Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 3426 https://internationalpubls.com The Cauchy Problems for Fractional Q-Difference Equations with Integral Conditions in Banach Spaces Faouzi Hireche Abdelhamid Ibn Badis University, Mostaganem 27000, Algeria. faouzi.hireche.ma@gmail.com; faouzi.hireche@univ-mosta.dz Article History: Received: 19-08-2025 Revised: 24-09-2025 Accepted: 15-10-2025 Abstract: In In this paper, we investigate the existence of solutions to the fractional q- difference equation of the type 𝐷𝑐 π‘ž 𝛼𝑒(𝑑) = 𝐴𝑒(𝑑) + 𝑓(𝑑, 𝑒(𝑑)), 𝑑 ∈ 𝐽 ≔ [0,1] with 𝑒(0) = π‘Ž ∫ 𝑒(𝑠)π‘‘π‘žπ‘  + 𝑏, 1 0 where 0 < 𝛼 < 1, 𝑓 ∈ 𝐢(𝐽 Γ— 𝑋, 𝑋), and 𝐴(𝑑) is a bounded linear operator on a Banach space 𝑋 The operator 𝐷𝑐 π‘ž 𝛼𝑒(𝑑) denotes the Caputo fractional q-derivative of order 𝛼. Our existence result are obtained by using the Banach fixed point theorem and the Schaefer fixed point theorem. Keywords: Fixed point, Existence, Caputo fractional q-derivative, Fractional q- difference equations. 1. Introduction Over the past years, the theory of fractional calculus has received increasing attention from researchers and has become one of the most active areas of research due to its significant importance and wide applications on many subjects. The importance of this theory lies in its ability to contribute to mathematical modeling in various fields such as technical sciences, physics, engineering, biophysics and biomathematics. For more details, see [9–11, 13, 16]. At the beginning of the twentieth century, Jackson was the first to develop quantum calculus, also known as q-difference calculus, by introducing the concept of the q- integral along with several other fundamental notions in this theory. For further details on this topic, see references [8, 12]. In the late 1960s, a new branch known as fractional q-difference calculus emerged as a generalization of the q-difference calculus. This development is attributed to Al-Salam [6] and Agarwal [2]. This branch has received considerable attention in the academic community due to its wide range of applications in modeling mathematical phenomena across various scientific fields. Recently, Several researchers have studied the fractional