Research article

Explicit evaluations of subfamilies of the hypergeometric function 3F2(1) along with specific fractional integrals

  • Received: 02 February 2025 Revised: 01 March 2025 Accepted: 07 March 2025 Published: 14 March 2025
  • MSC : 26A33, 33C05, 33C20

  • The present study explores the application of hypergeometric functions in evaluating fractional integrals, providing a comprehensive framework to bridge fractional calculus and special functions. As a generalization of classical integrals, fractional integrals have gained prominence due to their wide applicability in modeling anomalous diffusion, viscoelastic systems, and other non-local phenomena. Hypergeometric functions, renowned for their rich analytical properties and ability to represent solutions to differential equations, offer an elegant and versatile tool for solving fractional integrals. In this paper, we evaluate a new class of fractional integrals, presenting results that contribute significantly to the study of generalized hypergeometric functions, particularly 3F2(1). The results reveal previously unexplored connections within these functions, providing new insights and extending their applicability. Furthermore, evaluating these fractional integrals holds promise for advancing the theoretical understanding and practical applications of fractional differential equations.

    Citation: Abdelhamid Zaidi, Saleh Almuthaybiri. Explicit evaluations of subfamilies of the hypergeometric function 3F2(1) along with specific fractional integrals[J]. AIMS Mathematics, 2025, 10(3): 5731-5761. doi: 10.3934/math.2025264

    Related Papers:

    [1] Mahmoud Abul-Ez, Mohra Zayed, Ali Youssef . Further study on the conformable fractional Gauss hypergeometric function. AIMS Mathematics, 2021, 6(9): 10130-10163. doi: 10.3934/math.2021588
    [2] Gauhar Rahman, Shahid Mubeen, Kottakkaran Sooppy Nisar . On generalized $\mathtt{k}$-fractional derivative operator. AIMS Mathematics, 2020, 5(3): 1936-1945. doi: 10.3934/math.2020129
    [3] Muajebah Hidan, Mohamed Akel, Hala Abd-Elmageed, Mohamed Abdalla . Solution of fractional kinetic equations involving extended $ (k, \tau) $-Gauss hypergeometric matrix functions. AIMS Mathematics, 2022, 7(8): 14474-14491. doi: 10.3934/math.2022798
    [4] A. Belafhal, N. Nossir, L. Dalil-Essakali, T. Usman . Integral transforms involving the product of Humbert and Bessel functions and its application. AIMS Mathematics, 2020, 5(2): 1260-1274. doi: 10.3934/math.2020086
    [5] Marta Na Chen, Wenchang Chu . Yabu's formulae for hypergeometric $ _3F_2 $-series through Whipple's quadratic transformations. AIMS Mathematics, 2024, 9(8): 21799-21815. doi: 10.3934/math.20241060
    [6] D. L. Suthar, D. Baleanu, S. D. Purohit, F. Uçar . Certain k-fractional calculus operators and image formulas of k-Struve function. AIMS Mathematics, 2020, 5(3): 1706-1719. doi: 10.3934/math.2020115
    [7] Saima Naheed, Shahid Mubeen, Thabet Abdeljawad . Fractional calculus of generalized Lommel-Wright function and its extended Beta transform. AIMS Mathematics, 2021, 6(8): 8276-8293. doi: 10.3934/math.2021479
    [8] Ali Khalouta, Abdelouahab Kadem . A new computational for approximate analytical solutions of nonlinear time-fractional wave-like equations with variable coefficients. AIMS Mathematics, 2020, 5(1): 1-14. doi: 10.3934/math.2020001
    [9] Muhammad Imran Liaqat, Sina Etemad, Shahram Rezapour, Choonkil Park . A novel analytical Aboodh residual power series method for solving linear and nonlinear time-fractional partial differential equations with variable coefficients. AIMS Mathematics, 2022, 7(9): 16917-16948. doi: 10.3934/math.2022929
    [10] A. Khoshkenar, M. Ilie, K. Hosseini, D. Baleanu, S. Salahshour, C. Park, J. R. Lee . Further studies on ordinary differential equations involving the $ M $-fractional derivative. AIMS Mathematics, 2022, 7(6): 10977-10993. doi: 10.3934/math.2022613
  • The present study explores the application of hypergeometric functions in evaluating fractional integrals, providing a comprehensive framework to bridge fractional calculus and special functions. As a generalization of classical integrals, fractional integrals have gained prominence due to their wide applicability in modeling anomalous diffusion, viscoelastic systems, and other non-local phenomena. Hypergeometric functions, renowned for their rich analytical properties and ability to represent solutions to differential equations, offer an elegant and versatile tool for solving fractional integrals. In this paper, we evaluate a new class of fractional integrals, presenting results that contribute significantly to the study of generalized hypergeometric functions, particularly 3F2(1). The results reveal previously unexplored connections within these functions, providing new insights and extending their applicability. Furthermore, evaluating these fractional integrals holds promise for advancing the theoretical understanding and practical applications of fractional differential equations.



    Historically, hypergeometric functions emerged during the 18th century in the work of mathematicians such as Euler and Gauss, who developed theories around hypergeometric series and associated integrals. These functions were first considered as generalizations of geometric series and solutions of higher-order linear differential equations. Today, hypergeometric functions are at the center of an entire field of research, that of special functions [1]. Moreover, it is now well known that most special functions can be expressed in terms of hypergeometric functions, and these functions can be represented using either series or integrals. This dual representation makes it an excellent tool for evaluating series and integrals or solving differential equations. Hypergeometric functions have a wide range of applications. From our literature review, we found that these functions are utilized to express solutions in various fields, including probability and statistics [2,3,4], combinatorics and number theory [5,6,7], random walks [8,9,10], random graphs [11], quantum mechanics (see [12], p. 89, 96, 127 and [13], p. 235, 290, 333), conformal mapping [14], and fractional hypergeometric differential equations [15,16], among many other problems.

