Nonlocal Initial Value Problems for Hybrid Caputo Fractional Integro-Differential Equations Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 3 (2025) 985 https://internationalpubls.com Nonlocal Initial Value Problems for Hybrid Caputo Fractional Integro- Differential Equations Dr. Moffek Hamza Ecole Normale SupΓ©rieure de Ouargla,30000 Ouargla,Algeria , Email: moffek.hamza@ens-ouargla.dz Article History: Received: 19-09-2024 Revised: 24-03-2025 Accepted: 11-04-2025 Abstract: This paper investigates nonlocal initial value problems for hybrid Caputo fractional integro-differential equations. By employing a fixed-point theorem due to Dhage, we establish the existence of solutions to these problems. The theoretical findings are illustrated through a concrete example, showcasing the applicability of our results. Keywords: The fractional Caputo derivative, The fractional integral, hybrid, Dhage fixed point. Introduction Fractional calculus, an extension of classical calculus, has garnered significant attention in recent years due to its ability to describe complex phenomena that integer-order derivatives and integrals fail to capture accurately. This branch of mathematics has proven its utility in various domains, including physics, engineering, biology, and economics. ([10],[13],[14],[16],[4],[12]). Nonlocal initial value problems (NIVPs) represent a category of problems in which the initial conditions depend on the values of the unknown function at multiple points rather than a single point. Such problems naturally arise in numerous real-world applications, such as heat transfer, viscoelastic material behavior, and control systems. Hybrid differential equations, which combine differential and integral operators, have emerged as a powerful tool for modeling complex systems. In recent years, there has been growing interest in studying hybrid fractional differential equations, which incorporate fractional derivatives and integrals into the hybrid structure. ([10],[13],[14],[16],[4],[12]). Lakshmikanthan and Dhage [7] They initiated the study of hybrid equations by introducing a novel class of nonlinear differential equations known as ordinary hybrid differential equations. { 𝑑 𝑑𝑑 ( π‘₯(𝑑) 𝑓(𝑑,π‘₯(𝑑)) ) = 𝑔(𝑑, π‘₯(𝑑)), π‘Ž. 𝑒. 