sadek Gala, Maria Alessandra Ragusa . A regularity criterion of weak solutions to the 3D Boussinesq equations. AIMS Mathematics, 2017, 2(3): 451-457. doi: 10.3934/Math.2017.2.451 |
[2] | Sadek Gala, Maria Alessandra Ragusa . A logarithmically improved regularity criterion for the 3D MHD equations in Morrey-Campanato space. AIMS Mathematics, 2017, 2(1): 16-23. doi: 10.3934/Math.2017.1.16 |
[3] | Li Lu . One new blow-up criterion for the two-dimensional full compressible magnetohydrodynamic equations. AIMS Mathematics, 2023, 8(7): 15876-15891. doi: 10.3934/math.2023810 |
[4] | Sadek Gala, Mohamed Mechdene, Maria Alessandra Ragusa . Logarithmically improved regularity criteria for the Boussinesq equations. AIMS Mathematics, 2017, 2(2): 336-347. doi: 10.3934/Math.2017.2.336 |
[5] | Jae-Myoung Kim . Local interior regularity for the 3D MHD equations in nonendpoint borderline Lorentz space. AIMS Mathematics, 2021, 6(3): 2440-2453. doi: 10.3934/math.2021148 |
[6] | Yanping Zhou, Xuemei Deng, Qunyi Bie, Lingping Kang . Energy conservation for the compressible ideal Hall-MHD equations. AIMS Mathematics, 2022, 7(9): 17150-17165. doi: 10.3934/math.2022944 |
[7] | Sadek Gala . A note on the Liouville type theorem for the smooth solutions of the stationary Hall-MHD system. AIMS Mathematics, 2016, 1(3): 282-287. doi: 10.3934/Math.2016.3.282 |
[8] | Qiang Li, Mianlu Zou . A regularity criterion via horizontal components of velocity and molecular orientations for the 3D nematic liquid crystal flows. AIMS Mathematics, 2022, 7(5): 9278-9287. doi: 10.3934/math.2022514 |
[9] | Tariq Mahmood, Zhaoyang Shang . Blow-up criterion for incompressible nematic type liquid crystal equations in three-dimensional space. AIMS Mathematics, 2020, 5(2): 746-765. doi: 10.3934/math.2020051 |
[10] | Zhaoyang Shang . Osgood type blow-up criterion for the 3D Boussinesq equations with partial viscosity. AIMS Mathematics, 2018, 3(1): 1-11. doi: 10.3934/Math.2018.1.1 |
This study focuses on developing efficient numerical techniques for solving the fractional Keller-Segel (KS) model, which is critical in explaining chemotaxis events. Within the Caputo operator framework, the study applied two unique methodologies: The Aboodh residual power series method (ARPSM) and the Aboodh transform iteration method (ATIM). These approaches were used to find precise solutions to the fractional KS equation, resulting in a better understanding of chemotactic behavior in biological systems. The comparative examination of the ARPSM and ATIM revealed their distinct strengths and applications in solving complicated fractional models. The work advances numerical approaches for fractional differential equations and improves our understanding of chemotaxis dynamics using a precise modeling approach.
We generalize the classical Halanay inequality to encompass fractional-order systems with both discrete and distributed neutral delays. This inequality, originally formulated for integer-order systems, is now generalized to non-integer orders.
Lemma 1.1. Consider a nonnegative function w(t) that satisfies the inequality
w′(t)≤−K1w(t)+K2supt−τ≤s≤tw(s),t≥a, |
where 0<K2<K1. Under these conditions, positive constants K3 and K4 exist such that
w(t)≤K3e−K4(t−a),t≥a. |
Halanay first introduced this inequality while studying the stability of a specific differential equation [10]
υ′(t)=−Aυ(t)+Bυ(t−τ),τ>0. |
Since then, the inequality has been generalized to include variable coefficients and delays of varying magnitude, both bounded and unbounded [1,25,26]. These generalizations have found applications in Hopfield neural networks and the analysis of Volterra functional equations, particularly in the context of problems described by the following system [12,16,27]:
{x′i(t)=−cixi(t)+∑nj=1bijfj(xj(t−τ))+∑nj=1aijfj(xj(t))+Ii,t>0,xi(t)=ϕi(t),−τ≤t≤0, i=1,...,n. |
Such problems arise in various fields, including parallel computing, cryptography, image processing, combinatorial optimization, signal theory, and geology [15,17,18].
Additionally, a generalization of the Halanay inequality to systems with distributed delays is presented in [21]:
w′(x)≤−B(x)w(x)+A(x)∫∞0k(s)w(x−s)ds,x≥0. |
The solutions exhibit exponential decay if the kernels satisfy the conditions
∫∞0eβsk(s)ds<∞, |
for some β>0, and
A(x)∫∞0k(s)ds≤B(x)−C,C>0,x∈R. |
See also [22] for further details.
This study broadens the scope of Halanay's inequality to encompass fractional-order systems. The justification for using fractional derivatives is provided in [2,3]. We also consider neutral delays, where delays appear in the leading derivative. Specifically, we analyze the stability of the following problem:
{Dφ,αC[w(t)−pw(t−υ)]≤−qw(t)+∫taw(r)k(t−r)dr, p>0, 0<α<1, υ,t>a,w(t)=ϖ(t),a−υ≤t≤a. | (1.1) |
We establish sufficient conditions on the kernel k to guarantee Mittag-Leffler stability, ensuring that the solutions satisfy
w(t)≤AEα(−q[φ(t)−φ(a)]α),t>a. |
We provide examples of function families that satisfy our assumptions. As an application, we consider a fractional-order Cohen-Grossberg neural network system with neutral delays [9]. This system represents a more general form of the traditional Hopfield neural network.
There is extensive research on the existence, stability, and long-term behavior of Cohen-Grossberg neural network systems. Our focus is on research that specifically addresses networks with time delays or fractional-order dynamics. For integer-order neutral Cohen-Grossberg systems, refer to [5,7,24]. The fractional case with discrete delays was explored in [14]. While the Halanay inequality has been adapted for fractional-order systems with discrete delays in [4,11,28], we are unaware of any work addressing our specific problem (1.1).
The techniques used for integer-order systems are not directly applicable to the fractional-order case. For example, the Mittag-Leffler functions lack the semigroup property, and estimating the expression Eα(−q(φ(t−υ)−φ(a))α)/Eα(−q(φ(t)−φ(a))α) is challenging for convergence analysis. The ideal decay rate would be Eα(−q(φ(t)−φ(a))α), but the neutral delay introduces new challenges, particularly near ν. Approximating with (φ(t)−φ(a))−α (using Mainardi's conjecture) does not fully resolve these issues.
This paper is organized into eight sections, beginning with background information in Section 2. Section 3 presents our inequality for systems with discrete time delays, and Section 4 discusses two potential kernel functions. Section 5 investigates a fractional Halanay inequality in the presence of distributed neutral delays. Solutions of arbitrary signs for the problem in Section 3 are addressed in Section 6, and Section 7 applies our results to a Cohen-Grossberg system with neutral delays. Section 8 provides the conclusion, summarizing the findings and highlighting directions for future research.
This section provides fundamental definitions and lemmas essential for the subsequent analysis. Throughout the paper, we consider [a,b] to be an infinite or finite interval, and φ to be an n- continuously differentiable function on [a,b] such that φ is increasing and φ′(ϰ)≠0 on [a,b].
Definition 2.1. The φ-Riemann-Liouville fractional integral of a function ω with respect to a function φ is defined as
Iφ,αω(z)=1Γ(α)∫za[φ(z)−φ(s)]α−1ω(s)φ′(s)ds,α>0,z>a |
provided that the right side exists.