    Hypergeometric functions usually have no explicit expression and are only represented by power series or integrals, which makes their evaluation time-consuming. Research on hypergeometric functions is divided into two main branches: continuous and discrete. The continuous branch focuses on the analytical study of these functions, treating their arguments as continuous variables (see [17,18,19,20,21,22,23,24]). In contrast, the discrete branch examines these functions by substituting their arguments with integers or specific values. Research in the discrete branch has surged in the past decade, driven by advancements in powerful computer algebra software and the wide range of problems that can be solved using hypergeometric functions. This study belongs to the discrete branch and aims to provide new results for different families of the generalized hypergeometric function 3F2(1). The literature includes several explicit forms of 3F2(a1,a2,a3;b1;b2;1), for particular choices of the parameters (a1,a2,a3,b1,b2). Thus, in [25], the authors used the Gamma function to derive explicit forms for 3F2(a,b,c;1+ab,1+ac;1) and 3F2(a,b,c;1+ab,a+2bc1;1). Moreover, in [26], the authors used specialized software and managed to generate, without any mathematical proof, about thirty explicit formulas of 3F2(a1,a2,a3;b1;b2;1), for particular choices of the parameters (a1,a2,a3,b1,b2). Furthermore, in [27], the authors exhibited the explicit expressions of 3F2(2n,a,1+d;2a+1,d;2) and 3F2(2n1,a,1+d;2a+1,d;2) for nN. Besides, in [28], the authors succeeded in determining the explicit expressions of the following sequences:

    3F2(16,56,12+n;1,32+n;1),3F2(16,56,12n;1,12n;1),3F2(16,56,13+n;1,43+n;1),3F2(16,56,13n;1,23n;1),3F2(16,56,23+n;1,53+n;1),3F2(16,56,23n;1,13n;1),3F2(16,56,14+n;1,54+n;1),3F2(16,56,14n;1,34+n;1),3F2(16,56,34+n;1,74+n;1),3F2(16,56,14n;1,14n;1),

    for all nN. Finally, in [29], the authors provided the explicit forms of the sets 3F2(2x,2x+12,x;12,1+x;1) and 3F2(2x,2x12,x;32,1+x;1), for all x(,14).

    The main objective of our study is to find explicit forms for the sets:

    K(α)=3F2(1α,1,α+1;α+1,α+2;1),α(12,+),G(α)=3F2(1α,1,2+α;1+α,3+α;1),α(12,+),H(p)=3F2(12p,1,1+2p;32+p,2p+2;1),pN. (1.1)

    These sets emerge naturally from an exact evaluation of certain classes of fractional integrals, as we show in Section 4.

    In order to understand the notation used above and throughout, we present in this section some basic notations, definitions, and intermediate results, which will be useful to justify certain passages in the proofs of this manuscript. Let us now present a set of symbols and notations.

    N, Z, R, and C denote the sets of non-negative integers, integers, real numbers, and complex numbers, respectively,

    X denotes any set X{0},

    Z0 denotes set N={,n,,1,0},

    B(0,1)={zC||z|<1},

    ¯B(0,1)={zC||z|1},

    R(z) denotes the real part of z.

    Now we present some basic notations, definitions, and intermediate results related to the so-called the Gauss hypergeometric function.

    Definition 2.1. [30] The Euler gamma function Γ(z) is defined by

    Γ(z)=0tz1etdt,  zC|R(z)>0. (2.1)

    Using integration by parts, one sees that

    Γ(z+1)=zΓ(z),  R(z)>0. (2.2)

    The extension of the Euler gamma function to the half-plane R(z)0 is given by

    Γ(z)=Γ(z+k)(z)k,   (R(z)>k;  kN;zZ0),

    where (z)k is the Pochhammer symbol defined for all zC and kN by

    (z)0=1  and  (z)k=z(z+1)(z+k1),  kN. (2.3)

    Relations (2.2) and (2.3) give

    Γ(k+1)=(1)k=k!,  kN. (2.4)

    Definition 2.2. [30] The Gauss hypergeometric function 2F1(a,b;c;z) is defined in the unit disk as the sum of the hypergeometric series as follows:

    2F1(a,b;c;z)=k=0(a)k(b)k(c)kzkk!,(a,bC;cCZ0;z¯B;R(cba)>0). (2.5)

    Furthermore, if 0<R(b)<R(c) and |arg(1z)|<π, then 2F1(a,b;c;z) is given by the following Euler integral representation:

    2F1(a,b;c;z)=Γ(c)Γ(b)Γ(cb)10xb1(1x)cb1(1zx)adx. (2.6)

    If z=1 with R(cba)>0, the Gauss hypergeometric function has the following property:

    2F1(a,b;c;1)=Γ(c)Γ(cab)Γ(ca)Γ(cb). (2.7)

    A natural extension of 2F1 to 3F2 is defined by

    3F2(a,b,c;d,e;z)=+k=0(a)k(b)k(c)k(d)k(e)kzkk!,
    (z¯BandR(d+eabc)>0).