q-difference equations in- volving the Caputo fractional q-derivative by using all kinds of fixed point theorems and obtained many interesting results , for example, by Abbas et al [1], Ahmad and al. [5]. In [3], N. Allouch et al studied the existence of solutions to the following fractional q-difference equations with nonlinear integral conditions: π·π‘ž 𝛼𝑐 𝑒(𝑑) = 𝑓(𝑑, 𝑒(𝑑)), 𝑑 ∈ 𝐼 = [0, 𝑇], 1 < 𝛼 ≀ 2, 𝑒(0) βˆ’ 𝑒′(0) = ∫ 𝑔(𝑠, 𝑒(𝑠))𝑑𝑠, 𝑇 0 mailto:faouzi.hireche.ma@gmail.com Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 3427 https://internationalpubls.com 𝑒(𝑇) + 𝑒′(𝑇) = ∫ β„Ž(𝑠, 𝑒(𝑠))𝑑𝑠, 𝑇 0 where 𝑇 > 0, π‘ž ∈]0,1[, 𝐷𝑐 π‘ž 𝛼 denotes the Caputo fractional q-difference derivative of order 1 < 𝛼 ≀ 2, and 𝑓, 𝑔, β„Ž ∈ 𝐢(𝐼 Γ— 𝑋,𝑋). In [4], N. Allouch et al applied some standard fixed point theorems and investigated the existence of solutions of fractional q-difference equations of the type: π·π‘ž 𝛼𝑐 𝑒(𝑑) = 𝑓(𝑑, 𝑒(𝑑)), 𝑑 ∈ 𝐼 = [0, 𝑇], 1 < 𝛼 ≀ 1, π‘Žπ‘’(0) + 𝑏𝑒(𝑇) = 𝑐, where 𝑇 > 0, π‘ž ∈]0,1[, 𝐷𝑐 π‘ž 𝛼 denotes the Caputo fractional q-difference derivative of order 𝛼, 𝑓 ∈ 𝐢(𝐼 Γ— 𝑋, 𝑋) an d π‘Ž + 𝑏 β‰  0. In this paper, we establish the existence of solutions to the fractional q-difference equations of the type: π·π‘ž 𝛼𝑐 𝑒(𝑑) = 𝐴(𝑑) + 𝑓(𝑑, 𝑒(𝑑)), 𝑑 ∈ 𝐽 ≔ [0,1], (1.1) 𝑒(0) = π‘Ž ∫ 𝑒(𝑠)π‘‘π‘žπ‘  + 𝑏, 1 0 (1.2) where 0 < 𝛼 < 1, 𝑓 ∈ 𝐢(𝐽 Γ— 𝑋, 𝑋), and 𝐴(𝑑) is a bounded linear operator on a Banach space 𝑋. The operator 𝐷𝑐 π‘ž 𝛼 denotes the Caputo fractional q-difference derivative of order 𝛼. The existence result is based on the fixed point theorem and the Schaefer fixed point theorem. The paper is structured as follows. In Section 2, we present the notations and definitions required for the study, and we review essential preliminaries from fractional q-calculus. Section 3 contains the principal results: the first derived from the Banach fixed point theorem, and the second from Schaefer’s fixed point theorem. Section 4 is devoted to an illustrative example highlighting the applicability of these results. 