𝑑 ∈ 𝐼0, π‘₯(𝑑0) = π‘₯0 ∈ ℝ They formulated essential hybrid differential inequalities that serve as key tools for proving the existence of extremal solutions. Zhao et al. [18] extended Dhage’s work to the fractional-order case by examining boundary value problems involving fractional hybrid differential equations. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 3 (2025) 986 https://internationalpubls.com { 𝐷0+ 𝛼 ( π‘₯(𝑑) 𝑓(𝑑,π‘₯(𝑑)) ) = 𝑔(𝑑, π‘₯(𝑑)), 𝑑 ∈ [0, 𝑇], π‘₯(𝑑0) = 0, where 𝐷0+ 𝛼 is the Riemann-Liouville fractional derivative of order 0 < 𝛼 < 1. Hybrid fractional differential equations and inclusions have been the focus of considerable research in recent years. Prior to proceeding, we present a brief overview of some relevant contributions in this field. Ahmad et al. [2] examined the existence of solutions for a hybrid inclusion problem involving nonlocal boundary conditions. { 𝐢𝐷0+ 𝛼 ( π‘₯(𝑑)βˆ’βˆ‘ 𝐼 0+ π›½π‘–π‘š 𝑖=1 β„Žπ‘–(𝑑,π‘₯(𝑑)) 𝑔(𝑑,π‘₯(𝑑)) ) ∈ 𝒒(𝑑, π‘₯(𝑑)), π‘Ž. 𝑒. 𝑑 ∈ [0,1], π‘₯(0) = πœ‡(πœ‰),  π‘₯(1) = π‘Ž ∈ ℝ. where 𝐢𝐷0+ 𝛼 denotes the Caputo fractional derivative of order 1 < 𝛼 ≀ 2 and 𝐼 0+ 𝛽𝑖 is the Riemann– Liouville fractional integral of order 𝛽𝑖 > 0 with 𝑖 ∈ {1,2,3. . . , π‘š}. In [6], Derbazi et al. confirmed the existence and uniqueness of solutions for a fractional hybrid boundary value problem. { 𝐢𝐷0+ 𝛼 ( π‘₯(𝑑)βˆ’β„Ž(𝑑,π‘₯(𝑑)) 𝑔(𝑑,π‘₯(𝑑)) ) = Θ(𝑑, π‘₯(𝑑)), π‘Ž. 𝑒. 𝑑 ∈ [0, 𝑇], π‘Ž1 ( π‘₯(𝑑)βˆ’β„Ž(𝑑,π‘₯(𝑑)) 𝑔(𝑑,π‘₯(𝑑)) ) |𝑑=0 + 𝑏1 ( π‘₯(𝑑)βˆ’β„Ž(𝑑,π‘₯(𝑑)) 𝑔(𝑑,π‘₯(𝑑)) ) |𝑑=𝑇 = πœ†1, π‘Ž2 𝐢𝐷 0+ 𝛽 ( π‘₯(𝑑)βˆ’β„Ž(𝑑,π‘₯(𝑑)) 𝑔(𝑑,π‘₯(𝑑)) ) |𝑑=πœ‚ + 𝑏2 𝐢𝐷 0+ 𝛽 ( π‘₯(𝑑)βˆ’β„Ž(𝑑,π‘₯(𝑑)) 𝑔(𝑑,π‘₯(𝑑)) ) |𝑑=𝑇 = πœ†2. where 1 < 𝛼 ≀ 2 , 0 < 𝛽 ≀ 1, πœ‚ ∈ [0, 𝑇] and π‘Ž1, π‘Ž2, 𝑏1, 𝑏2, πœ†1, πœ†2 are real constants. . Baleanu et al. [3] they employed a generalized version of Dhage’s hybrid fixed point theorem for the sum of three fractional operators to examine the existence of solutions to a fractional hybrid integro-differential equation subject to mixed hybrid integral boundary conditions. { 𝐢𝐷0+ πœ” ( π‘₯(𝑑)βˆ’β„Ž(𝑑,π‘₯(𝑑),𝐼 0+ 𝛾1π‘₯(𝑑),𝐼 0+ 𝛾2π‘₯(𝑑),...,𝐼 0+ 𝛾𝑛π‘₯(𝑑)) 𝑔(𝑑,π‘₯(𝑑),𝐼 0+ πœ‡1π‘₯(𝑑),𝐼 0+ πœ‡2π‘₯(𝑑),...,𝐼 0+ πœ‡π‘šπ‘₯(𝑑)) ) = Ξ₯(𝑑, π‘₯(𝑑)), π‘Ž. 𝑒. 