    In [31] Theorem 38, Rainville proves a general integral representation for p+kFq+k, but here we state the following three special cases,

    Case 1: Let p=2, q=k=1, and choose a=1α, b=1, c=α+1, d=α+1, e=α+2, and z=1. Then, 3F2 is given by the following integral representation:

    3F2(1α,1,α+1;α+1,α+2;1)=(α+1)10xα2F1(1α,1;α+1;x)dx. (2.8)

    Case 2: Let p=2, q=k=1, and choose a=1α, b=1, c=α+2, d=α+1, e=α+3, and z=1. Then, 3F2 is given by the following integral representation:

    3F2(1α,1,α+2;α+1,α+3;1)=(α+2)10xα+12F1(1α,1;α+1;x)dx. (2.9)

    Case 3: Let p=2, q=k=1, and choose a=1α, b=1, c=2α, d=α+1, e=2α+1, and z=1. Then, 3F2 is given by the following integral representation:

    3F2(1α,1,2α;α+1,2α+1;1)=2α10x2α12F1(1α,1;α+1;x)dx. (2.10)

    The following is the definition of the Riemann-Liouville fractional integral Iαf of order α.

    Definition 2.3. [30] Let Ω=[τ,η]. The Riemann-Liouville fractional integral Iαf of order αC (R(α)>0) is defined by

    Iαf(t)=1Γ(α)tτ(ts)α1f(s)ds,t>τandR(α)>0. (2.11)

    In this section, we establish some results which will play an important role herein. We believe that some of these results may be new.

    To justify the interchangeability between the integral and the sum, or to rewrite certain integrals, we give the following two lemmas that we will refer to several times in our work.

    Lemma 2.1. Let a,b,cC, cZ0, and R(cab)>0. Then, the series

    k=0(a)k(b)k(c)kzk,

    is normally convergent on the interval [1,1].

    Proof of Lemma 2.1. Since a,b,cC, cZ0, and R(cab)>0, the Gauss hypergeometric function

    2F1(a,b;c;z)=k=0(a)k(b)k(c)kzkk!, (2.12)

    is defined for any complex number z¯B(0,1). Moreover, the series (2.12) is absolutely convergent for all z=1. Therefore, the series uk is convergent, where uk is defined by

    uk=|(a)k(b)k(c)k|,kN.

    Furthermore, it is clear that for all z[1,1],kN, we have

    |(a)k(b)k(c)kzk|uk. (2.13)

    The convergence of the series uk together with the relation (2.13) leads to the normal (therefore uniform) convergence of the series (a)k(b)k(c)kzk on the interval [1,1]. The proof is complete.

    Lemma 2.2. Let Ω=[τ,η] (<τ<η<) be a finite interval on the real axis R, and α>1/2. Then,

    ητ+k=0(1α)k(α+1)k(tτητ)kdt=+k=0(1α)k(α+1)kητ(tτητ)kdt. (2.14)

    Proof of Lemma 2.2. If we take a=1α, b=1, and c=α+1, then cZ0 and R(cab)=2α1>0, since α>1/2. Then by Lemma 2.1, the series (a)k(b)k(c)kzk converges normally on the interval [0,1][1,1]. Consequently, for all α>1/2, we have

    10+k=0(1α)k(α+1)kzkdz=+k=0(1α)k(α+1)k10zkdz. (2.15)

    By using the change of variable with z=tτητ, for relation (2.15) we have

    1(ητ)ητ+k=0(1α)k(α+1)k(tτητ)kdt=+k=0(1α)k(α+1)k1(ητ)ητ(tτητ)kdt. (2.16)

    Thus, we have obtained (2.14). The proof is complete.

    We now establish some results, which we believe are new. These results give the limit of some series.

    The following lemma gives the sum of the series Sα,0 defined by the left-hand side of relation (2.17).

    Lemma 2.3. For all α>1/2, we have

    Sα,0=+k=0(1α)k(α+1)k(k+α+1)=12α. (2.17)

    Proof of Lemma 2.3. For all kN, let uk be the general term of the series Sα,0 given by the relation (2.17). If we take a=1α, b=1, and c=α+1, then cZ0 and R(cab)=2α1>0, since α>1/2. Then, by Lemma 2.1 the series (1α)k(α+1)k is absolutely convergent, and since 0<uk(1α)k(α+1)k for all kN, we then deduce that the series Sα,0 is absolutely convergent. Thus, multiplying and dividing the term uk by (0α), we obtain

    Sα,0=+k=0(0α)(1α)k(0α)(α+1)k(k+α+1)=+k=0(α)k+1α(α+1)k+1=1α[+k=1(α)k(α+1)k]=1α[+k=0(α)k(α+1)k1]=1α[12F1(α,1;α+1;1)]. (2.18)

    From the property of 2F1, given by (2.7) we have

    2F1(α,1;α+1;1)=12, (2.19)

    and so substituting (2.19) into (2.18), we obtain (2.17). This completes the proof.

    The following lemma gives the sum of the series Sα,1 defined by the left-hand side of relation (2.20).