Definition 2.2. The φ-Caputo derivative of order α>0 is defined by
Dφ,αCω(ϰ)=Iφ,n−α(1φ′(ϰ)ddϰ)nω(ϰ), |
which can be expressed equivalently as
Dφ,αCω(ϰ)=1Γ(n−α)∫ϰa[φ(ϰ)−φ(τ)]n−α−1φ′(τ)ω[n]φ(τ)dτ, ϰ>a, |
where
ω[n]φ(ϰ)=(1φ′(ϰ)ddϰ)nω(ϰ), n=−[−α]. |
Particularly, when 0<α<1
Dφ,αCω(ϰ)=Iφ,1−α(1φ′(ϰ)ddϰ)ω(ϰ)=1Γ(1−α)∫ϰa[φ(ϰ)−φ(τ)]−αω′(τ)dτ. |
The Mittag-Leffler functions used in this context are defined as follows:
Eα(y):=∞∑n=0ynΓ(1+αn), Re(α)>0, |
and
Eα,β(y):=∞∑n=0ynΓ(β+αn), Re(β)>0, Re(α)>0. |
Lemma 2.1. [13] The Cauchy problem
{Dφ,αCy(ζ)=λy(ζ),0<α≤1, ζ>a,λ∈Ry(a)=ya, | (2.1) |
has the solution
y(ζ)=yaEα(λ[φ(ζ)−φ(a)]α),ζ≥a. |
Lemma 2.2. [13] The Cauchy problem
{Dφ,αCy(ζ)=λy(ζ)+h(ζ),0<α≤1, λ∈R, ζ>a,y(a)=ya∈R, | (2.2) |
admits the solution for ζ≥a
y(ζ)=yaEα(λ[φ(ζ)−φ(a)]α)+∫ζa[φ(ζ)−φ(s)]α−1Eα,α(λ[φ(ζ)−φ(s)]α)φ′(s)h(s)ds. |
Lemma 2.3. For λ,ν,ω>0, the following inequality is valid for all z>a:
∫za[φ(s)−φ(a)]λ−1[φ(z)−φ(s)]ν−1e−ω[φ(s)−φ(a)]φ′(s)ds≤C[φ(z)−φ(a)]ν−1, |
where
C=max{1,21−ν}Γ(λ)[1+λ(λ+1)/ν]ω−λ. |
Proof. For z>a, let
I(z)=[φ(z)−φ(a)]1−ν∫za[φ(s)−φ(a)]λ−1[φ(z)−φ(s)]ν−1e−ω[φ(s)−φ(a)]φ′(s)ds. |
Set ξ[φ(z)−φ(a)]=φ(s)−φ(a). Then, [φ(z)−φ(a)]dξ=φ′(s)ds and
I(z)=[φ(z)−φ(a)]λ∫10(1−ξ)ν−1ξλ−1e−ωξ[φ(z)−φ(a)]dξ, z>a. |
As for 0≤ξ<1/2, we have (1−ξ)ν−1≤max{1,21−ν}, therefore
I(z)≤max{1,21−ν}[φ(z)−φ(a)]λ∫1/20ξλ−1e−ωξ[φ(z)−φ(a)]dξ+[φ(z)−φ(a)]λ∫11/2(1−ξ)ν−1ξλ−1e−ωξ[φ(z)−φ(a)]dξ. | (2.3) |
Let u=ωξ[φ(z)−φ(a)]. Then, dξ=[φ(z)−φ(a)]−1ω−1du and
[φ(z)−φ(a)]λ∫1/20ξλ−1e−ωξ[φ(z)−φ(a)]dξ≤ω−λ∫∞0uλ−1e−udu=ω−λΓ(λ). | (2.4) |
If 1≤ωξ[φ(z)−φ(a)], then
eωξ[φ(z)−φ(a)]≥[ωξ[φ(z)−φ(a)]]1+[λ]Γ([λ]+2)≥[ωξ[φ(z)−φ(a)]]λΓ(λ+2). |
Therefore, when 1/2<ξ≤1,
ξλ−1e−ωξ[φ(z)−φ(a)]≤ξλ−1Γ(2+λ)[ωξ[φ(z)−φ(a)]]λ≤2ω−λΓ(λ+2)[φ(z)−φ(a)]λ, |
and consequently
[φ(z)−φ(a)]λ∫11/2(1−ξ)ν−1ξλ−1e−ωξ[φ(z)−φ(a)]dξ≤[φ(z)−φ(a)]λ∫11/2(1−ξ)ν−12ω−λΓ(2+λ)[φ(z)−φ(a)]λdξ=2ω−λΓ(2+λ)∫11/2(1−ξ)ν−1dξ=21−νω−λΓ(λ+2)ν. |
When ωξ[φ(z)−φ(a)]<1, it implies that [ωξ[φ(z)−φ(a)]]λ<1≤eωξ[φ(z)−φ(a)]. Consequently,
[φ(z)−φ(a)]λ∫11/2ξλ−1(1−ξ)ν−1e−ωξ[φ(z)−φ(a)]dξ<[φ(z)−φ(a)]λ∫11/2ξλ−1(1−ξ)ν−1[ωξ[φ(z)−φ(a)]]−λdξ<2ω−λ∫11/2(1−ξ)ν−1dξ=21−νω−λν. | (2.5) |
Taking into account (2.3)–(2.5), we infer that
I(z)≤max{1,21−ν}ω−λΓ(λ)+21−νω−λΓ(λ+2)ν≤max{1,21−ν}ω−λΓ(λ)(1+λ(λ+1)ν), z>a. |
The proof is complete.
Lemma 2.4. [8, (4.4.10), (4.9.4)] For β>0, ν>0, and λ,λ∗∈C, λ≠λ∗, we have
∫ϰ0zβ−1Eα,β(λzα)(ϰ−z)ν−1Eα,ν(λ∗(ϰ−z)α)dz=λEα,β+ν(λϰα)−λ∗Eα,β+ν(λ∗ϰα)λ−λ∗ϰβ+ν−1, |
and for σ>0, γ>0,
Iσzγ−1Eα,γ(pzα)(ϰ)=ϰσ+γ−1Eα,σ+γ(pϰα). |
Lemma 2.5. For β>0, ν>0, and λ,λ∗∈C, λ≠λ∗, we have
∫ϰaEα,β(λ[φ(z)−φ(a)]α)[φ(ϰ)−φ(z)]ν−1[φ(z)−φ(a)]β−1×Eα,ν(λ∗[φ(ϰ)−φ(z)]α)φ′(z)dz=[φ(ϰ)−φ(a)]β+ν−1λ∗Eα,β+ν(λ∗[φ(ϰ)−φ(a)]α)−λEα,β+ν(λ[φ(ϰ)−φ(a)]α)λ∗−λ, |
and for σ>0, γ>0,
Iφ,σ[φ(z)−φ(a)]γ−1Eα,γ(p[φ(z)−φ(a)]α)(ϰ)=[φ(ϰ)−φ(a)]σ+γ−1×Eα,σ+γ(p[φ(ϰ)−φ(a)]α). | (2.6) |
Proof. Let u=φ(ϰ)−φ(z). Then,
∫ϰaEα,β(λ[φ(z)−φ(a)]α)[φ(ϰ)−φ(z)]ν−1[φ(z)−φ(a)]β−1×Eα,ν(λ∗[φ(ϰ)−φ(z)]α)φ′(z)dz=∫φ(ϰ)−φ(a)0Eα,β(λ[φ(ϰ)−φ(a)−u]α)[φ(ϰ)−φ(a)−u]β−1uν−1Eα,ν(λ∗uα)du. |
At this point, we can utilize Lemma 2.4 to derive the following:
∫ϰaEα,β(λ[φ(z)−φ(a)]α)[φ(ϰ)−φ(z)]ν−1[φ(z)−φ(a)]β−1×Eα,ν(λ∗[φ(ϰ)−φ(z)]α)φ′(z)dz=[φ(ϰ)−φ(a)]β+ν−1λ∗Eα,β+ν(λ∗[φ(ϰ)−φ(a)]α)−λEα,β+ν(λ[φ(ϰ)−φ(a)]α)λ∗−λ. |
To prove the second formula in the lemma, we have
Iφ,σ[φ(z)−φ(a)]γ−1Eα,γ(p[φ(z)−φ(a)]α)(ϰ)=1Γ(σ)∫ϰaEα,γ(p[φ(z)−φ(a)]α)[φ(ϰ)−φ(z)]σ−1[φ(z)−φ(a)]γ−1φ′(z)dz. |
From the first formula in the lemma, with β=γ, ν=σ, λ=p, λ∗=0, we obtain
Iφ,σ[φ(z)−φ(a)]γ−1Eα,γ(p[φ(z)−φ(a)]α)(ϰ)=1Γ(σ)∫ϰa[φ(z)−φ(a)]γ−1Eα,γ(p[φ(z)−φ(a)]α)[φ(ϰ)−φ(z)]σ−1φ′(z)dz=[φ(ϰ)−φ(a)]γ+σ−1Eα,γ+σ(p[φ(ϰ)−φ(a)]α), |
where we have used
Eα,σ(λ∗[φ(ϰ)−φ(z)]α)=1Γ(σ). |
Mainardi's conjecture. [19] For fixed γ with 0<γ<1, the following holds:
11+qΓ(1−γ)tγ≤Eγ(−qtγ)≤1qΓ(1+γ)−1tγ+1,q, t≥0. | (2.7) |
This result was later established in [6,23].
To start, we will introduce the concept of Mittag-Leffler stability.
Definition 3.1. For 0<α<1, a solution v(z) is defined as α -Mittag-Leffler stable if there exist positive constants A and γ such that
‖v(z)‖≤AEα(−γ[φ(z)−φ(a)]α),z>a, |
where ‖.‖ represents a specific norm.
Theorem 3.1. Let u(t) be a nonnegative function fulfilling the conditions
Dφ,αC[u(t)−pu(t−υ)]≤−qu(t)+∫tau(s)k(t−s)ds,0<α<1,t>a, | (3.1) |
with the initial condition
u(t)=ϖ(t)≥0,a−υ≤t≤a, | (3.2) |
where k is a nonnegative function integrable over its domain, and q>0. Assume p>0, and that k satisfies the following inequality for some M>0:
∫taEα,α(−q[φ(t)−φ(s)]α)[φ(t)−φ(s)]α−1×(∫saEα(−q[φ(σ)−φ(a)]α)k(s−σ)dσ)φ′(s)ds≤MEα(−q[φ(t)−φ(a)]α),t>a. | (3.3) |
Further, assume that the constant M satisfies
M<1−1(φ(a+υ)−φ(a))α(1q+Γ(1−α)[φ(a+3υ)−φ(a)]α)p, | (3.4) |
with the additional condition
1(φ(a+υ)−φ(a))α(1q+Γ(1−α)[φ(a+3υ)−φ(a)]α)p<1. | (3.5) |
Then, u(t) exhibits Mittag-Leffler decay, i.e.,
u(t)≤CEα(−q[φ(t)−φ(a)]α),t>a |
for some constant C>0.