2. Preliminaries This section is concerned with presenting basic definitions together with auxiliary results required in the later parts of this paper. Assume that 𝑋 is a Banach space. Define 𝐽: = [0,1] and let 𝐢(𝐽, 𝑋) denote the Banach space of continuous functions 𝑒 from 𝐽 into 𝑋 with the norm β€–π‘’β€–βˆž = π‘ π‘’π‘π‘‘βˆˆπ½|𝑒(𝑑)|. Now, we introduce the essential definitions and relevant properties of the fractional q-calculus. For more details, see [8, 12]. We assume that π‘ž ∈]0,1[. For every π‘Ž ∈ ℝ, we define [π‘Ž]π‘ž = 1 βˆ’ π‘žπ‘Ž 1 βˆ’ π‘ž . Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 3428 https://internationalpubls.com Let π‘Ž, 𝑏 ∈ ℝ. The q-analogue of (π‘Ž βˆ’ 𝑏)(𝑛) is given by: (π‘Ž βˆ’ 𝑏)(𝑛) = { 1 𝑖𝑓 𝑛 = 0 ∏(π‘Ž βˆ’ π‘π‘žπ‘– π‘›βˆ’1 𝑖=0 ) 𝑖𝑓 𝑛 ∈ β„•βˆ— For 𝛽 ∈ ℝ, we have (π‘Ž βˆ’ 𝑏)(𝛽) = π‘Žπ›½βˆ( π‘Ž βˆ’ π‘π‘žπ‘– π‘Ž βˆ’ π‘π‘žπ‘–+𝛽 ) , π‘Ž, 𝑏 ∈ ℝ. ∞ 𝑖=0 Note that, if 𝑏 = 0, then π‘Ž(𝛽) = π‘Žπ›½ . Definition 1 [12] The q-gamma function is defined as follows: Ξ“π‘ž(𝛽) = (1 βˆ’ π‘ž)(π›½βˆ’1) (1 βˆ’ π‘ž)π›½βˆ’1 , 𝛽 > 0. Observe that the q-gamma function verifies Ξ“π‘ž(𝛽 + 1) = [𝛽]π‘žΞ“π‘ž(𝛽). Definition 2 [12] Let 𝑓: 𝐽 β†’ ℝ. The q-derivative of order 𝑛 ∈ β„• is given by: (π·π‘ž 0𝑓)(𝑑) = 𝑓(𝑑), (π·π‘ž 1𝑓)(𝑑) = 𝑓(𝑑) βˆ’ 𝑓(π‘žπ‘‘) (1 βˆ’ π‘ž)𝑑 , π‘Žπ‘›π‘‘ (π·π‘ž 𝑛𝑓)(𝑑) = (π·π‘ž 1π·π‘ž π‘›βˆ’1𝑓)(𝑑), 𝑛 ∈ β„•βˆ—. Definition 3 [12] Let 𝐽𝑑 = {π‘‘π‘ž 𝑛: 𝑛 ∈ β„•}⋃{0}. The q-integral of a function 𝑓: 𝐽𝑑 β†’ ℝ is defined by: (πΌπ‘žπ‘“)(𝑑) = ∫ 𝑓(𝑠)π‘‘π‘žπ‘  = βˆ‘π‘‘(1 βˆ’ π‘ž)π‘žπ‘›π‘“(π‘‘π‘žπ‘›), ∝ 𝑛=0 1 0 under the assumption that the series converges. Note that (π·π‘žπΌπ‘žπ‘“)(𝑑) = 𝑓(𝑑), Furthermore, if 𝑓 is continuous at 0, then (πΌπ‘žπ·π‘žπ‘“)(𝑑) = 𝑓(𝑑) βˆ’ 𝑓(0). Definition 4 [2] Let 𝑓: 𝐽 β†’ ℝ. the Riemann-Liouville fractional q-integral of order 𝛼 β‰₯ 0 is defined as: (πΌπ‘ž 𝛼𝑓)(𝑑) = { 𝑓(𝑑) 𝑖𝑓 𝛼 = 0, ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1) Ξ“π‘ž(𝛼) 𝑓(𝑠)π‘‘π‘žπ‘  𝑑 0 𝑖𝑓 𝛼 > 0. Observe that when 𝛼 = 1, we have (πΌπ‘ž 1𝑓)(𝑑) = (πΌπ‘žπ‘“)(𝑑). Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 3429 https://internationalpubls.com Lemma 5 [15] For all 𝛼 β‰₯ 0 and 𝛽 ∈] βˆ’ 1,+∞[, we have (πΌπ‘ž 𝛼(𝑑 βˆ’ π‘Ž)(𝛽))(𝑑) = Ξ“π‘ž(𝛽 + 1) Ξ“π‘ž(𝛼 + 𝛽 + 1) (𝑑 βˆ’ π‘Ž)(𝛼+𝛽), 0 < 𝛼 < 𝑑 < 1. In particular, (πΌπ‘ž 𝛼1)(𝑑) = 1 Ξ“π‘ž(𝛼 + 1) 𝑑(𝛼). Definition 6 [14] The Riemann-Liouville fractional q-derivative of order 𝛼 β‰₯ 0 for a function 𝑓: 𝐽 