    Lemma 2.4. For all α>1/2, we have

    Sα,1=+k=0(1α)k(α+1)k(α+2+k)=1α+1+12α22α+1. (2.20)

    Proof of Lemma 2.4. The proof is similar to the proof of Lemma 2.3. If we take a=1α, b=1, and c=α+1, then cZ0 and R(cab)=2α1>0, since α>1/2. We deduce that the series Sα,1 is absolutely convergent. Thus, multiplying and dividing the term uk by the same quantity (k+α+1), we obtain

    uk=(1α)k(k+α+1)(α+1)k(α+1+k)(α+1+k+1)=(1α)k(1α+k+2α)(α+1)k+2=(1α)k+1(α+1)k+2+2α(1α)k(α+1)k+2. (2.21)

    Applying the identity (a)k+1=a(1+a)k to α+1, we obtain the following two relations:

    (α+1)k+2=(α+1)(α+2)k+1,(α+1)k+2=(α+1)(α+2)(α+3)k, (2.22)

    and using the above relations and the fact that (a)0=1, the series Sα,1 can be rewritten as follows:

    Sα,1=1α+1+k=0(1α)k+1(α+2)k+1+2α(α+1)(α+2)+k=0(1α)k(α+3)k=1α+1+k=1(1α)k(α+2)k+2α(α+1)(α+2)+k=0(1α)k(α+3)k=1α+1[+k=0(1α)k(α+2)k1]+2α(α+1)(α+2)+k=0(1α)k(α+3)k=1α+1[2F1(1α,1;α+2;1)1]+2α(α+1)(α+2)2F1(1α,1;α+3;1).

    From the property of 2F1 given by (2.7), we have

    2F1(1α,1;α+2;1)=α+12α, (2.23)

    and

    2F1(1α,1;α+3;1)=α+22α+1. (2.24)

    Thus, we obtain

    Sα,1=1α+1[α+12α1]+2α(α+1)(α+2)α+22α+1=1α+1+12α2(2α+1). (2.25)

    The proof is complete.

    The following lemma gives the limit of the series Sα,2 defined by the left-hand side of relation (2.26).

    Lemma 2.5. For all α>1/2, we have

    Sα,2=+k=0(1α)k(α+1)k(k+2α)=12α3F2(1α,1,2α;α+1,2α+1;1). (2.26)

    Proof of Lemma 2.5. If a=1α, b=1, and c=α+1, then cZ0, and R(cab)=2α1>0, since α>1/2. Then, expressing the rightside of (2.10) as a series and changing the order of integration and summation which is justified by Lemma 2.1 (due to the uniform convergence of the series) gives

    2α10x2α12F1(1α,1;α+1;x)dx=2α+k=0(1α)k(1)k(α+1)k10x2α1xkk!dx=2α+k=0(1α)k(α+1)k1(k+2α).

    Thus, we obtained (2.26). The proof is complete.

    The following lemma gives the sum of the series Sα,3 defined by the left-hand side of relation (2.27).

    Corollary 2.1. For all α>1, we have

    Sα,3=+k=0(2α)k(α+1)k(2α+k)=α(1α)(2α1)+[13α2α(1α)]3F2(1α,1,2α;α+1,2α+1;1). (2.27)

    Proof of Corollary 2.1. The proof is similar to the proof of Lemma 2.4, and so we just sketch the basic idea. If we take a=2α, b=1, and c=α+1, then cZ0 and R(cab)=2α2>0, since α>1. Then, by Lemma 2.1 we deduce that the series Sα,3 is absolutely convergent. Thus, multiplying and dividing the term uk by the same quantity (1α), we obtain

    Sα,3=+k=0(2α)k(α+1)k(2α+k)=+k=0(1α)(2α)k(α+1)k(1α)(2α+k)=+k=0(1α)k+1(1α)(α+1)k(2α+k)=11α[+k=0(1α)k(k+1α)(α+1)k(2α+k)]=11α[+k=0(1α)k(k+2α+13α)(α+1)k(2α+k)]=11α[+k=0(1α)k(α+1)k+(13α)+k=0(1α)k(α+1)k(2α+k)]=11α[2F1(1α,1;α+1;1)+(13α)+k=0(1α)k(α+1)k(2α+k)].

    Above we use the property of 2F1 (2.7) and the result of Lemma 2.5 to obtain (2.27). The proof is complete.

    In the following corollary, we give the calculation of 3F2(1,1,4;3,5;1), which we believe may be new.

    Corollary 2.1.

    3F2(1,1,4;3,5;1)=1115. (2.28)

    Proof of Corollary 2.1. Note that when α=2, the numerical series introduced in Lemmas 2.4 and 2.5 coincide. Therefore, the right-hand terms of relations (2.20) and (2.26) are equal when α=2. Thus,

    3F2(1,1,4;3,5;1)=4(13+1425)=7385=1115. (2.29)

    The proof is complete.

    This section explores specific subfamilies of 3F2(1) and is structured into two subsections. The first subsection presents the explicit forms of the subfamilies {3F2(1α,1,α+1;α+1,α+2;1)} and {3F2(1α,1,α+2;α+1,α+3;1)} for all α>12, while the second subsection provides the explicit form of the subfamily {3F2(12p,1,1+2p;32+p,2p+2;1)} for all pN.

    This part aims to find the explicit form of the function K(α)=:3F2(1α,1,α+1;α+1,α+2;1) (Theorem 3.1). To do this, we write K in the form of a series of functions (Lemma 3.1), and then we use the result of Lemma 2.3 to prove our main result of this section, Theorem 3.1.

    In the following lemma, we express the function K(α) as a series.

    Lemma 3.1. For all α>1/2, we have

    3F2(1α,1,α+1;α+1,α+2;1)=(α+1)+k=0(1α)k(α+1)k(k+α+1). (3.1)

    Proof of Lemma 3.1. If a=1α, b=1, and c=α+1, then cZ0 and R(cab)=2α1>0, since α>1/2. Then, expressing the rightside of (2.8) as a series, changing the order of integration and summation, which is justified by Lemma 2.1, and applying the steps of the proof of Lemma 2.5, we can readily derive the proof of Lemma 3.1.