Proof. Solutions of (3.1) and (3.2) will be compared to those of
{Dφ,αC[w(t)−pw(t−υ)]=−qw(t)+∫taw(s)k(t−s)ds,0<α<1,t>a,w(t)=ϖ(t)≥0,a−υ≤t≤a. | (3.6) |
The equation presented in (3.6) can be expressed equivalently as
Dφ,αC[w(t)−pw(t−υ)]=−q[w(t)−pw(t−υ)]+∫tak(t−s)w(s)ds−qpw(t−υ),t>a. |
This permits to profit from the form
w(t)−pw(t−υ)=[ϖ(a)−pϖ(a−υ)]Eα(−q[φ(t)−φ(a)]α)+∫ta[φ(t)−φ(s)]α−1Eα,α(−q[φ(t)−φ(s)]α)×(−qpw(s−υ)+∫sak(s−σ)w(σ)dσ)φ′(s)ds. |
Capitalizing on the nonnegativity of the solution, we find for t>a,
w(t)≤ϖ(a)Eα(−q(φ(t)−φ(a))α)+pw(t−υ)+∫taEα,α(−q[φ(t)−φ(s)]α)×[φ(t)−φ(s)]α−1(∫sak(s−σ)w(σ)dσ)φ′(s)ds. | (3.7) |
Therefore, for t>a,
w(t)Eα(−q(φ(t)−φ(a))α)≤ϖ(a)+pEα(−q(φ(t)−φ(a))α)w(t−υ)+1Eα(−q(φ(t)−φ(a))α)∫ta[φ(t)−φ(s)]α−1Eα,α(−q[φ(t)−φ(s)]α)×(∫sak(s−σ)Eα(−q(φ(σ)−φ(a))α)w(σ)Eα(−q(φ(σ)−φ(a))α)dσ)φ′(s)ds, |
and
w(t)Eα(−q(φ(t)−φ(a))α)≤ϖ(a)+pEα(−q(φ(t)−φ(a))α)w(t−υ)+1Eα(−q(φ(t)−φ(a))α)∫ta[φ(t)−φ(s)]α−1×Eα,α(−q[φ(t)−φ(s)]α)×(∫sak(s−σ)Eα(−q(φ(σ)−φ(a))α)dσ)φ′(s)ds×supa≤σ≤tw(σ)Eα(−q(φ(σ)−φ(a))α)≤ϖ(a)+pEα(−q(φ(t)−φ(a))α)w(t−ν)+Msupa≤σ≤tw(σ)Eα(−q(φ(σ)−φ(a))α). |
We will repeatedly utilize the following estimation:
1Eα(−q(φ(t)−φ(a))α)∫taEα,α(−q[φ(t)−φ(s)]α)[φ(t)−φ(s)]α−1×(∫sak(s−σ)w(σ)dσ)φ′(s)ds=1Eα(−q(φ(t)−φ(a))α)∫taEα,α(−q[φ(t)−φ(s)]α)[φ(t)−φ(s)]α−1×(∫saEα(−q[φ(σ)−φ(a)]α)k(s−σ)w(σ)Eα(−q[φ(σ)−φ(a)]α)dσ)φ′(s)ds≤Msupa≤σ≤tw(σ)Eα(−q(φ(σ)−φ(a))α),t>a. | (3.8) |
Then, for t>a, the following inequality holds:
w(t)Eα(−q[φ(t)−φ(a)]α)≤ϖ(a)+pEα(−q[φ(t)−φ(a)]α)w(t−υ)+Msupa≤σ≤tw(σ)Eα(−q[φ(σ)−φ(a)]α). | (3.9) |
This inequality will serve as our initial reference.
For t∈[a,a+υ], since Eα(−q[φ(t)−φ(a)]α) is decreasing, it follows that
Eα(−q[φ(t)−φ(a)]α)≥Eα(−q[φ(a+υ)−φ(a)]α), |
and hence
w(t)Eα(−q[φ(t)−φ(a)]α)≤(1+pEα(−q[φ(a+υ)−φ(a)]α)supa−υ≤σ≤aϖ(σ)+Msupa≤σ≤tw(σ)Eα(−q[φ(σ)−φ(a)]α), |
or
(1−M)w(t)Eα(−q(φ(t)−φ(a))α)≤(1+pEα(−q(φ(a+υ)−φ(a))α)supa−υ≤σ≤aϖ(σ). | (3.10) |
If t∈[a+υ,a+2υ], owing to relations (3.9) and (3.10), we find
w(t)Eα(−q(φ(t)−φ(a))α)≤supa−υ≤σ≤aϖ(σ)+p1−M(1+pEα(−q(φ(a+υ)−φ(a))α)×Eα(−q(φ(t−υ)−φ(a))α)Eα(−q(φ(t)−φ(a))α)supa−ν≤σ≤aϖ(σ)+Msupa≤σ≤tw(σ)Eα(−q(φ(σ)−φ(a))α). |
Observe that
Eα(−q(φ(t−υ)−φ(a))α)Eα(−q(φ(t)−φ(a))α)≤1Eα(−q(φ(t)−φ(a))α)≤1Eα(−q(φ(2υ+a)−φ(a))α)≤1+qΓ(1−α)(φ(2υ+a)−φ(a))α=:A. | (3.11) |
Therefore,
w(t)Eα(−q(φ(t)−φ(a))α)≤[1+A(Eα(−q(φ(υ+a)−φ(a))α+p)pEα(−q(φ(υ+a)−φ(a))α(1−M)]supa−υ≤σ≤aϖ(σ)+Msupa≤σ≤tw(σ)Eα(−q(φ(σ)−φ(a))α), |
and consequently,
w(t)Eα(−q(φ(t)−φ(a))α)(1−M)≤[1+A(1−M)p+AEα(−q[φ(a+υ)−φ(a)]α)(1−M)p2]supa−υ≤σ≤aϖ(σ). | (3.12) |
Notice that we will write (3.12) as
w(t)Eα(−q(φ(t)−φ(a))α)(1−M)≤AEα(−q(φ(υ+a)−φ(a))α)×[1+p1−M+(p1−M)2]supa−υ≤σ≤aϖ(σ). | (3.13) |
When t∈[a+2ν,a+3ν], the estimations
φ(t)−φ(a)φ(t−υ)−φ(a)≤φ(a+3υ)−φ(a)φ(a+υ)−φ(a), |
together with (2.7), imply for t≥a+2ν,
Eα(−q(φ(t−υ)−φ(a))α)Eα(−q(φ(t)−φ(a))α)≤1+q(φ(t)−φ(a))αΓ(1−α)1+q(φ(t−υ)−φ(a))αΓ(1+α)−1≤1+q(φ(t)−φ(a))αΓ(1−α)qΓ(1+α)−1(φ(t−υ)−φ(a))α≤Γ(1+α)q(φ(t−υ)−φ(a))α+Γ(1+α)(φ(t)−φ(a))αΓ(1−α)(φ(t−υ)−φ(a))α≤Γ(1+α)q(φ(a+υ)−φ(a))α+(φ(a+3υ)−φ(a))αΓ(1+α)Γ(1−α)(φ(a+υ)−φ(a))α≤Γ(1+α)(φ(a+υ)−φ(a))α×(1q+Γ(1−α)(φ(a+3υ)−φ(a))α), | (3.14) |
Notice that Γ(1+α) can be approximated by one.
By virtue of relations (3.13) and (3.14), having in mind (3.9), we infer
w(t)Eα(−q(φ(t)−φ(a))α)≤ϖ(a)+p1−MEα(−q(φ(t−υ)−φ(a))α)Eα(−q(φ(t)−φ(a))α)×AEα(−q(φ(a+υ)−φ(a))α)×[1+p1−M+(p1−M)2]supa−υ≤σ≤aϖ(σ)+Msupa≤σ≤tw(σ)Eα(−q(φ(σ)−φ(a))α), |
or
w(t)Eα(−q[φ(t)−φ(a)]α)(1−M)≤supa−υ≤σ≤aϖ(σ){1+p1−MAVEα(−q[φ(υ+a)−φ(a)]α)×[1+p1−M+(p1−M)2]}, | (3.15) |
where
V:=1(φ(a+υ)−φ(a))α(1q+Γ(1−α)[φ(a+3υ)−φ(a)]α). |
As
AVEα(−q[φ(a+υ)−φ(a)]α)>1, |
we can rewrite Eq (3.15) as follows:
(1−M)w(t)Eα(−q[φ(t)−φ(a)]α)≤supa−υ≤σ≤aϖ(σ)AEα(−q[φ(υ+a)−φ(a)]α)×{1+pV1−M+(pV1−M)2+(pV1−M)3}. |
We now make the following claim.
Claim. For t∈[a+(n−1)υ,a+nυ],
(1−M)w(t)Eα(−q(φ(t)−φ(a))α)≤AEα(−q(φ(υ+a)−φ(a))α)×∑nk=0(pV1−M)ksupa−ν≤σ≤aϖ(σ). |
It is evident that the assertion is valid for the cases n=1, 2, and 3. Assume that it holds for n, i.e., on [a+(n−1)υ,a+nυ]. Now, let t∈[a+nυ,a+υ(n+1)]. Utilizing (3.9), we derive
w(t)Eα(−q[φ(t)−φ(a)]α)≤supa−υ≤σ≤aϖ(σ)+pEα(−q[φ(t−υ)−φ(a)]α)(1−M)Eα(−q[φ(t)−φ(a)]α)×AEα(−q[φ(a+υ)−φ(a)]α)∑nk=0(pV1−M)ksupa−υ≤σ≤aϖ(σ)+Msupa≤σ≤tw(σ)Eα(−q[φ(σ)−φ(a)]α). |
and by (3.14)
w(t)Eα(−q(φ(t)−φ(a))α)(1−M)≤[1+Vp1−MAEα(−q(φ(a+υ)−φ(a))α)∑nk=0(Vp1−M)k]supa−υ≤σ≤aϖ(σ)≤AEα(−q(φ(a+υ)−φ(a))α)[1+∑n+1k=1(Vp1−M)k]supa−υ≤σ≤aϖ(σ)=AEα(−q[φ(a+υ)−φ(a)]α)∑n+1k=0(Vp1−M)ksupa−υ≤σ≤aϖ(σ). |
Therefore, the claim holds true. Then, for t>a,
w(t)≤[AEα(−q[φ(a+υ)−φ(a)]α)(1−M)∑∞k=0(pV1−M)ksupa−υ≤σ≤aϖ(σ)]×Eα(−q(φ(t)−φ(a))α). | (3.16) |
The series in (3.16) converges due to (3.4) and (3.5). The proof is complete.
In this section, we identify two classes of functions that satisfy the conditions of the theorem.