𝑑 ∈ [0,1], πœ†1 ∫ 𝐢 1 0 𝐷 0+ 𝛽1 ( π‘₯(𝑠)βˆ’β„Ž(𝑠,π‘₯(𝑠),𝐼𝛾1π‘₯(𝑠),𝐼𝛾2π‘₯(𝑠),...,𝐼𝛾𝑛π‘₯(𝑠)) 𝑔(𝑠,π‘₯(𝑠),πΌπœ‡1π‘₯(𝑠),πΌπœ‡2π‘₯(𝑠),...,πΌπœ‡π‘šπ‘₯(𝑠)) )𝑑𝑠 +πœ†2 𝐢𝐷 0+ 𝛼1 ( π‘₯(𝑑)βˆ’β„Ž(𝑑,π‘₯(𝑑),𝐼 0+ 𝛾1π‘₯(𝑑),𝐼 0+ 𝛾2π‘₯(𝑑),...,𝐼 0+ 𝛾𝑛π‘₯(𝑑)) 𝑔(𝑑,π‘₯(𝑑),𝐼 0+ πœ‡1π‘₯(𝑑),𝐼 0+ πœ‡2π‘₯(𝑑),...,𝐼 0+ πœ‡π‘šπ‘₯(𝑑)) ) |𝑑=1 +πœ†3 ( π‘₯(𝑑)βˆ’β„Ž(𝑑,π‘₯(𝑑),𝐼 0+ 𝛾1π‘₯(𝑑),𝐼 0+ 𝛾2π‘₯(𝑑),...,𝐼 0+ 𝛾𝑛π‘₯(𝑑)) 𝑔(𝑑,π‘₯(𝑑),𝐼 0+ πœ‡1π‘₯(𝑑),𝐼 0+ πœ‡2π‘₯(𝑑),...,𝐼 0+ πœ‡π‘šπ‘₯(𝑑)) ) |𝑑=0 = 0 πœ†4 ∫ 𝐢 1 0 𝐷 0+ 𝛽2 ( π‘₯(𝑠)βˆ’β„Ž(𝑠,π‘₯(𝑠),𝐼𝛾1π‘₯(𝑠),𝐼𝛾2π‘₯(𝑠),...,𝐼𝛾𝑛π‘₯(𝑠)) 𝑔(𝑠,π‘₯(𝑠),πΌπœ‡1π‘₯(𝑠),πΌπœ‡2π‘₯(𝑠),...,πΌπœ‡π‘šπ‘₯(𝑠)) )𝑑𝑠 +πœ†5 𝐢𝐷 0+ 𝛼2 ( π‘₯(𝑑)βˆ’β„Ž(𝑑,π‘₯(𝑑),𝐼 0+ 𝛾1π‘₯(𝑑),𝐼 0+ 𝛾2π‘₯(𝑑),...,𝐼 0+ 𝛾𝑛π‘₯(𝑑)) 𝑔(𝑑,π‘₯(𝑑),𝐼 0+ πœ‡1π‘₯(𝑑),𝐼 0+ πœ‡2π‘₯(𝑑),...,𝐼 0+ πœ‡π‘šπ‘₯(𝑑)) ) |𝑑=1 +πœ†6 ( π‘₯(𝑑)βˆ’β„Ž(𝑑,π‘₯(𝑑),𝐼 0+ 𝛾1π‘₯(𝑑),𝐼 0+ 𝛾2π‘₯(𝑑),...,𝐼 0+ 𝛾𝑛π‘₯(𝑑)) 𝑔(𝑑,π‘₯(𝑑),𝐼 0+ πœ‡1π‘₯(𝑑),𝐼 0+ πœ‡2π‘₯(𝑑),...,𝐼 0+ πœ‡π‘šπ‘₯(𝑑)) ) |𝑑=0 = 0. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 3 (2025) 987 https://internationalpubls.com where 1 < πœ” ≀ 2, 𝛽1, 𝛽2 ∈ (0,1], 𝛼1, 𝛼2 ∈ (0,1], πœ†1, πœ†2, πœ†3, πœ†4, πœ†5, πœ†6 ∈ ℝ + and 𝛾𝑖 > 0, πœ‡π‘— > 0 with 𝑖 ∈ {1,2, . . . 𝑛} and 𝑗 ∈ {1,2, . . . π‘š}. Building upon the previous works, we establish an existence result for a class of fractional hybrid integro-differential problem. 𝐢𝐷0+ 𝛼 ( 𝑒(𝑑) 𝑓(𝑑,𝑒(𝑑)) ) + 𝑔(𝑑, 𝐼 0+ πœ‡1𝑒(𝑑), 𝐼 0+ πœ‡2𝑒(𝑑), … , 𝐼 0+ πœ‡π‘›π‘’(𝑑)) + ∫ 𝐾 𝑑 0 (𝑑, 𝑠, 𝑒(𝑠)𝑑𝑠 = 0, 𝑑 ∈ 𝐼 (1) 𝑒(0) = β„Ž(𝑒), π‘Žπ· ( 𝑒(𝑑) 𝑓(𝑑,𝑒(𝑑)) ) |𝑑=0 + 𝑏 𝐢𝐷0+ 𝛼 ( 𝑒(𝑑) 𝑓(𝑑,𝑒(𝑑)) ) |𝑑=1 = 0. (2) where 𝛼 ∈ (1,2], π‘Ž, 𝑏 ∈ ℝ, 𝐼 := [0,1]. Also, 𝐢𝐷0+ 𝛼 denotes the fractional Caputo derivative of order 𝛼, 𝐼 0+ πœ‡π‘– denotes the fractional Riemann–Liouville integral of order πœ‡π‘– > 0 for all 𝑖 ∈ {1,2, . . . , 𝑛}, and the maps 𝑓: 𝐼 Γ— ℝ β†’ β„βˆ—, 𝑔: 𝐼 Γ— ℝ𝑛+1 β†’ ℝ and 𝐾: 𝐼 Γ— 𝐼 Γ— ℝ β†’ ℝ are continuous. This paper proceeds as follows: Some fundamental preliminaries are revisited in Section 2. In Section 3, we present the equivalent fractional integral equation corresponding to the linear part of the hybrid fractional differential equation ([1],[2]), and we prove the main existence result of this paper.One example is given in Section 4 to support the established findings. Preliminaries In this section, we present definitions and properties of fractional integration and differentiation, as well as the fixed point theorem employed in this work. For further details, the reader