    Now we state and prove our main result of this section, Theorem 3.1.

    Theorem 3.1. For all α>1/2, we have

    3F2(1α,1,α+1;α+1,α+2;1)=α+12α. (3.2)

    Proof of Theorem 3.1. By identifying relations (2.17) and (3.1), we obtain

    3F2(1α,1,α+2;α+1,α+3;1)=(α+1)(12α)=α+12α.

    The proof is complete.

    This part aims to find the explicit form of the function G(α)=:3F2(1α,1,α+2;α+1,α+3;1) (Theorem 3.2). To do this, we write G in the form of a series of functions (Lemma 3.2), then we use the result of Lemma 2.4 to prove our main result of this section, Theorem 3.2. Our argument in this section is similar to the previous section.

    In the following lemma, we express the function G(α) as a series.

    Lemma 3.2. For all α>1/2, we have

    3F2(1α,1,α+2;α+1,α+3;1)=(α+2)+k=0(1α)k(α+1)k(k+α+2). (3.3)

    Proof of Lemma 3.2. If a=1α, b=1, and c=α+1, then cZ0 and R(cab)=2α1>0, since α>1/2. Then, expressing the rightside of (2.9) as a series, changing the order of integration and summation, which is justified by Lemma 2.1, and applying the steps of the proof of Lemma 2.5, we can readily derive the proof of Lemma 3.2.

    Now we state and prove our main result of this section, Theorem 3.2.

    Theorem 3.2. For all α>1/2, we have

    3F2(1α,1,α+2;α+1,α+3;1)=12+1α+1α+132α+1. (3.4)

    Proof of Theorem 3.2. By identifying relations (2.20) and (3.3), we obtain

    3F2(1α,1,α+2;α+1,α+3;1)=(α+2)(1α+1+12α22α+1)=12+1α+1α+132α+1.

    The proof is complete.

    This section deals with the family of functions F(α)=3F2(1α,1,2α;α+1,2α+1;1). It is easy to find a representation for it by a series of functions +k=0fk(α) (see Lemma 2.5). However, it is not obvious to find an explicit one unless αN or a rational number of the form α=2p+12 and pN. Note that when α=pN, then +k=0fk(α) is equal to p1k=0fk(α). Therefore, this case will be excluded from this study. In summary, this part aims to determine the explicit form of F(α) when α=2p+12, which coincides with 3F2(12p,1,1+2p;32+p,2p+2;1) and which we will designate by H(p). To do this, we first calculate H(1) in Section 3.3.1 to make the calculation of H(p) easy to follow in Section 3.3.2.

    The main result of this section is summarized in the following theorem. The proof of this theorem is postponed to the end of this section.

    Theorem 3.3. For all pN, we have

    3F2(12p,1,1+2p;32+p,2p+2;1)=(2p+1)Kp(2a2p+1ln(2)+2a2p+1(Ep+Bp)+2pj=1ajBj),

    where

    Kp=(12p)(32p)(52p)(1+2p)(1+2p)a2p+1=22p(2p)!(3p)!(6p+1)!(p)!Ep=2pk=112kBj=j1k=012k2p+1,j=1,,2paj=2(1)j(2)2p(j)!(2pj)!(6p2j+1),j=1,,2p. (3.5)

    This part aims to find the explicit form of the function H(1). To do this, we write H(1) in the form of a numerical series. Then, we determine the limit of this series.

    In Lemma 3.3, we give the exact value of 3F2(12,1,3;52,4;1).

    Lemma 3.3.

    3F2(12,1,3;52,4;1)=3335635ln(2). (3.6)

    Proof of Lemma 3.3. For p=1 (i.e., α=32), after simplifications, relation (2.26) gives

    3+k=01(2k1)(2k+1)(2k+3)(k+3)=133F2(12,1,3;52,4;1), (3.7)

    that is, 3F2(12,1,3;52,4;1)=9S, where

    S=+k=01(2k1)(2k+1)(2k+3)(k+3). (3.8)

    The decomposition into partial fractions of the general term uk, of the series S=uk, gives

    uk=1(2k1)(2k+1)(2k+3)(k+3)=128(2k1)110(2k+1)+112(2k+3)1105(k+3). (3.9)

    Let n be a fixed positive integer. Then, (Sn)n0 and (Tn)n1 are sequences defined by

    Sn=nk=01(2k1)(2k+1)(2k+3)(k+3)Tn=nk=112k1. (3.10)

    We will simplify the partial sum Sn in order to find its limit when n tends to infinity. To do this, we will express the partial sums,

    Un=nk=012k1;Vn=nk=012k+1;Wn=nk=012k+3,

    as a function of Tn. It is easy to check the following equalities:

    Un=1+TnVn=Tn+12n+1Wn=1+Tn+12n+1+12n+3. (3.11)

    We then deduce Sn as a function of Tn:

    Sn=Un28Vn10+Wn121105nk=01k+3=542+An+Bn, (3.12)

    where

    An=2105Tn1105nk=01k+3Bn=160(2n+1)+112(2n+3). (3.13)

    Furthermore, we have

    nk=01k+3=2nk=012(k+3)=2n+3k=312k=2(1214+nk=112k+12(n+1)+12(n+2)+12(n+3))=2(34+nk=112k+12(n+1)+12(n+2)+12(n+3))=2(34+nk=112k+Cn), (3.14)

    where

    Cn=12(n+1)+12(n+2)+12(n+3).