First class: Consider the set of functions k that fulfill the following inequality for all s≥a:
∫saEα(−q[φ(σ)−φ(a)]α)k(s−σ)dσ≤C1[φ(s)−φ(a)]λ−1,C1,λ>0. | (4.1) |
The family of functions k(t−s) defined as
k(t−s)≤C2[φ(t)−φ(s)]−αe−b[φ(s)−φ(a)]φ′(s) |
satisfies the specified relation when the constants b and C2 are carefully chosen. Indeed, since
Eα(−qtα)≤11+qtαΓ(1+α)=Γ(1+α)Γ(1+α)+qtα≤Γ(1+α)qtα,t>0, | (4.2) |
it follows that
∫saEα(−q[φ(σ)−φ(a)]α)k(s−σ)dσ≤C2Γ(1+α)q∫sa[φ(σ)−φ(a)]−α[φ(s)−φ(σ)]−αe−b[φ(σ)−φ(a)]φ′(σ)dσ≤2αC2Γ(1+α)Γ(1−α)[3−α]bα−1q[φ(s)−φ(a)]−α,s>a. |
Therefore, (4.1) holds with
C1:=2αC2Γ(1+α)Γ(1−α)[3−α]bα−1q,λ:=1−α. |
By applying formula (2.6), we obtain
∫taEα,α(−q[φ(t)−φ(s)]α)[φ(t)−φ(s)]α−1×(∫sak(s−σ)Eα(−q[φ(σ)−φ(a)]α)dσ)φ′(s)ds≤C1∫taEα,α(−q[φ(t)−φ(s)]α)[φ(t)−φ(s)]α−1[φ(s)−φ(a)]−αφ′(s)ds≤C1Γ(α)Eα,1(−q[φ(t)−φ(a)]α). | (4.3) |
To ensure that assumption (3.4) is met, we can select C1 (or C2 for the specific example) such that
C1Γ(α)<1−1(φ(a+υ)−φ(a))α(1q+Γ(1−α)[φ(a+3υ)−φ(a)]α)p. |
Second class: Assume that k(t−s)≤C3[φ(t)−φ(s)]α−1Eα,α(−b[φ(t)−φ(s)]α)φ′(s) for some b>0 and C3>0 to be determined. A double use of (2.6) and (4.2) gives
C3∫ta[φ(t)−φ(s)]α−1Eα,α(−q[φ(t)−φ(s)]α)×(∫sa[φ(s)−φ(σ)]α−1Eα,α(−b[φ(s)−φ(σ)]α)Eα(−q[φ(σ)−φ(a)]α)φ′(σ)dσ)φ′(s)ds≤C3Γ(1+α)q∫taEα,α(−q[φ(t)−φ(s)]α)[φ(t)−φ(s)]α−1×(∫sa[φ(s)−φ(σ)]α−1Eα,α(−b[φ(s)−φ(σ)]α)[φ(σ)−φ(a)]−αφ′(σ)dσ)φ′(s)ds≤C3Γ(α)Γ(1+α)q∫taEα,α(−q[φ(t)−φ(s)]αEα,1(−b[φ(s)−φ(a)]α[φ(t)−φ(s)]α−1φ′(s)ds≤C3Γ2(1+α)Γ(α)qb∫taEα,α(−q[φ(t)−φ(s)]α[φ(t)−φ(s)]α−1[φ(s)−φ(a)]−αφ′(s)ds≤C3Γ2(1+α)Γ2(α)qbEα,1(−q[φ(t)−φ(a)]α. | (4.4) |
Clearly, M=C3Γ2(1+α)Γ2(α)qb. It suffices now to impose the condition on C3 and/or the constant b in order to fulfill the condition on M.
In this section, we will examine the inequality that arises when the neutral delay is distributed,
{Dφ,αC[u(t)−p∫tau(s)g(t−s)ds]≤−qu(t)+∫tau(s)k(t−s)ds, t,υ>a,0<α<1, p>0,u(t)=u0≥0,t∈[a−υ,a], | (5.1) |
which we will contrast with
{Dφ,αC[w(t)−p∫taw(s)g(t−s)ds]=−qw(t)+∫taw(s)k(t−s)ds,t,υ>a,0<α<1, p>0,w(t)=w0=u0≥0,t∈[a−υ,a]. | (5.2) |
We assume g is a continuous function (to be determined later) and that the solutions are nonnegative.
Let us reformulate this as
{Dφ,αC[w(t)−p∫taw(s)g(t−s)ds]=−q[w(t)−p∫taw(s)g(t−s)ds]−qp∫taw(s)g(t−s)ds+∫taw(s)k(t−s)ds,t,υ>a,0<α<1, p>0w(t)=w0≥0,t∈[a−υ,a]. |
Therefore,
w(t)−p∫taw(s)g(t−s)ds=Eα(−q[φ(t)−φ(a)]α)w0+∫ta[φ(t)−φ(s)]α−1Eα,α(−q[φ(t)−φ(s)]α)×(−qp∫sag(s−σ)w(σ)dσ+∫sak(s−σ)w(σ)dσ)φ′(s)ds, |
and, for t>a,
w(t)≤Eα(−q[φ(t)−φ(a)]α)w0+p∫tag(t−s)w(s)ds+∫taEα,α(−q[φ(t)−φ(s)]α)×[φ(t)−φ(s)]α−1(∫sak(s−σ)w(σ)dσ)φ′(s)ds. | (5.3) |
Dividing both sides of (5.3) by Eα(−q[φ(t)−φ(a)]α), we find
w(t)Eα(−q[φ(t)−φ(a)]α)=w0+pEα(−q[φ(t)−φ(a)]α)∫taw(s)g(t−s)ds+1Eα(−q[φ(t)−φ(a)]α)∫ta[φ(t)−φ(s)]α−1×Eα,α(−q[φ(t)−φ(s)]α)×(∫sak(s−σ)Eα(−q[φ(σ)−φ(a)]α)dσ)φ′(s)ds×supa≤σ≤tw(σ)Eα(−q[φ(σ)−φ(a)]α), |
or, for t>a,
w(t)Eα(−q[φ(t)−φ(a)]α)≤w0+pEα(−q[φ(t)−φ(a)]α)∫tag(t−s)Eα(−q[φ(s)−φ(a)]α)×(w(s)Eα(−q[φ(s)−φ(a)]α))ds+Msupa≤σ≤tw(σ)Eα(−q[φ(σ)−φ(a)]α). |
The relation
pEα(−q[φ(t)−φ(a)]α)∫tag(t−s)Eα(−q[φ(s)−φ(a)]α)ds≤M∗, |
is assumed for some M∗>0. Then,
w(t)Eα(−q[φ(t)−φ(a)]α)≤w0+(M∗+M)supa≤σ≤tw(σ)Eα(−q[φ(σ)−φ(a)]α),t>a, |
and
w(t)≤w01−M∗−MEα(−q[φ(t)−φ(a)]α),t>a, |
in the case that
M∗+M<1. |
Example. Take k as above, and select g fulfilling
g(t−s)≤C4[φ(t)−φ(s)]α−1Eα,α(−c[φ(t)−φ(s)]α)φ′(s), |
for some C4,c>q. Then,
∫taEα(−q[φ(s)−φ(a)]α)g(t−s)ds≤Γ(1+α)q∫ta[φ(s)−φ(a)]−αg(t−s)ds≤C4Γ(1+α)q∫taEα,α(−c[φ(t)−φ(s)]α)×[φ(t)−φ(s)]α−1[φ(s)−φ(a)]−αφ′(s)ds≤C4Γ(1+α)Γ(α)qEα,1(−q[φ(t)−φ(a)]α),t>a. |
A value for M∗ would be
M∗=C4pΓ(1+α)Γ(α)q. |
Therefore, we have proved the following theorem.
Theorem 5.1. Let u(t) be a nonnegative solution of (5.1), where q and p are positive and k and g are continuous functions with k(t), g(t)≥0 for all t such that
∫taEα,α(−q[φ(t)−φ(s)]α)[φ(t)−φ(s)]α−1×(∫saEα(−q[φ(σ)−φ(a)]α)k(s−σ)dσ)φ′(s)ds≤MEα(−q[φ(t)−φ(a)]α),t>a, |
p∫tag(t−s)Eα(−q[φ(s)−φ(a)]α)ds≤M∗Eα(−q[φ(t)−φ(a)]α),t>a, |
hold for some M, M∗>0 with
M∗+M<1. |
Then, we can find a positive constant C such that
w(t)≤CEα(−q[φ(t)−φ(a)]α),t>a. |
Before delving into applications, it is important to note that previous research on Halanay inequalities, including our earlier work, often assumes that solutions are non-negative. This supposition is sufficient for applications like neural networks without time delays. To determine the stability of the equilibrium solution, we can simplify the problem by shifting the equilibrium point to the origin using a variable transformation and then analyzing the magnitude of the solutions. However, when dealing with systems that have time delays, this approach becomes more complex. Directly proving stability for solutions that can be positive or negative presents new challenges, as time delays now appear within convolution integrals. The necessary estimations are more intricate and require careful analysis.