β†’ ℝ is defined as follows: (π·π‘ž 0𝑓)(𝑑) = 𝑓(𝑑) and (π·π‘ž 𝛼𝑓)(𝑑) = (π·π‘ž [𝛼]πΌπ‘ž [𝛼]βˆ’π›Όπ‘“) (𝑑), 𝑑 ∈ 𝐽, where [𝛼] is the integer part of 𝛼. Definition 7 [14] Consider a function 𝑓: 𝐽 β†’ ℝ and let 𝛼 β‰₯ 0. The Caputo fractional q- derivative of order 𝛼 is defined as follows: (π·π‘ž 0𝑓)(𝑑) = 𝑓(𝑑) and ( π·π‘ž 𝛼𝑐 𝑓)(𝑑) = (πΌπ‘ž [𝛼]βˆ’π›Ό π·π‘ž [𝛼] 𝑓) (𝑑), 𝑑 ∈ 𝐽, where [𝛼] is the integer part of 𝛼. Lemma 8 [14] Suppose that 𝛼,𝛽 β‰₯ 0, and let 𝑓: 𝐽 β†’ ℝ be a given function. Then, the following identities hold: (i) (πΌπ‘ž π›ΌπΌπ‘ž 𝛽 𝑓)(𝑑) = (πΌπ‘ž 𝛼+𝛽 𝑓)(𝑑), (ii) (π·π‘ž π›ΌπΌπ‘ž 𝛽 𝑓)(𝑑) = 𝑓(𝑑). Lemma 9 [14] Assume 𝛼 β‰₯ 0, and let 𝑓 be a function defined on the interval 𝐽. The following identity holds (πΌπ‘ž 𝛼 π·π‘ž 𝛼𝑐 𝑓)(𝑑) = 𝑓(𝑑) βˆ’ βˆ‘ π‘‘π‘˜ Ξ“π‘ž(π‘˜ + 1) (π·π‘ž 𝛼𝑓)(0). [𝛼]βˆ’1 π‘˜=0 If 𝛼 ∈]0,1[, we have (πΌπ‘ž 𝛼 π·π‘ž 𝛼𝑐 𝑓)(𝑑) = 𝑓(𝑑) βˆ’ 𝑓(0). Theorem 10 (Banach contraction principle) [7] Suppose that 𝐢 is a non-empty closed subset of a Banach space 𝑋. If 𝐻: 𝐢 β†’ 𝐢 is a contraction, then 𝐻 admits a unique fixed point in 𝐢. Theorem 11 (Schaefer) [17] Let 𝑋 be a Banach space and let 𝐻:𝑋 β†’ 𝑋 be a completely continuous operator. Assume that the set β„° ≔ {𝑒 ∈ 𝑋 |𝑒 = πœ†π»(𝑒), πœ† ∈]0,1[} is bounded. Then 𝐻 admits a fixed point in 𝑋. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 3430 https://internationalpubls.com 3. Existence In this section, we investigate the existence of solutions for the fractional qqq-difference problem given by (1.1)-(1.2). Definition 12 A function 𝑒 ∈ 𝐢([0,1], 𝑋) is called a solution of the fractional q-difference problem (1.1)-(1.2) if 𝑒 satisfies the equation 𝐷𝑐 π‘ž 𝛼𝑒(𝑑) = 𝐴𝑒(𝑑) + 𝑓(𝑑, 𝑒(𝑑)) on 𝐽 = [0,1], and the condition 𝑒(0) = π‘Ž ∫ 𝑒(𝑠)π‘‘π‘žπ‘  + 𝑏. 1 0 To establish the existence of solutions for the fractional problem (1.1)-(1.2), we require the following lemma: Lemma 13 Let 𝛼 ∈]0,1[ and let β„Ž: [0,1] Γ— 𝑋 β†’ 𝑋 be continuous function. The solution of the fractional q-difference problem π·π‘ž 𝛼𝑐 𝑒(𝑑) = 𝐴(𝑑) + 𝑓(𝑑, 𝑒(𝑑)), 𝑑 ∈ 𝐽 = [0,1], 𝑒(0) = π‘Ž ∫ 𝑒(𝑠)π‘‘π‘žπ‘  + 𝑏, 1 0 is given by 𝑒(𝑑) = π‘Žβˆ« 𝑒(𝑠)π‘‘π‘žπ‘  + 𝑏 + 1 Ξ“π‘ž(𝛼) ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1) 𝑑 0 𝑓(𝑠, 𝑒(𝑠))π‘‘π‘žπ‘  1 0 + 1 Ξ“π‘ž(𝛼) ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1)𝐴𝑒(𝑠)π‘‘π‘žπ‘ . 