    Consequently,

    An=2105Tn2105(34+nk=112k+Cn)=2105(nk=112k1nk=112k+34Cn)=2105(nk=1(1)k+1k+34Cn)=2105(Dn+34Cn), (3.15)

    where

    Dn=nk=1(1)k+1k.

    Based on relations (3.12) and (3.15), we obtain

    Sn=542+2105(Dn+34Cn)+Bn=11105+2105(DnCn)+Bn. (3.16)

    Furthermore, we know that for all real numbers x1 such that |x|1, we have

    limn+nk=0(1)k+1kxk=ln(1+x). (3.17)

    Consequently,

    limn+Dn=ln(2). (3.18)

    Moreover, it is easy to verify that

    limn+Bn=0,limn+Cn=0. (3.19)

    Finally, we have

    limn+Sn=11105+2105ln(2). (3.20)

    By grouping relations (3.7) and (3.20), we deduce that

    3F2(12,1,3;52,4;1)=9(11105+2105ln(2))=3335635ln(2). (3.21)

    The proof is complete.

    This section explores specific subfamilies of 3F2(1) and is structured into two subsections. The first subsection presents the explicit forms of the subfamilies F(1) and F(2), while the second subsection provides the explicit form of the subfamily F(3). This part aims to find the explicit form of the function H(p), pN. To do this, we will follow the same approach as that used in Section 3.3.1 to calculate H(1).

    In Lemma 3.5, we give the explicit expression of (1α)k1+α when α=2p+12.

    Lemma 3.4. For all pN,kN, we have

    (12p+12)k(1+2p+12)k=(12p)(12p+1))(1+2p)(1+2p)(2k+12p)(2k+32p)(2k1+2p)(2k+1+2p). (3.22)

    Proof of Lemma 3.5. If α=2p+12, then we have

    (1α)k=(12p)(32p)(52p)(k32p)(k12p),(α+1)k=(32+p)(52+p)(k12+p)(k+12+p). (3.23)

    Note that when k2p+2, there are j=k2p1 terms in common between (1α)k and (α+1)k. Indeed, we observe the first number in common if k12p=32+p, that is k=2p+2. Therefore, if k=2p+3, then there are two terms in common, and so on. Thus, if k2p+2, then (1α)k and (1+α)k are written as follows:

    (1α)k=(12p)(12p+2p)(32+p)(k12p),(α+1)k=(32+p)(52+p)(kp12)(kp+12)(k+12+p). (3.24)

    Therefore, their quotient can be simplified as follows:

    (1α)k(α+1)k=(12p)(12+1p)(12+2pp)(kp+12)(kp+1+12)(kp+2p+12)=(12(p0))(12(p1))(12(p2p))(k+12(p0))(k+12(p1))(k+12(p2p))=22p+1(12(p0))(12(p1))(12(p2p))22p+1(2k+12(p0))(2k+12(p1))(2k+12(p2p))=(12p)(12p+2))(1+2p)(1+2p)(2k+12p)(2k+32p)(2k1+2p)(2k+1+2p)=(12p)(32p))(1+2p)(1+2p)(2k+12p)(2k+32p)(2k1+2p)(2k+1+2p). (3.25)

    When k2p+1, we will show that the quotient (1α)k(α+1)k can be reduced to the form given by the last line of relation (3.25).

    When k=0, we have

    (1α)0(α+1)0=11=(12p)(32p)(1+2p)(1+2p)(12p)(32p))(1+2p)(1+2p)=(12p)(32p)(1+2p)(1+2p)(2×0+12p)(2×0+32p))(2×01+2p)(2×0+1+2p). (3.26)

    When k=1, we have

    (1α)1(α+1)1=12p(3+2p)=(12p)[(32p)(1+2p)(1+2p)][(32p)(1+2p)(1+2p)](3+2p)=(12p)(32p)(1+2p)(1+2p)(2×1+12p)(2×1+32p)(2×11+2p)(2×1+1+2p). (3.27)

    More generally, when k is an integer such that 0k2p+1, we have

    (1α)k(α+1)k=(12p)(32p)(2k32p)(2k12p)(3+2p)(5+2p)(2k1+2p)(2k+1+2p)=(12p)(32p)(2k12p)[(2k+12p)(1+2p)][(2k+12p)(1+2p)](3+2p)(5+2p)(2k+1+2p)=(12p)(32p)(1+2p)(1+2p)(2k+12p)(1+2p)(3+2p)(5+2p)(2k+1+2p). (3.28)

    Thus, we have shown that (1α)k(α+1)k is written in the form (3.22) for all kN. The proof is complete.

    Remark 3.1. For α=2p+12, we deduce from Lemma 3.5 that

    (1α)k(α+1)k(k+2p+1)=Kpuk, (3.29)

    where

    Kp=(12p)(32p)(1+2p)(1+2p)uk=1(2k+12p)(2k+32p)(2k+1+2p)(k+2p+1). (3.30)

    From the above remark, the decomposition into partial fractions of uk gives

    uk=a02k+12p+a12k+32p++a2p2k+1+2p+a2p+1k+2p+1=a02k+12(p0)+a12k+12(p1)++a2p2k+12(p2p)+a2p+1k+2p+1=2pi=0ai2k+12(pi)+a2p+1k+2p+1. (3.31)

    For all i=0,,2p, to find ai, simply multiply uk by (2k+12(pi)), Then, evaluate the resulting expression at k=2(pi)12. For now, let us calculate only the first three coefficients a0,a1, and a2.