Now, we return to
{Dφ,αC[u(t)−pu(t−υ)]≤−qu(t)+∫tak(t−s)u(s)ds, p>0,0<α<1,t,υ>a,u(t)=ϖ(t)≥0,a−υ≤t≤a, |
with |ϖ(s)|≤w0Eα(−q(φ(s+υ)−φ(a))α) for s∈[a−υ,a], w0>0. To clarify these concepts, let us suppose that 1>p>0, and examine the following expression:
w(t)−pw(t−υ)=[ϖ(a)−pϖ(a−υ)]Eα(−q[φ(t)−φ(a)]α)+∫ta[φ(t)−φ(s)]α−1Eα,α(−q[φ(t)−φ(s)]α)×(−qpw(s−υ)+∫sak(s−σ)w(σ)dσ)φ′(s)ds. |
Then, for t>a
|w(t)|≤2w0Eα(−q[φ(t)−φ(a)]α)+p|w(t−υ)|+qp∫taEα,α(−q[φ(t)−φ(s)]α)[φ(t)−φ(s)]α−1|w(s−υ)|φ′(s)ds+∫taEα,α(−q[φ(t)−φ(s)]α)[φ(t)−φ(s)]α−1×(∫sak(s−σ)|w(σ)|dσ)φ′(s)ds. | (6.1) |
For t∈[a,a+υ],
|w(t)|Eα(−q[φ(t)−φ(a)]α)≤3w0+qpw0Eα(−q[φ(t)−φ(a)]α)∫ta[φ(t)−φ(s)]α−1×Eα,α(−q[φ(t)−φ(s)]α)Eα(−q[φ(s)−φ(a)]α)φ′(s)ds+Msupa≤σ≤tw(σ)Eα(−q[φ(σ)−φ(a)]α), |
where M is defined as in Eq (3.3). Again, as
∫taEα,α(−q[φ(t)−φ(s)]α)[φ(t)−φ(s)]α−1Eα(−q[φ(s)−φ(a)]α)φ′(s)ds≤Γ(1+α)q∫taEα,α(−q[φ(t)−φ(s)]α)[φ(t)−φ(s)]α−1[φ(s)−φ(a)]−αφ′(s)ds≤Γ(1+α)Γ(α)qEα,1(−q[φ(t)−φ(a)]α), | (6.2) |
we can write
|w(t)|Eα(−q[φ(t)−φ(a)]α)≤3w0+w0Γ(1+α)Γ(α)p+Msupa≤σ≤tw(σ)Eα(−q[φ(σ)−φ(a)]α), |
or
(1−M)|w(t)|Eα(−q[φ(t)−φ(a)]α)≤3w0+w0Γ(1+α)Γ(α)p. | (6.3) |
If t∈[a+υ,a+2υ], we first observe that
|w(t−υ)|≤3w0+w0Γ(1+α)Γ(α)p(1−M)×Eα(−q[φ(t−υ)−φ(a)]α)Eα(−q[φ(t)−φ(a)]α)Eα(−q[φ(t)−φ(a)]α)≤A3w0+w0Γ(1+α)Γ(α)p(1−M)Eα(−q(φ(t)−φ(a))α), |
where A is as in (3.11). Using the fact that
w0≤A3w0+w0Γ(1+α)Γ(α)p1−M, |
and relations (6.1) and (6.3), we get
|w(t)|≤2w0Eα(−q[φ(t)−φ(a)]α)+pA3w0+w0Γ(1+α)Γ(α)p(1−M)Eα(−q(φ(t)−φ(a))α)+qpA3w0+w0Γ(1+α)Γ(α)p(1−M)×∫taEα,α(−q[φ(t)−φ(s)]α)[φ(t)−φ(s)]α−1×Eα(−q(φ(s)−φ(a))α)φ′(s)ds+∫taEα,α(−q[φ(t)−φ(s)]α)[φ(t)−φ(s)]α−1×(∫sak(s−σ)|w(σ)|dσ)φ′(s)ds. |
Next, in view of (6.2), we find
|w(t)|≤2w0Eα(−q[φ(t)−φ(a)]α)+pA3w0+w0Γ(α)Γ(α+1)p(1−M)Eα(−q(φ(t)−φ(a))α)+qpA3w0+w0Γ(1+α)Γ(α)p(1−M)×Γ(1+α)Γ(α)qEα(−q[φ(t)−φ(a)]α)+∫ta[φ(t)−φ(s)]α−1Eα,α(−q[φ(t)−φ(s)]α)×(∫sak(s−σ)|w(σ)|dσ)φ′(s)ds. |
or
(1−M)|w(t)|Eα(−q[φ(t)−φ(a)]α)≤2w0+pAw0[1+Γ(1+α)Γ(α)](1−M)×(3+Γ(1+α)Γ(α)p)≤2w0+3Aw0[1+Γ(1+α)Γ(α)](1−M)p+Aw0[1+Γ(1+α)Γ(α)]2(1−M)p2. | (6.4) |
For t∈[a+2υ,a+3υ], by virtue of (3.14),
Eα(−q(φ(t−υ)−φ(a))α)Eα(−q(φ(t)−φ(a))α)≤1(φ(a+υ)−φ(a))α×(1q+Γ(1−α)(φ(a+3υ)−φ(a))α)=:V>1, |
and therefore
|w(t)|≤2w0Eα(−q[φ(t)−φ(a)]α)+pV(1−M)×[2w0+3Aw0[1+Γ(1+α)Γ(α)](1−M)p+Aw0[1+Γ(1+α)Γ(α)]2(1−M)p2]×Eα(−q(φ(t)−φ(a))+pVΓ(1+α)Γ(α)(1−M)×[2w0+3Aw0[1+Γ(1+α)Γ(α)](1−M)p+Aw0[1+Γ(1+α)Γ(α)]2(1−M)p2]×Eα(−q(φ(t)−φ(a))+∫ta[φ(t)−φ(s)]α−1Eα,α(−q[φ(t)−φ(s)]α)(∫sak(s−σ)|w(σ)|dσ)φ′(s)ds. |
So,
(1−M)|w(t)|Eα(−q[φ(t)−φ(a)]α)≤2w0+pV(1−M)[2w0+3Aw0[1+Γ(1+α)Γ(α)](1−M)p+Aw0[1+Γ(1+α)Γ(α)]2(1−M)p2]+pVΓ(1+α)Γ(α)(1−M)×[2w0+3Aw0[1+Γ(1+α)Γ(α)](1−M)p+Aw0[1+Γ(1+α)Γ(α)]2(1−M)p2], |
or
(1−M)|w(t)|Eα(−q[φ(t)−φ(a)]α)≤2w0+2w0pV[1+Γ(1+α)Γ(α)]1−M+3w0Ap2V[1+Γ(1+α)Γ(α)]2(1−M)2+Aw0V[1+Γ(1+α)Γ(α)]3(1−M)2p3. | (6.5) |
Writing (6.5) in the form
|w(t)|Eα(−q[φ(t)−φ(a)]α)(1−M)≤2w0+2w0pV[1+Γ(1+α)Γ(α)]1−M+3w0A(pV[1+Γ(1+α)Γ(α)](1−M))2+w0A(pV[1+Γ(1+α)Γ(α)]1−M)3≤3w0A[1+pV[1+Γ(1+α)Γ(α)]1−M+(pV[1+Γ(1+α)Γ(α)]1−M)2+(pV[1+Γ(1+α)Γ(α)]1−M)3] | (6.6) |
provides the basis for our next claim.
Claim. On the interval [a+(n−1)υ,a+nυ], it is clear that
|w(t)|Eα(−q[φ(t)−φ(a)]α)(1−Mw0)≤3A∑nk=0(Vp[1+Γ(1+α)Γ(α)]1−M)k. |
The validity of the claim for n=1,2, and 3 is established by Eqs (6.3), (6.4), and (6.6). Let t∈[a+nυ,a+(n+1)υ]. Then from (6.1),
|w(t)|≤2w0Eα(−q[φ(t)−φ(a)]α)+3ApVw01−M∑nk=0(Vp[Γ(α)Γ(1+α)+1]1−M)kEα(−q[φ(t)−φ(a)]α)+3ApΓ(1+α)Γ(α)w0V1−M∑nk=0(Vp[Γ(α)Γ(1+α)+1]1−M)k×Eα(−q[φ(t)−φ(a)]α)+∫taEα,α(−q[φ(t)−φ(s)]α)[φ(t)−φ(s)]α−1(∫sak(s−σ)|w(σ)|dσ)φ′(s)ds, |
or
(1−Mw0)|w(t)|Eα(−q[φ(t)−φ(a)]α)≤2+3VpA1−M∑nk=0(Vp[Γ(1+α)Γ(α)+1]1−M)k+3VpA1−MΓ(1+α)Γ(α)×∑nk=0(Vp[Γ(1+α)Γ(α)+1]1−M)k. |
Then,
(1−Mw0)|w(t)|Eα(−q[φ(t)−φ(a)]α)≤3A{1+[Γ(1+α)Γ(α)+1]pV1−M∑nk=0(Vp[Γ(1+α)Γ(α)+1]1−M)k}, |
i.e.,
(1−Mw0)|w(t)|Eα(−q[φ(t)−φ(a)]α)≤3A{1+∑nk=0(Vp[Γ(1+α)Γ(α)+1]1−M)1+k}. |
Thus,
(1−Mw0)|w(t)|Eα(−q[φ(t)−φ(a)]α)≤3A∑n+1k=0(Vp[Γ(1+α)Γ(α)+1]1−M)k, |
demonstrating that the assertion holds. Moreover, the series converges if the following condition is satisfied:
1+Γ(1+α)Γ(α)1−MVp<1. |
We have just proved the following result.
Theorem 6.1. Suppose that u(t) is a solution of
{Dφ,αC[u(t)−pu(t−υ)]≤−qu(t)+∫t0k(t−s)u(s)ds,t,υ>a,p>0,0<α<1,u(t)=ϖ(t),a−υ≤t≤a, |
with |ϖ(t)|≤Eα(−q(φ(t+υ)−φ(a))α), a−υ≤t≤a, q>0, p>0, and k is a nonnegative function verifying
∫ta[φ(t)−φ(s)]α−1Eα,α(−q[φ(t)−φ(s)]α)×(∫saEα(−q[φ(σ)−φ(a)]α)k(s−σ)dσ)φ′(s)ds≤MEα(−q[φ(t)−φ(a)]α),t>a, |
for some M such that
M<1−[Γ(1+α)Γ(α)+1]Vp, |
with
[Γ(1+α)Γ(α)+1]Vp<1. |
Then,
|w(t)|≤CEα(−q[φ(t)−φ(a)]α),t>a, |
where C>0 is a positive constant.