may refer to references [ [10], [13], [14] , [8]]. Definition 1. Let 𝑔 be a real function defined on [0,1] and 𝛼 > 0. Then the left and right Riemann- Liouville fractional integrals of order 𝛼 of 𝑔 are defined respectively by 𝐼0+ 𝛼 𝑔(𝑑) = 1 Ξ“(𝛼) ∫ 𝑔(𝑠) (π‘‘βˆ’π‘ )1βˆ’π›Ό 𝑑 0 𝑑𝑠 𝐼1βˆ’ 𝛼 𝑔(𝑑) = 1 Ξ“(𝛼) ∫ 𝑔(𝑠) (π‘ βˆ’π‘‘)1βˆ’π›Ό 1 𝑑 𝑑𝑠 Definition 2. The left and the right Caputo fractional derivative of order 𝛼 > 0, of a function 𝑔 are, respectively 𝐢𝐷0+ 𝛼 𝑔(𝑑) = (𝐼0+ π‘›βˆ’π›Ό 𝑑𝑛 𝑑𝑑𝑛 𝑔(𝑑)) 𝐢𝐷1βˆ’ 𝛼 𝑔(𝑑) = (βˆ’1)𝑛(𝐼1βˆ’ π‘›βˆ’π›Ό 𝑑𝑛 𝑑𝑑𝑛 𝑔(𝑑)) where 𝑛 βˆ’ 1 < 𝛼 < 𝑛. Proposition 3. Let 𝑛 βˆ’ 1 < 𝛼 < 𝑛 and 𝑓 ∈ 𝐿1[0 ,1]. Then (1) 𝐼0+ 𝛼 𝐢𝐷0+ 𝛼 𝑓(𝑑) = 𝑓(𝑑) βˆ’ βˆ‘ 𝑓(π‘˜)(0) π‘˜! π‘›βˆ’1 π‘˜=0 π‘‘π‘˜ (2) 𝐼1βˆ’ 𝛼 𝐢𝐷1βˆ’ 𝛼 𝑓(𝑑) = 𝑓(𝑑) βˆ’ βˆ‘ (βˆ’1)π‘˜π‘“(π‘˜)(1) π‘˜! π‘›βˆ’1 π‘˜=0 (1 βˆ’ 𝑑)π‘˜ Theorem 4. (Dhage fixed point theorem)[8]) Let 𝑀 be a closed, bounded, convex and nonempty subset of a Banach algebra (𝐸, βˆ₯ . βˆ₯) , and let 𝐴: 𝐸 β†’ 𝐸 and 𝐡:𝑀 β†’ 𝐸 be two operators such that (i) 𝐴 is Lipschitzian with Lipschitz constant πœ†, (ii) 𝐡 is completely continuous,, (iii) π‘₯ = 𝐴π‘₯𝐡𝑧 β‡’ π‘₯ ∈ 𝑀 π‘“π‘œπ‘Ÿ π‘Žπ‘™π‘™ 𝑧 ∈ 𝑀, (iv) πœ†πΏ < 1, where 𝐿 =βˆ₯ 𝐡(𝑀) βˆ₯= 𝑠𝑒𝑝{βˆ₯ 𝐡(π‘₯) βˆ₯: π‘₯ ∈ 𝑀}. Then the operator equation 𝐴𝑦𝐡𝑦 = 𝑦 has a solution in 𝑀. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 3 (2025) 988 https://internationalpubls.com Main results Lemma 5. Let 𝑦 ∈ 𝐴𝐢([0,1], ℝ) Then 𝑒 is a solution of the hybrid fractional integrodifferential problem { 𝐢𝐷0+ 𝛼 ( 𝑒(𝑑) 𝑓(𝑑,𝑒(𝑑)) ) + 𝑦(𝑑) = 0, 𝑑 ∈ 𝐼 ≔ [0,1], 𝑒(0) = β„Ž(𝑒), π‘Žπ· ( 𝑒(𝑑) 𝑓(𝑑,𝑒(𝑑)) ) |𝑑=0 + 𝑏 𝐢𝐷0+ 𝛼 ( 𝑒(𝑑) 𝑓(𝑑,𝑒(𝑑)) ) |𝑑=1 = 0. (3) if and only if 𝑒 is a solution for the integral equation 𝑒(𝑑) = 𝑓(𝑑, 𝑒(𝑑)) [βˆ’βˆ« (π‘‘βˆ’πœ)π›Όβˆ’1 Ξ“(𝛼) 𝑑 0 𝑦(𝜏)π‘‘πœ + Ξ“(3βˆ’π›Ό)𝑏𝑑 π‘ŽΞ“(3βˆ’π›Ό)+𝑏 ∫ 𝑦 1 0 (𝜏)π‘‘πœ + β„Ž(𝑒) 𝑓(0,β„Ž(𝑒)) ] (4) Proof. we apply the right-hand side fractional integral 𝐼0+ 𝛼 to equation ([3]).We get 𝑒(𝑑) 𝑓(𝑑,𝑒(𝑑)) = βˆ’βˆ« (π‘‘βˆ’πœ)π›Όβˆ’1 Ξ“(𝛼) 𝑑 0 𝑦(𝜏)π‘‘πœ + 𝑐1 + 𝑐2𝑑. (5) Using the conditions nonlocal 𝑒(0) = β„Ž(𝑒), so 𝑐1 = β„Ž(𝑒) 𝑓(0,β„Ž(𝑒)) .and we have 𝐢𝐷0+ π›Όβˆ’1 ( 𝑒(𝑑) 𝑓(𝑑,𝑒(𝑑)) ) = βˆ’βˆ« 𝑦 𝑑 0 (𝜏)π‘‘πœ + 𝑐2 𝑑2βˆ’π›Ό Ξ“(3βˆ’π›Ό) , and 𝐷 𝑒(𝑑) 𝑓(𝑑,𝑒(𝑑)) = βˆ’βˆ« (π‘‘βˆ’πœ)π›Όβˆ’2 Ξ“(π›Όβˆ’1) 𝑑 0 𝑦(𝜏)π‘‘πœ + 𝑐2, so π‘Žπ· ( 𝑒(𝑑) 𝑓(𝑑,𝑒(𝑑)) ) |𝑑=0 + 𝑏 𝐢𝐷0+ 𝛼 ( 𝑒(𝑑) 𝑓(𝑑,𝑒(𝑑)) ) |𝑑=1 = π‘Žπ‘2 + 𝑏 (βˆ’βˆ« 𝑦 1 0 (𝜏)π‘‘πœ + 𝑐2 Ξ“(3βˆ’π›Ό) ) then we get 𝑐2 = Ξ“(3βˆ’π›Ό)𝑏 π‘ŽΞ“(3βˆ’π›Ό)+𝑏 ∫ 𝑦 1 0 (𝜏)π‘‘πœ Substituting the values of 𝑐1, 𝑐2 in ([5]), we get solution ([4]). The converse follows by direct computation. This completes the proof. In the sequel, we need the following assumptions. (H1) The function 𝑓: 𝐼 Γ— ℝ β†’ β„βˆ’ {0} is a continuous function satisfying the Lipschitz condition for a constant πœ†π‘“ ∣ 𝑓(𝑑, 𝑒) βˆ’ 𝑓(𝑑, 𝑣) βˆ£β‰€ πœ†π‘“ ∣ 𝑒 βˆ’ 𝑣 ∣. (H2) The function β„Ž:ℝ β†’ ℝ is a continuous function and there exists a constant 𝑀0 > 0 such that : | β„Ž(𝑒) 𝑓(0,β„Ž(𝑒)) | ≀ 𝑀0. (H3) The function 𝑔: 𝐼 Γ— ℝ𝑛+1 β†’ ℝ is a continuous function and there exists a bounded mapping πœƒ: 𝐼 Γ—β†’ ℝ+ such that for all 𝑒𝑖 , 𝑣𝑖 ∈ 𝐸, Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 3 (2025) 989 https://internationalpubls.com ∣ 𝑔(𝑑, 𝑒1(𝑑), 𝑒2(𝑑), . . . , 𝑒𝑛+1(𝑑)) βˆ’ 𝑔(𝑑, 𝑣1(𝑑), 𝑣2(𝑑), . . . , 𝑣𝑛+1(𝑑)) βˆ£β‰€ πœƒ(𝑑)βˆ‘ βˆ£π‘›+1 𝑖=1 𝑒𝑖(𝑑) βˆ’ 𝑣𝑖(𝑑) ∣, (H4) The function 𝐾: 𝐼 Γ— 𝐼 Γ— ℝ β†’ ℝ+ is a continuous function and there exists a constant 𝑀1 > 0such that : π‘€π‘Žπ‘₯{𝐾(𝑑, 𝑠, 𝑒(𝑠)): 𝑑, 𝑠 ∈ 𝐼; ∣ 𝑒(𝑠) βˆ£β‰€ 𝑅} ≀ 𝑀1 where 𝑅 = 𝑀𝑓Ξ₯ 1βˆ’πœ†π‘“Ξ₯ and Ξ₯ = [ 1 Ξ“(𝛼 + 1) + 𝑏Γ(3 βˆ’ 𝛼) π‘ŽΞ“(3 βˆ’ 𝛼) + 𝑏 ] [πœƒβˆ—πœ‰π‘… + πΊβˆ— +𝑀1] + 𝑀0 where πœƒβˆ— = π‘ π‘’π‘π‘‘βˆˆπΌπœƒ(𝑑), 𝐺 βˆ— = π‘ π‘’π‘π‘‘βˆˆπΌ ∣ 𝑔(𝑑, 0,0, . . . ,0) ∣, 𝑀𝑓 = π‘ π‘’π‘π‘‘βˆˆπΌπ‘“(𝑑, 0), π‘Žπ‘›π‘‘ πœ‰ = 1 + βˆ‘ 1 Ξ“(1+πœ‡π‘–) 𝑛 𝑖=1 Theorem 6. Assume that conditions (H1)–(H4) hold.and if πœ†π‘“Ξ₯ < 1.then the problem ([1]-[2]) has at least one solution in 𝐸 = 𝐢([0,1]) Proof. We consider a subset Ξ© of 𝐸 given by Ξ© = {𝑒 ∈ 𝐸: βˆ₯ 𝑒 βˆ₯𝐸≀ 𝑅} and we define the operators 𝐴:𝐸 β†’ 𝐸 and 𝐡:Ξ© β†’ 𝐸 as follows: 𝐴𝑒(𝑑) = 𝑓(𝑑, 𝑒(𝑑)).  𝑑 ∈ 𝐼, 𝐡𝑒(𝑑) = βˆ’βˆ« (π‘‘βˆ’πœ)π›Όβˆ’1 Ξ“(𝛼) 𝑑 0 [𝑔(𝜏, 𝐼 0+ πœ‡1𝑒(𝜏), 𝐼 0+ πœ‡2𝑒(𝜏), . . . , 𝐼 0+ πœ‡π‘›π‘’(𝜏)) + ∫ 𝐾 𝜏 0 (𝜏, 𝑠, 𝑒(𝑠)𝑑𝑠]π‘‘πœ + 𝑏Γ(3βˆ’π›Ό)𝑑 π‘ŽΞ“(3βˆ’π›Ό)+𝑏 ∫ [𝑔(𝜏, 𝐼0+ πœ‡1𝑒(𝜏), 𝐼 0+ πœ‡2𝑒(𝜏), . . . , 𝐼 0+ πœ‡π‘›π‘’(𝜏)) + ∫ 𝐾 𝜏 0 (𝜏, 𝑠, 𝑒(𝑠)𝑑𝑠] 1 0 π‘‘πœ + β„Ž(𝑒) 𝑓(0,β„Ž(𝑒)) . Obviously, problem ([1]-[2]) has a solution if and only if 𝐴π‘₯𝐡π‘₯ has a fixed point. Now, we show that the operators 𝐴 and 𝐡 satisfy all the conditions of theorem 4 in a series of steps. claim 1 𝐴 is a Lipschitz on 𝐸 Let 𝑒, 𝑣 ∈ 𝐸 for all 𝑑 ∈ 𝐼. Then in view of condition (H1), we get ∣ 𝐴𝑒(𝑑) βˆ’ 𝐴𝑣(𝑑) ∣=∣ 𝑓(𝑑, 𝑒(𝑑)) βˆ’ 𝑓(𝑑, 𝑣(𝑑)) βˆ£β‰€ πœ†π‘“ ∣ 𝑒 βˆ’ 𝑣 ∣ Then, for each 𝑑 ∈ 𝐼 we obtain βˆ₯ 𝐴𝑒 βˆ’ 𝐴𝑣 βˆ₯𝐸≀ πœ†π‘“ βˆ₯ 𝑒 βˆ’ 𝑣 βˆ₯𝐸 claim 2 𝐡 is completely continuous on Ξ©. We firstly show that𝐡 is uniformly bounded for any 𝑒 ∈ Ξ©, by (H2)-(H5), we have. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 3 (2025) 990 https://internationalpubls.com ∣ 𝐡𝑒(𝑑) βˆ£β‰€ ∫ βˆ£π‘‘βˆ’πœβˆ£π›Όβˆ’1 Ξ“(𝛼) 𝑑 0 [∣ 𝑔(𝜏, 𝑒(𝜏), 𝐼 0+ πœ‡1𝑒(𝜏), 𝐼 0+ πœ‡2𝑒(𝜏), . . . , 𝐼 0+ πœ‡π‘›π‘’(𝜏)) ∣ +∫ ∣ 𝜏 0 𝐾(𝜏, 𝑠, 𝑒(𝑠)𝑑𝑠 ∣]π‘‘πœ + 𝑏Γ(3βˆ’π›Ό)𝑑 π‘ŽΞ“(3βˆ’π›Ό)+𝑏 ∫ [∣ 𝑔(𝜏, 𝑒(𝜏), 𝐼0+ πœ‡1𝑒(𝜏), 𝐼 0+ πœ‡2𝑒(𝜏), . . . , 𝐼 0+ πœ‡π‘›π‘’(𝜏)) ∣ +∫ ∣ 𝜏 0 𝐾(𝜏, 𝑠, 𝑒(𝑠) ∣ 𝑑𝑠] 1 0 π‘‘πœ +| β„Ž(𝑒) 𝑓(0,β„Ž(𝑒)) |, ≀ ∫ βˆ£π‘‘βˆ’πœβˆ£π›Όβˆ’1 Ξ“(𝛼) 𝑑 0 [∣ 𝑔(𝜏, 𝑒(𝜏), 𝐼 0+ πœ‡1𝑒(𝜏), 𝐼 0+ πœ‡2𝑒(𝜏), . . . , 𝐼 0+ πœ‡π‘›π‘’(𝜏)) βˆ’ 𝑔(𝑑, 0, . . . ,0) ∣ +∣ 𝑔(𝑑, 0, . . . ,0) ∣ + ∫ ∣ 𝜏 0 𝐾(𝜏, 𝑠, 𝑒(𝑠) ∣ 𝑑𝑠]π‘‘πœ + 𝑏Γ(3βˆ’π›Ό)𝑑 π‘ŽΞ“(3βˆ’π›Ό)+𝑏 ∫ [ 1 0 ∣ 𝑔(𝜏, 𝑒(𝜏), 𝐼 0+ πœ‡1𝑒(𝜏), 𝐼 0+ πœ‡2𝑒(𝜏), . . . , 𝐼 0+ πœ‡π‘›π‘’(𝜏)) βˆ’ 𝑔(𝑑, 0, . . . ,0) ∣ +∣ 𝑔(𝑑, 0, . . . ,0) ∣ + ∫ ∣ 𝜏 0 𝐾(𝜏, 𝑠, 𝑒(𝑠) ∣ 𝑑𝑠]π‘‘πœ +| β„Ž(𝑒) 𝑓(0,β„Ž(𝑒)) |, ≀ 1 Ξ“(𝛼+1) [πœƒβˆ— (1 + 1 Ξ“(πœ‡1+1) + 1 Ξ“(πœ‡2+1) +. . . + 1 Ξ“(πœ‡π‘›+1) ) ∣ 𝑒 ∣ +πΊβˆ— +𝑀1] + 𝑏Γ(3βˆ’π›Ό) π‘ŽΞ“(3βˆ’π›Ό)+𝑏 [πœƒβˆ— (1 + 1 Ξ“(πœ‡1+1) + 1 Ξ“(πœ‡2+1) +. . . + 1 Ξ“(πœ‡π‘›+1) ) ∣ 𝑒 ∣ +πΊβˆ— +𝑀1] + 𝑀0 ≀ [ 1 Ξ“(𝛼+1) + 𝑏Γ(3βˆ’π›Ό) π‘ŽΞ“(3βˆ’π›Ό)+𝑏 ] [πœƒβˆ—πœ‰π‘… + πΊβˆ— +𝑀1] + 𝑀0 ≀ Ξ₯ Thus, we get βˆ₯ 𝐡𝑒 βˆ₯𝐸≀ Ξ₯for all 𝑒 ∈ Ξ©, this proves that 𝐡 is uniformly bounded in Ξ©. Next we show that 𝐡 is continuous on Ξ©. Let {𝑒𝑛}π‘›βˆˆβ„• be a sequence in Ξ© converging to a point 𝑒 ∈ Ξ©.Then by (H2)-(H4), for all 𝑑 ∈ 𝐼, one has ∣ 𝐡𝑒𝑛(𝑑) βˆ’ 𝐡𝑒(𝑑) βˆ£β‰€ ∫ βˆ£π‘‘βˆ’πœβˆ£π›Όβˆ’1 Ξ“(𝛼) 𝑑 0 [∣ 𝑔(𝜏, 𝑒𝑛, 𝐼0+ πœ‡1𝑒𝑛(𝜏), 𝐼0+ πœ‡2𝑒𝑛(𝜏), . . . , 𝐼0+ πœ‡π‘›π‘’π‘›(𝜏)) βˆ’π‘”(𝜏, 𝑒(𝜏), 𝐼 0+ πœ‡1𝑒(𝜏), 𝐼 0+ πœ‡2𝑒(𝜏), … , 𝐼 0+ πœ‡π‘›π‘’(𝜏)) ∣ +∫ ∣ 𝜏 0 𝐾(𝜏, 𝑠, 𝑒𝑛(𝑠) βˆ’ 𝐾(𝜏, 𝑠, 𝑒(𝑠) ∣ 𝑑𝑠]π‘‘πœ + 𝑏Γ(3βˆ’π›Ό)𝑑 π‘ŽΞ“(3βˆ’π›Ό)+𝑏 ∫ [ 1 0 ∣ 𝑔(𝜏, 𝑒𝑛, 𝐼0+ πœ‡1𝑒𝑛(𝜏), 𝐼0+ πœ‡2𝑒𝑛(𝜏), . . . , 𝐼0+ πœ‡π‘›π‘’π‘›(𝜏)) βˆ’π‘”(𝜏, 𝑒(𝜏), 𝐼 0+ πœ‡1𝑒(𝜏), 𝐼 0+ πœ‡2𝑒(𝜏), … , 𝐼 0+ πœ‡π‘›π‘’(𝜏)) ∣ +∫ ∣ 𝜏 0 𝐾(𝜏, 𝑠, 𝑒𝑛 (𝑠) βˆ’ 𝐾(𝜏, 𝑠, 𝑒(𝑠) ∣ 𝑑𝑠]π‘‘πœ +| β„Ž(𝑒𝑛) 𝑓(0,β„Ž(𝑒𝑛)) βˆ’ β„Ž(𝑒𝑛) 𝑓(0,β„Ž(𝑒𝑛)) |, ≀ 1 Ξ“(𝛼+1) [πœƒβˆ— (1 + 1 Ξ“(πœ‡1+1) + 1 Ξ“(πœ‡2+1) +. . . + 1 Ξ“(πœ‡π‘›+1) ) ∣ 𝑒𝑛 βˆ’ 𝑒 ∣ +π‘˜0 ∣ 𝑒𝑛 βˆ’ 