    For a0, we evaluate the resulting expression at k=2p12 (i.e., 2k=2p1), so we obtain

    1a0=(2p1+12(p1))(2p1+12(p2p)12(2p1+4p+2)=(2×1)(2×2)(2×2p)12(6p+1),=22p(2p)!12(6p+1)=12(1)0(0!)22p(2p0)!(6p2×0+1). (3.32)

    Consequently,

    a0=2(1)0(0!)22p(2p0)!(6p2×0+1). (3.33)

    For a1, we evaluate the resulting expression at k=2p32 (i.e., 2k=2p3), so we obtain

    1a1=(2p3+12(p0))(2p3+12(p2p))12(2p3+4p+2)=(2)(2×1)(2×3)(2×(2p1))12(6p1)=(1)12122p1(2p1)!12(6p1)=12(1)1(1!)(2)2p(2p1)!(6p2×1+1). (3.34)

    Consequently,

    a1=2(1)1(1!)(2)2p(2p1)!(6p2×1+1). (3.35)

    For a2, we evaluate the resulting expression at k=2p52 (i.e., 2k=2p5), so we obtain

    1a2=(2p5+12(p0))(2p5+12(p2p))12(2p5+4p+2)=(22)(21)(2×1)(2×3)(2×(2p2))12(6p3)=(1)222(2!)22p2(2p2)!12(6p3)=12(1)2(2!)(2)2p(2p2)!(6p2×2+1). (3.36)

    Consequently,

    a2=2(1)2(2)2p(2p2)!(6p2×2+1). (3.37)

    The calculation of the first three coefficients a0,a1,a2 allowed us to guess the general expression of ai for all i=0,,2p, which is stated in the following Lemma 3.5.

    Lemma 3.5. Let pN. Then, for all i=0,,2p, we have

    ai=2(1)i(2)2p(i)!(2pi)!(6p2i+1). (3.38)

    Proof of Lemma 3.5. We will confirm this expression by a direct calculation of ai. To do this, we evaluate the resulting expression at k=2p(2i+1)2 (i.e., 2k=2p(2i+1)), so we obtain

    1ai=(2p(2i+1)+12(p0))(2p(2i+1)+12(p1))(2p(2i+1)+12(p(i1)))(2p(2i+1)+12(p(i+1)))(2p(2i+1)+12(p2p))12(2p(2i+1)+4p+2)=(2(i0))(2(i1))(2(i(i1)))(2×1)(2×2)(2(2pi))12(6p2i+1)=12(2)i(i)!22pi(2pi)!(6p2i+1)=12(1)i(2)i(i)!22pi(2pi)!(6p2i+1)=12(1)i(2)2p(i)!(2pi)!(6p2i+1). (3.39)

    Thus, we find the expression of ai stated in relation (3.38). The proof is then complete.

    All that remains is to determine the expression of a2p+1. This will be the subject of Lemma 3.6.

    Lemma 3.6. The last coefficient of the decomposition into partial fractions (3.31) is given by

    a2p+1=22p(2p)!(3p)!(6p+1)!(p)!. (3.40)

    Proof of Lemma 3.6. To find a2p+1, multiply uk by (k+2p+1). Then, evaluate the resulting expression at k=2p1 (i.e., 2k=4p2). We then obtain

    1a2p+1=(4p22p+1)(4p22p+3)(4p2+2p1)(4p2+2p+1)=(6p1)(6p+1)(6p+3)(2p3)(2p1)=(6p1)(6p)(6p+1)(6p+2)(6p+3)(2p3)(2p2)(2p1)(6p)(6p+2)(2p4)(2p2)=(1)2p+1(6p+1)(6p)(6p1)(6p2)(6p3)(2p+3)(2p+2)(2p+1)(1)2p(6p)(6p2)(2p+4)(2p+2)=(2p+1)(2p+2)(6p+1)2(p+1)2(p+2)2(3p)=[1×2××2p](2p+1)(2p+2)(6p+1)[1×2××p][1×2××2p]23p(p+1)+1[1×2××p](p+1)(p+2)(3p)=(6p+1)!(p)!22p(2p)!(3p)!. (3.41)

    The proof is complete.

    The following remark shows the validation of formulas (3.38) and (3.40) when p=1.

    Remark 3.2. For p=1, we will check the concordance of the coefficients a0,,a3 given by relations (3.40) and (3.38) with those presented in relation (3.9). When p=1, relations (3.38) and (3.40) give

    a0=2(1)0(2)2(0)!(2)!(7)=128a1=2(1)1(2)2(1)!(1)!(5)=110a2=2(1)2(2)2(2)!(0)!(3)=112a3=22(2)!(3)!(7)!(1)!=1105. (3.42)

    Thus, we find the same coefficients of the decomposition into partial fractions of uk given by (3.9).

    Lemma 3.7 presents a relation between the coefficient a2p+1 and the coefficients (ai)0i2p.

    Lemma 3.7. For all pN, we have

    2pi=0ai=2a2p+1. (3.43)

    Proof of Lemma 3.7. We have shown in relation (3.31) that, for all k>0, the term uk is written as a partial fraction (3.31), where (ai)0i2p and a2p+1 are given by (3.38) and (3.40).