Neural networks are a fundamental part of artificial intelligence and are widely used to address complex problems in various fields. In this work, we utilize our findings to analyze the behavior of Cohen-Grossberg neural networks. Specifically, we consider the following problems:
{Dφ,αC[xi(t)−pxi(t−υ)]=−hi(xi(t))[gi(xi(t))−n∑j=1aijfj(xj(t))−n∑j=1bijlj(xj(t−τ))−n∑j=1dij∫∞akj(s)Φj(xj(t−s))ds−Ii], t,υ>a, p>0xi(t)=xi0(t),t∈[a−υ,a], i=1,2,...,n, |
and
{Dφ,αC[xi(t)−p∫taxi(s)ψi(t−s)ds]=−hi(xi(t))[gi(xi(t))−n∑j=1bijlj(xj(t−τ))−n∑j=1aijfj(xj(t))−n∑j=1dij∫∞aΦj(xj(t−s))kj(s)ds−Ii], t>a, p>0,xi(0)=xi0(t), t≤a, i=1,2,...,n, |
where xi.(t) stands the state of the ith neuron, n is the number of neurons, gi is a suitable function, hi represents an amplification function, bij, aij, dij represent the weights or strengths of the connections from the jth neuron to the ith neuron, Ii is the external input to the ith neuron, ψi are the neutral delay kernels, fj,lj,Φj denote the signal transmission functions, υ is the neutral delay, τ corresponds to the transmission delay, ϕi is the history of the i th state, and kj denotes the delay kernel function. These systems represent a general class of Cohen-Grossberg neural networks with both continuously distributed and discrete delays. To streamline our analysis and highlight our key findings, we have opted to examine simpler systems with fixed time delays. More complex scenarios involving variable delays or multiple delays can be explored in future research. To simplify our analysis, let us examine the simpler case
{Dφ,αC[xi(t)−pxi(t−υ)]=−hi(xi(t))[gi(xi(t))−n∑j=1dij∫∞akj(s)fj(xj(t−s))ds−Ii],xi(t)=xi0(t),t∈[a−υ,a], i=1,2,...,n, | (7.1) |
for t,υ>a, p>0.
We adopt the following standard assumptions.
(A1) The functions fi are assumed to satisfy the Lipschitz condition
|fi(x)−fi(y)|≤Li|x−y| for every x,y∈R and for each i=1,2,...,n, |
where Li denotes the Lipschitz constant corresponding to the function fi.
(A2) The delay kernel functions kj are nonnegative and exhibit piecewise continuity. Additionally, each kj has a finite integral over its domain, expressed as κj=∫∞akj(s)ds<∞, for j=1,...,n.
(A3) The functions gi have derivatives that are uniformly bounded by a constant G. Specifically,
|g′i(z)|≤G, for all z∈R and for each i=1,2,...,n, |
where G>0 is a fixed constant.
(A4) The functions hi are strictly positive and continuous, and they satisfy the following bounds:
0<β_i≤hi(z)≤¯βi, for all z∈R and i=1,2,...,n. |
For simplicity, we suppose that the initial values xi0(t) are all zero for times before a.
Definition 7.1. The point x∗=(x∗1,x∗2,...,x∗n)T is said to be an equilibrium if, for each i=1,2,...,n, it satisfies the equation
gi(x∗i)=n∑j=1aijfj(x∗j)+n∑j=1dij∫∞akj(s)fj(x∗j)ds+Ii=n∑j=1(aij+dijκj)fj(x∗j)+Ii, t>a. |
Previous studies have shown that an equilibrium exists and is unique. To facilitate our analysis, we translate the equilibrium point to the origin of the coordinate system by using the substitution x(t)−x∗=y(t). This leads to the following:
{Dφ,αC[yi(t)−pyi(t−υ)]=−hi(x∗i+yi(t))[gi(yi(t)+x∗i) −n∑j=1dij∫tafj(x∗j+yj(t−s))kj(s)ds−Ii], t>a, i=1,...,n,yi(t)=ψi(t):=ϕi(t)−x∗i, t∈[a−υ,a], i=1,...,n, |
or
\begin{equation*} \left\{ \begin{array}{l} D_{C}^{\varphi , \alpha }\left[ y_{i}(t)-py_{i}(t-\upsilon )\right] = -H_{i}\left( y_{i}\left( t\right) \right) \left[ G_{i}\left( y_{i}\left( t\right) \right) \right. \\ \left. -\sum\limits_{j = 1}^{n}d_{ij}\int\nolimits_{0}^{t}F_{j}\left( y_{j}\left( t-s\right) \right) k_{j}\left( s\right) ds\right] , { \ }t > a, \text{ }i = 1, ..., n, \\ y_{i}\left( t\right) = \psi _{i}\left( t\right) : = \phi _{i}\left( t\right) -x_{i}^{\ast }, \text{ }t\in \lbrack a-\upsilon , a], \text{ }i = 1, ..., n, \end{array} \right. \end{equation*} |
where
\begin{equation*} \begin{array}{c} F_{i}\left( y_{i}\left( t\right) \right) = f_{i}\left( y_{i}\left( t\right) +x_{i}^{\ast }\right) -f_{i}\left( x_{i}^{\ast }\right) , \text{ }G_{i}\left( y_{i}\left( t\right) \right) = g_{i}\left( y_{i}\left( t\right) +x_{i}^{\ast }\right) -g_{i}\left( x^{\ast }\right) \\ H_{i}\left( y_{i}\left( t\right) \right) = h_{i}\left( y_{i}\left( t\right) +x_{i}^{\ast }\right) , { \ }t > a, \text{ }i = 1, ..., n. \end{array} \end{equation*} |
Using the mean value theorem, the following inequality can be established:
\begin{equation*} \begin{array}{l} D_{C}^{\varphi , \alpha }\left\vert y_{i}(t)-py_{i}(t-\upsilon )\right\vert \leq sgn\left[ y_{i}(t)-py_{i}(t-\upsilon )\right] D_{C}^{\varphi , \alpha } \left[ y_{i}(t)-py_{i}(t-\upsilon )\right] \\ = -sgn\left[ y_{i}(t)-py_{i}(t-\upsilon )\right] H_{i}\left( y_{i}\left( t\right) \right) \left[ g_{i}^{\prime }\left( \bar{x}_{i}\left( t\right) \right) y_{i}\left( t\right) -\sum\limits_{j = 1}^{n}d_{ij}\int\nolimits_{a}^{\infty }F_{j}\left( y_{j}\left( t-s\right) \right) k_{j}\left( s\right) ds\right] . \end{array} \end{equation*} |
By subtracting and adding the term pg_{i}^{\prime }\left(\bar{x}_{i}\left(t\right) \right) y_{i}(t-\upsilon), we obtain
\begin{equation*} \begin{array}{c} D_{C}^{\varphi , \alpha }\left\vert y_{i}(t)-py_{i}(t-\upsilon )\right\vert \leq -sgn\left[ y_{i}(t)-py_{i}(t-\upsilon )\right] H_{i}\left( y_{i}\left( t\right) \right) \left[ g_{i}^{\prime }\left( \bar{x}_{i}\left( t\right) \right) \left[ y_{i}(t)-py_{i}(t-\upsilon )\right] \right. \\ \left. +pg_{i}^{\prime }\left( \bar{x}_{i}\left( t\right) \right) y_{i}(t-\upsilon )-\sum\limits_{j = 1}^{n}d_{ij}\int\nolimits_{a}^{\infty }F_{j}\left( y_{j}\left( t-s\right) \right) k_{j}\left( s\right) ds\right] , { \ }t > a, \text{ }i = 1, ..., n, \end{array} \end{equation*} |
or
\begin{equation*} \begin{array}{c} D_{C}^{\varphi , \alpha }\left\vert y_{i}(t)-py_{i}(t-\upsilon )\right\vert \leq -H_{i}\left( y_{i}\left( t\right) \right) G\left\vert y_{i}(t)-py_{i}(t-\upsilon )\right\vert +pGH_{i}\left( y_{i}\left( t\right) \right) \left\vert y_{i}(t-\upsilon )\right\vert \\ +H_{i}\left( y_{i}\left( t\right) \right) \sum\limits_{j = 1}^{n}d_{ij}\int\nolimits_{a}^{\infty }k_{j}\left( s\right) L_{j}\left\vert y_{j}\left( t-s\right) \right\vert ds, { \ }t > a, \text{ } i = 1, 2, ..., n. \end{array} \end{equation*} |
Therefore,
\begin{equation*} \begin{array}{c} D_{C}^{\varphi , \alpha }\left\vert y_{i}(t)-py_{i}(t-\upsilon )\right\vert \leq -G\underline{\beta }_{i}\left\vert y_{i}(t)-py_{i}(t-\upsilon )\right\vert +pG\overline{\beta }_{i}\left\vert y_{i}(t-\upsilon )\right\vert \\ +\overline{\beta }_{i}\sum\limits_{j = 1}^{n}L_{j}d_{ij}\int\nolimits_{a}^{ \infty }k_{j}\left( s\right) \left\vert y_{j}\left( t-s\right) \right\vert ds, { \ }t > a, \text{ }i = 1, ..., n. \end{array} \end{equation*} |
Finally, we consider the equation for w_{i} and rewrite it in the following form:
\begin{equation*} \begin{array}{c} \left\vert w_{i}(t)-pw_{i}(t-\upsilon )\right\vert = E_{\alpha }(-G\underline{ \beta }_{i}\left[ \varphi \left( t\right) -\varphi \left( a\right) \right] ^{\alpha })\left\vert \Phi _{i}(a)-p\Phi _{i}(a-\upsilon )\right\vert \\ +\int_{a}^{t}\left[ \varphi \left( t\right) -\varphi \left( s\right) \right] ^{\alpha -1}E_{\alpha , \alpha }(-q\left[ \varphi \left( t\right) -\varphi \left( s\right) \right] ^{\alpha }) \\ \times \left( pG\overline{\beta }_{i}\left\vert w_{i}(t-\upsilon )\right\vert +\overline{\beta }_{i}\sum\limits_{j = 1}^{n}L_{j}d_{ij}\int \nolimits_{0}^{\infty }k_{j}\left( s\right) \left\vert w_{j}\left( t-s\right) \right\vert ds\right) \, \varphi ^{\prime }\left( s\right) ds, { \ }t > a, \text{ }i = 1, 2, ..., n. \end{array} \end{equation*} |
The Mittag-Leffler stability of this problem follows directly from our earlier result.