𝑒 ∣] + 𝑏Γ(3βˆ’π›Ό) π‘ŽΞ“(3βˆ’π›Ό)+𝑏 [πœƒβˆ— (1 + 1 Ξ“(πœ‡1+1) + 1 Ξ“(πœ‡2+1) +. . . + 1 Ξ“(πœ‡π‘›+1) ) ∣ 𝑒𝑛 βˆ’ 𝑒 ∣ +π‘˜0 ∣ 𝑒𝑛 βˆ’ 𝑒 ∣] +| β„Ž(𝑒𝑛) 𝑓(0,β„Ž(𝑒𝑛)) βˆ’ β„Ž(𝑒𝑛) 𝑓(0,β„Ž(𝑒𝑛)) |, ≀ [ 1 Ξ“(𝛼+1) + 𝑏Γ(3βˆ’π›Ό) π‘ŽΞ“(3βˆ’π›Ό)+𝑏 ] [πœƒβˆ—πœ‰ + π‘˜0] βˆ₯ 𝑒𝑛 βˆ’ 𝑒 βˆ₯𝐸 +| β„Ž(𝑒𝑛) 𝑓(0,β„Ž(𝑒𝑛)) βˆ’ β„Ž(𝑒𝑛) 𝑓(0,β„Ž(𝑒𝑛)) |, Since that functions β„Ž and 𝑓 are continuous, we deduce Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 3 (2025) 991 https://internationalpubls.com βˆ₯ 𝐡𝑒𝑛 βˆ’ 𝐡𝑒 βˆ₯𝐸→ 0 π‘Žπ‘  𝑛 β†’ ∞. Then 𝐡 is continuous. Next we prove that the operator𝐡 equicontinuous. Let 𝑒 ∈ Ξ© and 𝑑1, 𝑑2 ∈ 𝐼 with 𝑑1 < 𝑑2 Then we have ∣ 𝐡𝑒(𝑑2) βˆ’ 𝐡𝑒(𝑑1) βˆ£β‰€ | ∫ (𝑑2βˆ’πœ) π›Όβˆ’1 Ξ“(𝛼) 𝑑2 0 [𝑔(𝜏, 𝑒(𝜏), 𝐼 0+ πœ‡1𝑒(𝜏), 𝐼 0+ πœ‡2𝑒(𝜏), . . . , 𝐼 0+ πœ‡π‘›π‘’(𝜏)) + ∫ 𝐾 𝜏 0 (𝜏, 𝑠, 𝑒(𝑠)𝑑𝑠]π‘‘πœ + 𝑏Γ(3βˆ’π›Ό)𝑑2 π‘ŽΞ“(3βˆ’π›Ό)+𝑏 ∫ [𝑔(𝜏, 𝑒(𝜏), 𝐼0+ πœ‡1𝑒(𝜏), 𝐼 0+ πœ‡2𝑒(𝜏), . . . , 𝐼 0+ πœ‡π‘›π‘’(𝜏)) + ∫ 𝐾 𝜏 0 (𝜏, 𝑠, 𝑒(𝑠)𝑑𝑠] 1 0 π‘‘πœ βˆ’βˆ« (𝑑1βˆ’πœ) π›Όβˆ’1 Ξ“(𝛼) 𝑑1 0 [𝑔(𝜏, 𝑒(𝜏), 𝐼 0+ πœ‡1𝑒(𝜏), 𝐼 0+ πœ‡2𝑒(𝜏), . . . , 𝐼 0+ πœ‡π‘›π‘’(𝜏)) + ∫ ∣ 𝜏 0 𝐾(𝜏, 𝑠, 𝑒(𝑠)𝑑𝑠]π‘‘πœ + 𝑏Γ(3βˆ’π›Ό)𝑑1 π‘ŽΞ“(3βˆ’π›Ό)+𝑏 ∫ [𝑔(𝜏, 𝑒(𝜏), 𝐼0+ πœ‡1𝑒(𝜏), 𝐼 0+ πœ‡2𝑒(𝜏), . . . , 𝐼 0+ πœ‡π‘›π‘’(𝜏)) + ∫ 𝐾 𝜏 0 (𝜏, 𝑠, 𝑒(𝑠)𝑑𝑠] 1 0 π‘‘πœ| ≀ ∫ | 𝑑1 0 (𝑑2βˆ’πœ) π›Όβˆ’1βˆ’(𝑑1βˆ’πœ) π›Όβˆ’1 Ξ“(𝛼) |[ |𝑔(𝜏, 𝑒(𝜏), 𝐼 0+ πœ‡1𝑒(𝜏), 𝐼 0+ πœ‡2𝑒(𝜏), . . . , 𝐼 0+ πœ‡π‘›π‘’(𝜏)) + ∫ 𝐾 𝜏 0 (𝜏, 𝑠, 𝑒(𝑠)𝑑𝑠|]π‘‘πœ +∫ | 𝑑2 𝑑1 (𝑑2βˆ’πœ) π›Όβˆ’1 Ξ“(𝛼) |[ |𝑔(𝜏, 𝑒(𝜏), 𝐼 0+ πœ‡1𝑒(𝜏), 𝐼 0+ πœ‡2𝑒(𝜏), . . . , 𝐼 0+ πœ‡π‘›π‘’(𝜏)) + ∫ 𝐾 𝜏 0 (𝜏, 𝑠, 𝑒(𝑠)𝑑𝑠|]π‘‘πœ + 𝑏Γ(3βˆ’π›Ό)βˆ£π‘‘2βˆ’π‘‘1∣ π‘ŽΞ“(3βˆ’π›Ό)+𝑏 ∫ [ | 1 0 𝑔(𝜏, 𝑒(𝜏), 𝐼 0+ πœ‡1𝑒(𝜏), 𝐼 0+ πœ‡2𝑒(𝜏), . . . , 𝐼 0+ πœ‡π‘›π‘’(𝜏))| + ∫ | 𝜏 0 𝐾(𝜏, 𝑠, 𝑒(𝑠)𝑑𝑠|]π‘‘πœ ≀ [ πœƒβˆ—πœ‰π‘…+πΊβˆ—+𝑀1 Ξ“(𝛼+1) ] [2 ∣ 𝑑2 βˆ’ 𝑑1 ∣ 𝛼+ 𝑑2 𝛼 βˆ’ 𝑑1 𝛼] + 𝑏Γ(3βˆ’π›Ό)βˆ£π‘‘2βˆ’π‘‘1∣ π‘ŽΞ“(3βˆ’π›Ό)+𝑏 [πœƒβˆ—πœ‰π‘… + πΊβˆ— +𝑀1] which is independent of 𝑒 ∈ Ξ©. As 𝑑1 β†’ 𝑑2, the right-hand side of the above inequality tends to zero. Therefore, it follows from the ArzelΒ΄a-Ascoli theorem that 𝐡 is a completely continuous operator on Ξ©. claim 3 Now we show that the (iii) hypothesis of theorem 4 is satisfied. Let 𝑒 ∈ 𝐸 and 𝑣 ∈ Ξ© such that 𝑒 = 𝐴𝑒𝐡𝑣 Then, for 𝑑 ∈ 𝐼 we have ∣ 𝑒(𝑑) βˆ£β‰€βˆ£ 𝐴𝑒(𝑑) ∣∣ 𝐡𝑣(𝑑) ∣ β‰€βˆ£ 𝑓(𝑑, 𝑒(𝑑)) ∣ [ | βˆ’ ∫ (π‘‘βˆ’πœ)π›Όβˆ’1 Ξ“(𝛼) 𝑑 0 [𝑔(𝜏, 𝐼 0+ πœ‡1𝑒(𝜏), 𝐼 0+ πœ‡2𝑒(𝜏), . . . , 𝐼 0+ πœ‡π‘›π‘’(𝜏)) + ∫ 𝐾 𝜏 0 (𝜏, 𝑠, 𝑒(𝑠)𝑑𝑠]π‘‘πœ + 𝑏Γ(3βˆ’π›Ό)𝑑 π‘ŽΞ“(3βˆ’π›Ό)+𝑏 ∫ [𝑔(𝜏, 𝐼0+ πœ‡1𝑒(𝜏), 𝐼 0+ πœ‡2𝑒(𝜏), . . . , 𝐼 0+ πœ‡π‘›π‘’(𝜏)) + ∫ 𝐾 𝜏 0 (𝜏, 𝑠, 𝑒(𝑠)𝑑𝑠] 1 0 π‘‘πœ + β„Ž(𝑒) 𝑓(0,β„Ž(𝑒)) |] ≀ [∣ 𝑓(𝑑, 𝑒(𝑑)) βˆ’ 𝑓(𝑑, 0) ∣ +∣ 𝑓(𝑑, 0) ∣] ([ 1 Ξ“(𝛼+1) + 𝑏Γ(3βˆ’π›Ό) π‘ŽΞ“(3βˆ’π›Ό)+𝑏 ] [πœƒβˆ—πœ‰π‘… + πΊβˆ— +𝑀1] + 𝑀0) ≀ [πœ†π‘“ ∣ 𝑒 ∣ +𝑀𝑓]Ξ₯. Thus, we obtain βˆ₯ 𝑒(𝑑) βˆ₯𝐸≀ 𝑀𝑓Ξ₯ 1 βˆ’ πœ†π‘“Ξ₯ = 𝑅 Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 3 (2025) 992 https://internationalpubls.com Then 𝑒 ∈ Ξ©, thus the (iii) hypothesis of theorem 4 is satisfied. claim 4 Now, we show that πœ†π‘“πΏ < 1, where 𝐿 =βˆ₯ 𝐡(Ξ©) βˆ₯𝐸= sup{βˆ₯ 𝐡𝑒 βˆ₯𝐸: 𝑒 ∈ Ξ©} Since 𝐿 = supπ‘’βˆˆΞ©{supπ‘‘βˆˆπΌ ∣ 𝐡𝑒(𝑑) ∣} ≀ Ξ₯, then πœ†π‘“Ξ₯ < 1, Thus all the conditions of theorem 4 are satisfied and hence the operator equation 𝑒 = 𝐴𝑒𝐡𝑒 has a solution in Ξ©. In consequence, problem ([1]-[2]) has a solution on 𝐼. This completes the proof An Example This section includes an example that showcases how Theorem 6 can be applied. Let us consider the following boundary value problem: 𝐢𝐷0+ 1.7 [ 𝑒(𝑑) 𝑓(𝑑,𝑒(𝑑)) ] + 𝑔(𝑑, 𝑒(𝑑), 𝐼0+ 0.7𝑒(𝑑), 𝐼0+ 0.2𝑒(𝑑)) + ∫ 𝐾 𝑑 0 (𝑑, 𝑠, 𝑒(𝑠)))𝑑𝑠 = 0 , 𝑑 ∈ 𝐼 = [0, 1]. (πŸ”) 𝑒(0) = β„Ž(𝑒), 100𝐷 ( 𝑒(𝑑) 𝑓(𝑑,𝑒(𝑑)) ) |𝑑=0 + 𝐢𝐷0+ 0.7 ( 𝑒(𝑑) 𝑓(𝑑,𝑒(𝑑)) ) |𝑑=1 = 0. (πŸ•) here 𝛼 = 1.7, πœ‡1 = 0.7, πœ‡2 = 0.2, π‘Ž = 100 and 𝑏 = 1. Where 𝑓(𝑑, 𝑒(𝑑)) = 7π‘’βˆ’3𝑑 15(𝑑2+2) |𝑒|+1 |𝑒|+2 , and β„Ž(𝑒) = sin(𝑒) 100+𝑒2 , and 𝑔(𝑑, 𝑒(𝑑), 𝐼0+ 0.7𝑒(𝑑), 𝐼0+ 0.2𝑒(𝑑)) = 3 100(𝑑2+1) [𝑒(𝑑) + |cos(𝐼0+ 0.7𝑒(𝑑)) βˆ’ π‘β„Ž(𝐼0+ 0.2𝑒(𝑑))|] + 𝑑 100 , and 𝐾(𝑑, 𝑠, 𝑒(𝑠)) = cos(𝑒2)π‘’βˆ’π‘‘(𝑠2+1) 100 Note that 𝑀𝑓 = supπ‘‘βˆˆπΌ ∣ 𝑓(𝑑, 0) ∣= 7π‘’βˆ’3𝑑 30(𝑑2+2) = 7 60 and 𝑀0 = | β„Ž(𝑒(𝑑) 𝑓(0,β„Ž(𝑒(𝑑)) | = 60 70 Setting 𝑀1 = 2 100 , πΊβˆ— = supπ‘‘βˆˆπΌ ∣ 𝑔(𝑑, 0, . . . ,0) ∣= 0.01, and we have ∣ 𝑓(𝑑, 𝑒) βˆ’ 𝑓(𝑑, 𝑣) βˆ£β‰€ 7π‘’βˆ’3𝑑 15(𝑑2+2) | 𝑒+1 𝑒+2 βˆ’ 𝑣+1 𝑣+2 | ≀ 7 30 | βˆ£π‘£βˆ’π‘’βˆ£ βˆ£π‘£+2βˆ£βˆ£π‘’+2∣ ≀ 7 30 ∣ 𝑣 βˆ’ 𝑒 ∣. then πœ†π‘“ = 7 30 , for 𝑒, 𝑣 ∈ ℝ, we have ∣ 𝑔(𝑑, 𝑣(𝑑), 𝐼0+ 0.7𝑣(𝑑), 𝐼0+ 0.2𝑣(𝑑)) βˆ’ 𝑔(𝑑, 𝑒(𝑑), 𝐼0+ 0.7𝑒(𝑑), 𝐼0+ 0.2𝑒(𝑑)) ∣ ≀ 3 100(𝑑2+1) (1 + 𝑑0.2 Ξ“(1.2) + 𝑑0.7 Ξ“(1.7) ) ∣ 𝑣 βˆ’ 𝑒 ∣ ≀ 3 100(𝑑2+1) (1 + 1 Ξ“(1.2) + 1 Ξ“(1.7) ) ∣ 𝑣 βˆ’ 𝑒 ∣ Thus, the assumption (A2) holds true with πœƒ(𝑑) = 3 100(𝑑2+1) and πœƒβˆ— = 0.03 and πœ‰ = 3.189672. 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