𝑑 0 The first result is obtained by applying the Banach fixed point theorem. Theorem 14 Suppose that: (𝐻1) There exist π‘˜ > 0 such that βˆ€π‘‘ ∈ 𝐽, βˆ€π‘’, 𝑣 ∈ 𝑋, |𝑓(𝑑, 𝑒) βˆ’ 𝑓(𝑑, 𝑣)| ≀ π‘˜|𝑒 βˆ’ 𝑣|. If |𝛼| + π‘˜ + ‖𝐴‖ℒ(𝑋) Ξ“π‘ž(𝛼 + 1) < 1. (3.1) Then, the fractional q-difference problem (1.1)-(1.2) admits a unique solution on [0,1]. Proof 15 The fractional q-difference problem (1.1)-(1.2) can be reformulated in terms of a fixed point problem. For this purpose, we define the operator 𝐹: 𝐢([0,1], 𝑋) β†’ 𝐢([0,1], 𝑋), where Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 3431 https://internationalpubls.com 𝐹(𝑒(𝑑)) ≔ π‘Žβˆ« 𝑒(𝑠)π‘‘π‘žπ‘  + 𝑏 + 1 Ξ“π‘ž(𝛼) ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1) 𝑑 0 𝑓(𝑠, 𝑒(𝑠))π‘‘π‘žπ‘  1 0 (3.2) + 1 Ξ“π‘ž(𝛼) ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1)𝐴𝑒(𝑠)π‘‘π‘žπ‘ . 𝑑 0 It is evident that the fixed points of the operator 𝐹 correspond to solutions of the fractional q- difference problem (1.1)-(1.2). We shall use the Banach contraction mapping principle to demonstrate that 𝐹 defined by (3.2) has a fixed point. We shall demonstrate that 𝐹 is a contraction. Let 𝑒, 𝑣 ∈ 𝐢([0,1], 𝑋) and 𝑑 ∈ [0,1], we obtain |𝐹(𝑒)(𝑑) βˆ’ 𝐹(𝑣)(𝑑)| ≀ |π‘Ž|∫ |𝑒(𝑠) βˆ’ 𝑣(𝑠)|π‘‘π‘žπ‘  + 1 Ξ“π‘ž(𝛼) ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1) 𝑑 0 |𝑓(𝑠, 𝑒(𝑠)) βˆ’ 𝑓(𝑠, 𝑣(𝑠))|π‘‘π‘žπ‘  1 0 + 1 Ξ“π‘ž(𝛼) ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1)‖𝐴‖ℒ(𝑋)|𝑒(𝑠) 𝑑 0 βˆ’ 𝑣(𝑠)|π‘‘π‘žπ‘  ≀ |π‘Ž|π‘ π‘’π‘π‘ βˆˆ[0,1]|𝑒(𝑠) βˆ’ 𝑣(𝑠)| + π‘˜ Ξ“π‘ž(𝛼) π‘ π‘’π‘π‘ πœ–[0,1]|𝑒(𝑠) βˆ’ 𝑣(𝑠)|∫ (𝑑 βˆ’ π‘žπ‘ ) (π›Όβˆ’1)π‘‘π‘žπ‘  𝑑 0 + ‖𝐴‖ℒ(𝑋) Ξ“π‘ž(𝛼) π‘ π‘’π‘π‘ πœ–[0,1]|𝑒(𝑠) βˆ’ 𝑣(𝑠)|∫ (𝑑 βˆ’ π‘žπ‘ ) (π›Όβˆ’1)π‘‘π‘žπ‘  𝑑 0 ≀ |π‘Ž|π‘ π‘’π‘π‘ βˆˆ[0,1]|𝑒(𝑠) βˆ’ 𝑣(𝑠)| + π‘˜ Ξ“π‘ž(𝛼 + 1) π‘ π‘’π‘π‘ πœ–[0,1]|𝑒(𝑠) βˆ’ 𝑣(𝑠)| + ‖𝐴‖ℒ(𝑋) Ξ“π‘ž(𝛼 + 1) π‘ π‘’π‘π‘ πœ–[0,1]|𝑒(𝑠) βˆ’ 𝑣(𝑠)| = (|π‘Ž| + π‘˜ + ‖𝐴‖ℒ(𝑋) Ξ“π‘ž(𝛼 + 1) )π‘ π‘’π‘π‘ βˆˆ[0,1]|𝑒(𝑠) βˆ’ 𝑣(𝑠)|. Hence, ‖𝐹(𝑒) βˆ’ 𝐹(𝑣)β€–βˆž ≀ [|π‘Ž| + π‘˜ + ‖𝐴‖ℒ(𝑋) Ξ“π‘ž(𝛼 + 1) ] ‖𝑒 βˆ’ π‘£β€–βˆž. According to (3.2), the operator 𝐹 satisfies the contraction condition. Hence, by the Banach fixed point theorem, 𝐹 admits a fixed point, representing the solution of the fractional q-difference problem (1.1)-(1.2). Theorem 16 Suppose that: (𝐻2) The function 𝑓: [0,1] Γ— 𝑋 β†’ 𝑋 is continuous. (𝐻3) βˆƒπ‘€ > 0, βˆ€π‘‘ ∈ 𝐽, βˆ€π‘’ ∈ 𝑋, |𝑓(𝑑, 𝑒)| ≀ 𝑀. Hence, the fractional q-difference problem (1.1)-(1.2) admits at least one solution on [0,1]. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 3432 https://internationalpubls.com Proof 17 We apply Schaefer’s fixed point theorem to verify that the operator 𝐹, defined in (3.2), admits a fixed point. The proof is organized in four steps. Step 1: 𝐹 is continuous operator. Consider a sequence {𝑒𝑛} such that 𝑒𝑛 β†’ 𝑒 in 𝐢([0,1], 𝑋). Then for all 𝑑 ∈ [0,1]: |𝐹(𝑒𝑛)(𝑑) βˆ’ 𝐹(𝑒)(𝑑)| ≀ |π‘Ž|∫ |𝑒𝑛(𝑠) βˆ’ 𝑒(𝑠)|π‘‘π‘žπ‘  1 0 + 1 Ξ“π‘ž(𝛼) ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1)|𝑓(𝑠, 𝑒𝑛(𝑠)) βˆ’ 𝑓(𝑠, 𝑒(𝑠))|π‘‘π‘žπ‘  1 0 + 1 Ξ“π‘ž(𝛼) ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1)‖𝐴‖ℒ(𝑋)|𝑒𝑛(𝑠) βˆ’ 𝑒(𝑠)|π‘‘π‘žπ‘  𝑑 0 ≀ |π‘Ž|π‘ π‘’π‘π‘ βˆˆ[0,1]|𝑒𝑛(𝑠) βˆ’ 𝑒(𝑠)| + 1 Ξ“π‘ž(𝛼) π‘ π‘’π‘π‘ βˆˆ[0,1]|𝑓(𝑠, 𝑒𝑛(𝑠)) βˆ’ 𝑓(𝑠, 𝑒(𝑠))|∫ (𝑑 βˆ’ π‘žπ‘ ) (π›Όβˆ’1) 𝑑 0 π‘‘π‘žπ‘  + ‖𝐴‖ℒ(𝑋) Ξ“π‘ž(𝛼) π‘ π‘’π‘π‘ βˆˆ[0,1]|𝑒𝑛(𝑠) βˆ’ 𝑒(𝑠)|∫ (𝑑 βˆ’ π‘žπ‘ ) (π›Όβˆ’1)π‘‘π‘žπ‘  𝑑 0 ≀ |π‘Ž|π‘ π‘’π‘π‘ βˆˆ[0,1]|𝑒𝑛(𝑠) βˆ’ 𝑒(𝑠)| + 1 Ξ“π‘ž(𝛼 + 1) π‘ π‘’π‘π‘ βˆˆ[0,1]|𝑓(𝑠, 𝑒𝑛(𝑠)) βˆ’ 𝑓(𝑠, 𝑒(𝑠))| + ‖𝐴‖ℒ(𝑋) Ξ“π‘ž(𝛼 + 1) π‘ π‘’π‘π‘ βˆˆ[0,1]|𝑒𝑛(𝑠) βˆ’ 𝑒(𝑠)| = (|π‘Ž| + ‖𝐴‖ℒ(𝑋) Ξ“π‘ž(𝛼 + 1) ) π‘ π‘’π‘π‘ βˆˆ[0,1]|𝑒𝑛(𝑠) βˆ’ 𝑒(𝑠)| + 1 Ξ“π‘ž(𝛼 + 1) π‘ π‘’π‘π‘ βˆˆ[0.1]|𝑓(𝑠, 𝑒𝑛(𝑠)) βˆ’ 𝑓(𝑠, 𝑒(𝑠))|. Since the function 𝑓 is a continuous, we have ‖𝐹(𝑒𝑛) βˆ’ 𝐹(𝑒)β€–βˆž ≀ (|π‘Ž| + ‖𝐴‖𝓛(𝑋) Ξ“π‘ž(𝛼 + 1) ) ‖𝑒𝑛(βˆ™) βˆ’ 𝑒(βˆ™)β€–βˆž + 1 Ξ“π‘ž(𝛼 + 1) ‖𝑓(βˆ™, 𝑒𝑛(βˆ™)) βˆ’ 𝑓(βˆ™, 𝑒(βˆ™))β€–βˆž 𝑛→+∞ β†’ 0. Step 2: 𝐹 maps bounded sets into bounded sets in 𝐢([0,1], 𝑋). Indeed, it is enough to prove that for every πœ‚βˆ— > 0, there exists a constant β„“ > 0 such that for all 𝑒 ∈ π΅πœ‚βˆ— = {𝑒 ∈ 𝐢([0,1], ℝ): β€–π‘’β€–βˆž ≀ πœ‚ βˆ—}, we have ‖𝐹(𝑒)β€–βˆž ≀ β„“. By (𝐻3) we have for every 𝑑 ∈ [0,1]: Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 3433 https://internationalpubls.com |𝐹(𝑒)(𝑑)| ≀ |π‘Ž| ∫ |𝑒(𝑠)|π‘‘π‘žπ‘  1 0 + |𝑏| + 1 Ξ“π‘ž(𝛼) ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1) 𝑑 0 |𝑓(𝑠, 𝑒(𝑠))|π‘‘π‘žπ‘  + 1 Ξ“π‘ž(𝛼) ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1) 𝑑 0 ‖𝐴‖ℒ(𝑋)|𝑒(𝑠)|π‘‘π‘žπ‘  ≀ |π‘Ž|πœ‚βˆ— + |𝑏| + 𝑀 Ξ“π‘ž(𝛼) ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1)π‘‘π‘žπ‘  𝑑 0 + ‖𝐴‖ℒ(𝑋)πœ‚ βˆ— Ξ“π‘ž(𝛼) ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1) 𝑑 0 π‘‘π‘žπ‘  ≀ |π‘Ž|πœ‚βˆ— + |𝑏| + 𝑀 Ξ“π‘ž(𝛼 + 1) + ‖𝐴‖ℒ(𝑋)πœ‚ βˆ— Ξ“π‘ž(𝛼 + 1) . Hence ‖𝐹(𝑒)β€–βˆž ≀ |π‘Ž|πœ‚ βˆ— + |𝑏| + 𝑀 Ξ“π‘ž(𝛼 + 1) + ‖𝐴‖ℒ(𝑋)πœ‚ βˆ— Ξ“π‘ž(𝛼 + 1) ≔ β„“. Step 3: The operator 𝐹 maps bounded sets into equicontinuous sets of 𝐢([0,1], 𝑋). For 𝑑1, 𝑑2 ∈ [0,1] with 𝑑1 < 𝑑2, and for 𝑒 ∈ π΅πœ‚βˆ— , where π΅πœ‚βˆ— is the bounded subset of 𝐢([0,1], 𝑋) defined in step 2, we have |𝐹(𝑒)(𝑑2) βˆ’ 𝐹(𝑒)(𝑑1)| = | 1 Ξ“π‘ž(𝛼) ∫ [(𝑑2 βˆ’ π‘žπ‘ ) (π›Όβˆ’1) βˆ’ (𝑑1 βˆ’ π‘žπ‘ ) (π›Όβˆ’1)]𝑓(𝑠, 𝑒(𝑠))π‘‘π‘žπ‘  𝑑1 0 + 1 Ξ“π‘ž(𝛼) ∫ [(𝑑2 βˆ’ π‘žπ‘ ) (π›Όβˆ’1) βˆ’ (𝑑1 βˆ’ π‘žπ‘ ) (π›Όβˆ’1)]𝐴𝑒(𝑠)π‘‘π‘žπ‘  𝑑1 0 + 1 Ξ“π‘ž(𝛼) ∫ (𝑑2 βˆ’ π‘žπ‘ ) (π›Όβˆ’1)𝑓(𝑠, 𝑒(𝑠))π‘‘π‘žπ‘  + 1 Ξ“π‘ž(𝛼) ∫ (𝑑2 βˆ’ π‘žπ‘ ) (π›Όβˆ’1)𝐴𝑒(𝑠)π‘‘π‘žπ‘  𝑑2 𝑑1 𝑑2 𝑑1 | ≀ 𝑀 Ξ“π‘ž(𝛼) ∫ [(𝑑1 βˆ’ π‘žπ‘ ) (π›Όβˆ’1) βˆ’ (𝑑2 βˆ’ π‘žπ‘ ) (π›Όβˆ’1)]𝑓(𝑠, 𝑒(𝑠))π‘‘π‘žπ‘  𝑑1 0 + πœ‚βˆ—β€–π΄β€–β„’(𝑋) Ξ“π‘ž(𝛼) ∫ [(𝑑1 βˆ’ π‘žπ‘ ) (π›Όβˆ’1) βˆ’ (𝑑2 βˆ’ π‘žπ‘ ) (π›Όβˆ’1)]π‘‘π‘žπ‘  𝑑1 0 + 𝑀 Ξ“π‘ž(𝛼) ∫ (𝑑2 βˆ’ π‘žπ‘ ) (π›Όβˆ’1)π‘‘π‘žπ‘  + πœ‚βˆ—β€–π΄β€–β„’(𝑋) Ξ“π‘ž(𝛼) ∫ (𝑑2 βˆ’ π‘žπ‘ ) (π›Όβˆ’1)π‘‘π‘žπ‘  𝑑2 𝑑1 𝑑2 𝑑1 ≀ 𝑀 Ξ“π‘ž(𝛼 + 1) [(𝑑2 βˆ’ 𝑑1) (𝛼) + 𝑑1 (𝛼) βˆ’ 𝑑2 (𝛼)] + πœ‚βˆ—β€–π΄β€–β„’(𝑋) Ξ“π‘ž(𝛼 + 1) [(𝑑2 βˆ’ 𝑑1) (𝛼) + 𝑑1 (𝛼) βˆ’ 𝑑2 (𝛼)] + 𝑀 Ξ“π‘ž(𝛼 + 1) (𝑑2 βˆ’ 𝑑1) (𝛼) + πœ‚βˆ—β€–π΄β€–β„’(𝑋) Ξ“π‘ž(𝛼 + 1) (𝑑2 βˆ’ 𝑑1) (𝛼) ≀ [ 2𝑀 Ξ“π‘ž(𝛼 + 1) + 2πœ‚βˆ—β€–π΄β€–β„’(𝑋) Ξ“π‘ž(𝛼 + 1) ] (𝑑2 βˆ’ 𝑑1) (𝛼) + [ 𝑀 Ξ“π‘ž(𝛼 + 1) + πœ‚βˆ—β€–π΄β€–β„’(𝑋) Ξ“π‘ž(𝛼 + 1) ] (𝑑2 βˆ’ 𝑑1) (𝛼). As 𝑑1 β†’ 𝑑2, the right-hand side of the preceding inequality tends to zero. As a consequence of step 1 to 3 tougher with the ArzelΓ -Ascoli theorem, we can conclude that the operator 𝐹: 𝐢([0,1], 𝑋) β†’ 𝐢([0,1], 𝑋) is continuous and completely continuous. Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 3434 https://internationalpubls.com Step 4: A priori bounds. By Schauder’s fixed point theorem, it is sufficient to show that the set: β„° = {𝑒 ∈ 𝐢([0,1], 𝑋) |𝑒 = πœ†πΉ(𝑒), πœ† ∈]0,1[} is bounded. Let 𝑒 ∈ β„°. Then there exists πœ† ∈]0,1[ such that 𝑒 = πœ†πΉ(𝑒). Hence, for every 𝑑 ∈ [0,1], we have 𝑒(𝑑) = πœ† [π‘Žβˆ« 𝑒(𝑠)π‘‘π‘žπ‘  + 𝑏 + 1 Ξ“π‘ž(𝛼) ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1) 𝑑 0 𝑓(𝑠, 𝑒(𝑠))π‘‘π‘žπ‘  1 0 + 1 Ξ“π‘ž(𝛼) ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1)𝐴𝑒(𝑠)π‘‘π‘žπ‘  𝑑 0 ]. Under hypothesis (𝐻3), it follows that for every 𝑑 ∈ [0,1]: |𝐹(𝑒)(𝑑)| ≀ |π‘Ž|∫ |𝑒(𝑠)|π‘‘π‘žπ‘  1 0 + |𝑏| + 1 Ξ“π‘ž(𝛼) ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1) 𝑑 0 |𝑓(𝑠, 𝑒(𝑠))|π‘‘π‘žπ‘  + 1 Ξ“π‘ž(𝛼) ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1) 𝑑 0 ‖𝐴‖ℒ(𝑋)|𝑒(𝑠)|π‘‘π‘žπ‘  ≀ |π‘Ž| π‘ π‘’π‘π‘ βˆˆ[0,1]|𝑒(𝑠)| + |𝑏| + 𝑀 Ξ“π‘ž(𝛼) ∫ (𝑑 βˆ’ π‘žπ‘ )(π›Όβˆ’1)π‘‘π‘žπ‘  𝑑 0 + ‖𝐴‖ℒ(𝑋) Ξ“π‘ž(𝛼) π‘ π‘’π‘π‘ βˆˆ[0,1]|𝑒(𝑠)|∫ (𝑑 βˆ’ π‘žπ‘ ) (π›Όβˆ’1) 𝑑 0 π‘‘π‘žπ‘  ≀ |π‘Ž| π‘ π‘’π‘π‘ βˆˆ[0,1]|𝑒(𝑠)| + |𝑏| + 𝑀 Ξ“π‘ž(𝛼 + 1) + ‖𝐴‖ℒ(𝑋) Ξ“π‘ž(𝛼 + 1) π‘ π‘’π‘π‘ βˆˆ[0,1]|𝑒(𝑠)|. Then, for every 𝑑 ∈ [0,1], we have ‖𝐹(𝑒)β€–βˆž ≀ |π‘Ž| π‘ π‘’π‘π‘ βˆˆ[0,1]|𝑒(𝑠)| + |𝑏| + 𝑀 Ξ“π‘ž(𝛼 + 1) + ‖𝐴‖ℒ(𝑋) Ξ“π‘ž(𝛼 + 1) π‘ π‘’π‘π‘ βˆˆ[0,1]|𝑒(𝑠)| ≔ 𝑅. This shows that the set β„° is bounded. Consequently, by Schaefer fixed point theorem, we conclude that 𝐹 admits a fixed point which is a solution of the problem (1.1)-(1.2). 4. Application In this section, we provide an illustrative example to demonstrate the applicability of our result. Consider the following fractional q-difference problem with an integral boundary condition: 𝐷1 3 1 2𝑐 𝑒(𝑑) = 𝑑 100 𝑒(𝑑) + 𝑒(𝑑) (1+π‘π‘œπ‘ (𝑒(𝑑))) , 𝑑 ∈ [0,1], (4.1) 𝑒(0) = 2 3 ∫ 𝑒(𝑠)𝑑1 3 𝑠 + 1 2 . 1 0 (4.2) Communications on Applied Nonlinear Analysis ISSN: 1074-133X Vol 32 No. 10s (2025) 3435 https://internationalpubls.com Let 𝑓(𝑑, 𝑒) = 𝑒 (1 + π‘π‘œπ‘ (𝑒)) , (𝑑, 𝑒) ∈ [0,1] Γ—]0,+∞[ and 𝐴(𝑑) = 𝑑 100 . For all 𝑒, 𝑣 ∈]0,+∞[ and 𝑑 ∈ [0,1]. We have |𝑓(𝑑, 𝑒) βˆ’ 𝑓(𝑑, 𝑣)| ≀ | 𝑒 βˆ’ 𝑣 (1 + cos(𝑒))(1 + cos(𝑣)) | ≀ 1 4 |𝑒 βˆ’ 𝑣|. We see that the condition |π‘Ž| + π‘˜+‖𝐴‖ Ξ“π‘ž(𝛼+1) β‰ˆ 0.93 < 1 holds with 𝛼 = 1 2 , π‘˜ = 1 4 , π‘ž = 1 3 , ‖𝐴‖ = 1 100 and Ξ“1 3 ( 3 2 ) β‰ˆ 0.9376. Consequently, by Theorem 14, the fractional q-difference problem (4.1)- (4.2) admits a unique solution on the interval [0,1]. 5. 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