We have investigated a general Halanay inequality of fractional order with distributed delays, incorporating delays of neutral type. General sufficient conditions were established to guarantee the Mittag-Leffler stability of the solutions, supported by illustrative examples. The rate of stability obtained appears to be the best achievable, consistent with previous findings in fractional-order problems.
Furthermore, we applied our theoretical results to a practical problem, demonstrating their applicability. Our analysis suggests that these results can be extended to more general cases, such as variable delays or systems involving additional terms. It is worth noting that the conditions on the various parameters within the system could potentially be improved, as we did not focus on optimizing the estimations and bounds. In this regard, exploring optimal bounds for the delay coefficient p and the kernel k would be an interesting direction for future research.
The author declares that have not used Artificial Intelligence (AI) tools in the creation of this article.
The author sincerely appreciates the financial support and facilities provided by Imam Abdulrahman Bin Faisal University.
The author declares that there is no conflict of interest regarding the publication of this paper.
[1] | A. Carpinteri, F. Mainardi, Fractals and fractional calculus in continuum mechanics, Vienna: Springer, https://doi.org/10.1007/978-3-7091-2664-6 |
[2] |
L. Debnath, Recent applications of fractional calculus to science and engineering, Int. J. Math. Math. Sci., 2003 (2003), 753601. https://doi.org/10.1155/S0161171203301486 doi: 10.1155/S0161171203301486
![]() |
[3] |
J. T. Machado, V. Kiryakova, F. Mainardi, Recent history of fractional calculus, Commun. Nonlinear Sci. Numer. Simul., 16 (2011), 1140–1153. https://doi.org/10.1016/j.cnsns.2010.05.027 doi: 10.1016/j.cnsns.2010.05.027
![]() |
[4] |
A. A. M. Arafa, S. Z. Rida, H. Mohamed, Approximate analytical solutions of Schnakenberg systems by homotopy analysis method, Appl. Math. Model., 36 (2012), 4789–4796. https://doi.org/10.1016/j.apm.2011.12.014 doi: 10.1016/j.apm.2011.12.014
![]() |
[5] |
P. Sunthrayuth, A. M. Zidan, S. W. Yao, R. Shah, M. Inc, The comparative study for solving fractional-order Fornberg Whitham equation via \rho-Laplace transform, Symmetry, 13 (2021), 784. https://doi.org/10.3390/sym13050784 doi: 10.3390/sym13050784
![]() |
[6] |
R. Shah, H. Khan, D. Baleanu, Fractional Whitham Broer Kaup equations within modified analytical approaches, Axioms, 8 (2019), 125. https://doi.org/10.3390/axioms8040125 doi: 10.3390/axioms8040125
![]() |
[7] |
H. M. Srivastava, R. Shah, H. Khan, M. Arif, Some analytical and numerical investigation of a family of fractional-order Helmholtz equations in two space dimensions, Math. Methods Appl. Sci., 43 (2020), 199–212. https://doi.org/10.1002/mma.5846 doi: 10.1002/mma.5846
![]() |
[8] |
H. Yasmin, N. H. Aljahdaly, A. M. Saeed, Investigating symmetric soliton solutions for the fractional coupled konno onno system using improved versions of a novel analytical technique, Mathematics, 11 (2023), 2686. https://doi.org/10.3390/math11122686 doi: 10.3390/math11122686
![]() |
[9] |
M. M. Al-Sawalha, R. Shah, A. Khan, O. Y. Ababneh, T. Botmart, Fractional view analysis of Kersten-Krasil'shchik coupled KdV-mKdV systems with non-singular kernel derivatives, AIMS Mathematics, 7 (2022), 18334-18359. https://doi.org/10.3934/math.20221010 doi: 10.3934/math.20221010
![]() |
[10] |
A. A. Alderremy, R. Shah, N. Iqbal, S. Aly, K. Nonlaopon, Fractional series solution construction for nonlinear fractional reaction-diffusion Brusselator model utilizing Laplace residual power series, Symmetry, 14 (2022), 1944. https://doi.org/10.3390/sym14091944 doi: 10.3390/sym14091944
![]() |
[11] |
S. Alshammari, M. M. Al-Sawalha, R. Shah, Approximate analytical methods for a fractional-order nonlinear system of Jaulent Miodek equation with energy-dependent Schrodinger potential, Fractal Fract., 7 (2023), 140. https://doi.org/10.3390/fractalfract7020140 doi: 10.3390/fractalfract7020140
![]() |
[12] |
E. M. Elsayed, R. Shah, K. Nonlaopon, The analysis of the fractional-order Navier-Stokes equations by a novel approach, J. Funct. Spaces, 2022 (2022), 8979447. https://doi.org/10.1155/2022/8979447 doi: 10.1155/2022/8979447
![]() |
[13] |
M. Alqhtani, K. M. Saad, W. Weera, W. M. Hamanah, Analysis of the fractional-order local Poisson equation in fractal porous media, Symmetry, 14 (2022), 1323. https://doi.org/10.3390/sym14071323 doi: 10.3390/sym14071323
![]() |
[14] |
H. Yasmin, A. S. Alshehry, A. H. Ganie, A. M. Mahnashi, Perturbed Gerdjikov Ivanov equation: Soliton solutions via Backlund transformation, Optik, 298 (2024), 171576. http://dx.doi.org/10.1016/j.ijleo.2023.171576 doi: 10.1016/j.ijleo.2023.171576
![]() |
[15] |
N. A. Pirim, F. Ayaz, A new technique for solving fractional order systems: Hermite collocation method, Appl. Math., 7 (2016), 2307–2323. http://dx.doi.org/10.4236/am.2016.718182 doi: 10.4236/am.2016.718182
![]() |
[16] |
V. Marinca, N. Herisanu, Application of optimal homotopy asymptotic method for solving nonlinear equations arising in heat transfer, Int. Commun. Heat Mass Transfer, 35 (2008), 710–715. https://doi.org/10.1016/j.icheatmasstransfer.2008.02.010 doi: 10.1016/j.icheatmasstransfer.2008.02.010
![]() |
[17] | J. S. Duan, R. Rach, D. Baleanu, A. M. Wazwaz, A review of the Adomian decomposition method and its applications to fractional differential equations, Commun. Frac. Calc., 3 (2012), 73–99. |
[18] |
M. Khan, M. A. Gondal, I. Hussain, S. K. Vanani, A new comparative study between homotopy analysis transform method and homotopy perturbation transform method on a semi infinite domain, Math. Comput. Model., 55 (2012), 1143–1150. https://doi.org/10.1016/j.mcm.2011.09.038 doi: 10.1016/j.mcm.2011.09.038
![]() |
[19] |
A. Jabbari, H. Kheiri, A. Yildirim, Homotopy analysis and homotopy Pade methods for (1+1) and (2+1) dimensional dispersive long wave equations, Internat. J. Numer. Methods Heat Fluid Flow, 23 (2013), 692–706. http://dx.doi.org/10.1108/09615531311323818 doi: 10.1108/09615531311323818
![]() |
[20] |
R. K. Gazizov, A. A. Kasatkin, Construction of exact solutions for fractional order differential equations by the invariant subspace method, Comput. Math. Appl., 66 (2013), 576–584. https://doi.org/10.1016/j.camwa.2013.05.006 doi: 10.1016/j.camwa.2013.05.006
![]() |
[21] |
A. Prakash, P. Veeresha, D. G. Prakasha, M. Goyal, A new efficient technique for solving fractional coupled Navier-Stokes equations using q-homotopy analysis transform method, Pramana-J. Phys., 93 (2018), 6. https://doi.org/10.1007/s12043-019-1763-x doi: 10.1007/s12043-019-1763-x
![]() |
[22] |
R. K. Pandey, H. K. Mishra, Homotopy analysis Sumudu transform method for time-fractional third order dispersive partial differential equation, Adv. Comput. Math., 43 (2017), 365–383. https://doi.org/10.1007/s10444-016-9489-5 doi: 10.1007/s10444-016-9489-5
![]() |
[23] |
Z. H. Guo, O. Acan, S. Kumar, Sumudu transform series expansion method for solving the local fractional Laplace equation in fractal thermal problems, Thermal Sci., 20 (2016), 739–742. http://dx.doi.org/10.2298/TSCI16S3739G doi: 10.2298/TSCI16S3739G
![]() |
[24] |
K. K. Ali, M. Maneea, M. S. Mohamed, Solving nonlinear fractional models in superconductivity using the q-Homotopy analysis transform method, J. Math., 2023 (2023), 6647375. https://doi.org/10.1155/2023/6647375 doi: 10.1155/2023/6647375
![]() |
[25] |
Z. Y. Fan, K. K. Ali, M. Maneea, M. Inc, S. W. Yao, Solution of time fractional Fitzhugh-Nagumo equation using semi analytical techniques, Results Phys., 51 (2023), 106679. https://doi.org/10.1016/j.rinp.2023.106679 doi: 10.1016/j.rinp.2023.106679
![]() |
[26] |
K. K. Ali, F. E. A. Elbary, M. Maneea, Efficient techniques for nonlinear dynamics: A study of fractional generalized quintic Ginzburg-Landau equation, J. Taibah Univ. Sci., 18 (2024), 2333593. https://doi.org/10.1080/16583655.2024.2333593 doi: 10.1080/16583655.2024.2333593
![]() |
[27] | M. A. El-Tawil, S. N. Huseen, The q-homotopy analysis method (q-HAM), Int. J. Appl. Math. Mech., 8 (2012), 51–75. |
[28] | M. A. El-Tawil, S. N. Huseen, On convergence of the q-homotopy analysis method, Int. J. Contemp. Math. Sci., 8 (2013), 481–497. |
[29] |
Z. J. Liu, M. Y. Adamu, E. Suleiman, J. H. He, Hybridization of homotopy perturbation method and Laplace transformation for the partial differential equations, Thermal Sci., 21 (2017), 1843–1846. http://dx.doi.org/10.2298/TSCI160715078L doi: 10.2298/TSCI160715078L
![]() |
[30] | A. Prakash, H. Kaur, q-homotopy analysis transform method for space and time-fractional KdV-Burgers equation, Nonlinear Sci. Lett. A, 9 (2018), 44–61. |
[31] |
E. F. Keller, L. A. Segel, Initiation of slime mold aggregation viewed as an instability, J. Theoret. Biol., 26 (1970), 399–415. https://doi.org/10.1016/0022-5193(70)90092-5 doi: 10.1016/0022-5193(70)90092-5
![]() |
[32] |
A. Atangana, Extension of the Sumudu homotopy perturbation method to an attractor for one-dimensional Keller-Segel equations, Appl. Math. Model., 39 (2015), 2909–2916. https://doi.org/10.1016/j.apm.2014.09.029 doi: 10.1016/j.apm.2014.09.029
![]() |
[33] |
A. Atangana, B. S. T. Alkahtani, Analysis of the Keller-Segel model with a fractional derivative without singular kernel, Entropy, 17 (2015), 4439–4453. https://doi.org/10.3390/e17064439 doi: 10.3390/e17064439
![]() |
[34] |
A. Atangana, E. Alabaraoye, Solving a system of fractional partial differential equations arising in the model of HIV infection of CD4+ cells and attractor one-dimensional Keller-Segel equations, Adv. Differ. Equ., 2013 (2013), 94. https://doi.org/10.1186/1687-1847-2013-94 doi: 10.1186/1687-1847-2013-94
![]() |
[35] |
M. Zayernouri, A. Matzavinos, Fractional Adams-Bashforth/Moulton methods: An application to the fractional Keller-Segel chemotaxis system, J. Comput. Phys., 317 (2016), 1–14. https://doi.org/10.1016/j.jcp.2016.04.041 doi: 10.1016/j.jcp.2016.04.041
![]() |
[36] |
S. Kumar, A. Kumar, I. K. Argyros, A new analysis for the Keller-Segel model of fractional order, Numer. Algorithms, 75 (2017), 213–228. https://doi.org/10.1007/s11075-016-0202-z doi: 10.1007/s11075-016-0202-z
![]() |
[37] |
M. A. Dokuyucu, D. Baleanu, E. Çelik, Analysis of Keller-Segel model with Atangana-Baleanu fractional derivative, Filomat, 32 (2018), 5633–5643. http://dx.doi.org/10.2298/FIL1816633D doi: 10.2298/FIL1816633D
![]() |
[38] |
X. Luo, M. Nadeem, M. Inc, S. Dawood, Fractional complex transform and homotopy perturbation method for the approximate solution of Keller-Segel model, J. Funct. Spaces, 2022 (2022), 9637098. https://doi.org/10.1155/2022/9637098 doi: 10.1155/2022/9637098
![]() |
[39] |
O. A. 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. A. 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. A. Arqub, A. El-Ajou, Z. A. Zhour, S. Momani, Multiple solutions of nonlinear boundary value problems of fractional order: A new analytic iterative technique, Entropy, 16 (2014), 471–493. https://doi.org/10.3390/e16010471 doi: 10.3390/e16010471
![]() |
[42] |
A. El-Ajou, O. A. Arqub, S. Momani, Approximate analytical solution of the nonlinear fractional KdV-Burgers equation: A new iterative algorithm, J. Comput. Phys., 293 (2015), 81–95. https://doi.org/10.1016/j.jcp.2014.08.004 doi: 10.1016/j.jcp.2014.08.004
![]() |
[43] |
S. Rida, A. Arafa, A. Abedl-Rady, H. Abdl-Rahaim, Fractional physical differential equations via natural transform, Chinese J. Phys., 55 (2017), 1569–1575. https://doi.org/10.1016/j.cjph.2017.05.004 doi: 10.1016/j.cjph.2017.05.004
![]() |
[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. https://doi.org/10.1155/2019/6159024 doi: 10.1155/2019/6159024
![]() |
[45] |
Y. Xie, I. Ahmad, T. I. S. Ikpe, E. F. Sofia, H. Seno, What influence could the acceptance of visitors cause on the epidemic dynamics of a Reinfectious disease?: A mathematical model, Acta Biotheor., 72 (2024), 3. https://doi.org/10.1007/s10441-024-09478-w doi: 10.1007/s10441-024-09478-w
![]() |
[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. https://doi.org/10.1140/epjp/i2018-12007-1 doi: 10.1140/epjp/i2018-12007-1
![]() |
[47] | M. Alquran, K. Al-Khaled, S. Sivasundaram, H. M. Jaradat, Mathematical and numerical study of existence of bifurcations of the generalized fractional Burgers-Huxley equation, Nonlinear Stud., 24 (2017), 235–244. |
[48] |
I. Ahmad, H. Seno, An epidemic dynamics model with limited isolation capacity, Theory Biosci., 142 (2023), 259–273. https://doi.org/10.1007/s12064-023-00399-9 doi: 10.1007/s12064-023-00399-9
![]() |
[49] |
G. O. Ojo, N. I. Mahmudov, Aboodh transform iterative method for spatial diffusion of a biological population with fractional-order, Mathematics, 9 (2021), 155. https://doi.org/10.3390/math9020155 doi: 10.3390/math9020155
![]() |
[50] |
M. A. Awuya, G. O. Ojo, N. I. Mahmudov, Solution of space-time fractional differential equations using Aboodh transform iterative method, J. Math., 2022 (2022), 4861588. https://doi.org/10.1155/2022/4861588 doi: 10.1155/2022/4861588
![]() |
[51] |
M. A. Awuya, D. Subasi, Aboodh transform iterative method for solving fractional partial differential equation with Mittag-Leffler Kernel, Symmetry, 13 (2021), 2055. https://doi.org/10.3390/sym13112055 doi: 10.3390/sym13112055
![]() |
[52] |
M. I. Liaqat, S. Etemad, S. Rezapour, C. Park, A novel analytical Aboodh residual power series method for solving linear and nonlinear time-fractional partial differential equations with variable coefficients, AIMS Mathematics, 7 (2022), 16917–16948. http://dx.doi.org/10.3934/math.2022929 doi: 10.3934/math.2022929
![]() |
[53] |
M. I. Liaqat, A. Akgul, H. Abu-Zinadah, Analytical investigation of some time-fractional Black-Scholes models by the Aboodh residual power series method, Mathematics, 11 (2023), 276. https://doi.org/10.3390/math11020276 doi: 10.3390/math11020276
![]() |
[54] | K. S. Aboodh, The new integral transform'Aboodh transform, Glob. J. Pure Appl. Math., 9 (2013), 35–43. |
[55] | S. Aggarwal, R. Chauhan, A comparative study of Mohand and Aboodh transforms, Int. J. Res. Adv. Technol., 7 (2019), 520–529. |
[56] |
M. E. Benattia, K. Belghaba, Application of the Aboodh transform for solving fractional delay differential equations, Univ. J. Math. Appl., 3 (2020), 93–101. https://doi.org/10.32323/ujma.702033 doi: 10.32323/ujma.702033
![]() |
[57] |
B. B. Delgado, J. E. 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. https://doi.org/10.3390/fractalfract5030117 doi: 10.3390/fractalfract5030117
![]() |
[58] |
S. Alshammari, M. Al-Smadi, I. Hashim, M. A. Alias, Residual power series technique for simulating fractional Bagley-Torvik problems emerging in applied physics, Appl. Sci., 9 (2019), 5029. https://doi.org/10.3390/app9235029 doi: 10.3390/app9235029
![]() |
1. | Q. Rubbab, Y. Mahsud, S. Irshad, M. A. Imran, A. Ahmadian, S. Salahshour, M. Ferrara, Numerical simulations of unsteady flows in a rotating channel using a novel eigenfunction expansion method, 2020, 10, 2158-3226, 065035, 10.1063/5.0012874 | |
2. | Maria Alessandra Ragusa, Fan Wu, Regularity Criteria for the 3D Magneto-Hydrodynamics Equations in Anisotropic Lorentz Spaces, 2021, 13, 2073-8994, 625, 10.3390/sym13040625 | |
3. | Sadek Gala, Eugeny Galakhov, Maria Alessandra Ragusa, Olga Salieva, Beale–Kato–Majda Regularity Criterion of Smooth Solutions for the Hall-MHD Equations with Zero Viscosity, 2021, 1678-7544, 10.1007/s00574-021-00256-7 | |
4. | Sharad K. Yadav, Hideaki Miura, Rahul Pandit, Statistical properties of three-dimensional Hall magnetohydrodynamics turbulence, 2022, 34, 1070-6631, 095135, 10.1063/5.0107434 | |
5. | Sadek Gala, Michel Théra, Logarithmically improved regularity criterion for the 3D Hall-MHD equations, 2021, 40, 2238-3603, 10.1007/s40314-021-01585-5 | |
6. | Baoying Du, On three-dimensional Hall-magnetohydrodynamic equations with partial dissipation, 2022, 2022, 1687-2770, 10.1186/s13661-022-01587-0 |