    By reducing all the partial fractions to the same denominator and identifying the numerators, we then obtain 2p+2 equations with unknowns a0, , a2p, a2p+1. It is easy to see that the equation that relates the coefficients of the monomial k2p+1 is written in the following form 2pi=0k(2k)2pai+(2k)2p+1a2p+1=0, or in the equivalent form

    2pi=0ai=2a2p+1. (3.44)

    The proof is complete.

    In the following Lemma 3.8, we establish a supporting result that arises from the calculations performed in the previous results of this section. This result provides an explicit form of a finite sum.

    Lemma 3.8. For all pN, we have

    2pi=0(1)i(2)2p(i)!(2pi)!(6p2i+1)=22p(2p)!(3p)!(6p+1)!(p)!. (3.45)

    Proof of Lemma 3.8. Based on formula (3.43), we have

    2pi=0ai=2a2p+1. (3.46)

    By replacing in the previous equality the coefficients (ai)0i2p+1 by their expressions presented in relations (3.38) and (3.40), we directly obtain relation (3.45). The proof is complete.

    In the following section, we will prove that the series uk converges and we calculate its sum, where uk is defined by (3.30).

    Convergence of the series uk

    Let n be a fixed positive integer, and (Sn)n0 and (Tn)n1 be the sequences defined by

    Sn=nk=0uk,Tn=nk=012k2p+1. (3.47)

    We will write Sn as a function of Tn, prove that the sequence Sn converges, and determine its limit.

    For all j=1,,2p, we have

    nk=012k2(pj)+1=nk=012(k+j)2p+1=n+jk=j12k2p+1=nk=012k2p+1+n+jk=n+112k2p+1j1k=012k2p+1=Tn+Aj,nBj, (3.48)

    where

    Aj,n=n+jk=n+112k2p+1,Bj=j1k=012k2p+1. (3.49)

    Note that for j=0, we also have

    nk=012k2(p0)+1=nk=012k2p+1=Tn+A0,nB0, (3.50)

    where

    A0,n=B0=0. (3.51)

    Furthermore, we also have

    nk=01k+2p+1=2nk=012(k+2p+1)=2n+2p+1k=2p+112k=2nk=112k+2n+2p+1k=n+112k22pk=112k=2nk=112k+2Dn2Ep, (3.52)

    where

    Dn=n+2p+1k=n+112k,Ep=2pk=112k. (3.53)

    Moreover, we have

    Tn=nk=012k2p+1=p1k=012k2p+1+n+pk=p12k2p+1=p1k=012k2p+1+nk=012k+1=Bp+nk=012k+1, (3.54)

    where

    Bp=p1k=012k2p+1. (3.55)

    After writing Sn as a function of Tn, we will inject the expression of Tn given by (3.54) into Sn to prove that Sn converges and deduce its limit.

    Using relations (3.48), (3.54) (3.52), and (3.43), the partial sum Sn equals

    Sn=2pj=0ajnk=012k2(pj)+1+a2p+1nk=01k+2p+1=2pj=0aj(Tn+Aj,nBj)+a2p+1(2nk=112k+2Dn2Ep)=Tn2pj=0aj+2a2p+1nk=112k+2pj=1aj(Aj,nBj)+2a2p+1(DnEp)=2a2p+1Tn+2a2p+1nk=112k+2pj=1ajAj,n2pj=1ajBj+2a2p+1Dn2a2p+1Ep=2a2p+1nk=012k+12a2p+1Bp+2a2p+1nk=112k+2pj=1ajAj,n2pj=1ajBj+2a2p+1Dn2a2p+1Ep=2a2p+1(nk=012k+1nk=112k)2a2p+1Ep2pj=1ajBj2a2p+1Bp+2pj=1ajAj,n+2a2p+1Dn=2a2p+1nk=1(1)k+1k2a2p+1Ep2pj=1ajBj2a2p+1Bp+2pj=1ajAj,n+2a2p+1Dn. (3.56)

    Since

    limn+nk=1(1)k+1k=ln(2)limn+Aj,n=0,j=1,,2plimn+Dn=0, (3.57)

    we deduce that Sn converges, and that its limit verifies

    limn+Sn=2a2p+1ln(2)2a2p+1(Ep+Bp)2pj=1ajBj. (3.58)

    The following Lemma 3.9 gives the sum of the series uk.

    Lemma 3.9. For all pN, we have

    +k=0(12p)k(12+p)k(k+2p+1)=Kp(2a2p+1ln(2)+2a2p+1(Ep+Bp)+2pj=1ajBj), (3.59)

    where Kp, a2p+1, Ep, Bj, and aj are defined in (3.5).

    Proof of Lemma 3.9. By grouping relations (3.29), (3.47), and (3.58), we obtain

    +k=0(12p)k(12+p)k(k+2p+1)=Kplimn+Sn=Kp(2a2p+1ln(2)+2a2p+1(Ep+Bp)+2pj=1ajBj). (3.60)

    The proof is complete.

    The following remark gives the validation of formula (3.59) when p=1.

    Remark 3.3. For p=1, we will check the concordance of the limit given by relation (3.20) with that presented in relation (3.58). When p=1, we easily obtain E1=34, B1=1, and B2=0. Moreover, the values of (ai)0i3 are given in (3.42). Thus, relation (3.58) gives

    limn+Sn=2(1105)ln(2)2(1105)(341)[110(1)+112(0)]=2105ln(2)+1105(322)110=2105ln(2)121021210=2105ln(2)22210=2105ln(2)11105. (3.61)

    Thus, we find the same limit as that found in relation (3.20).

    With the intermediate results from Section 3.3 now found, we can prove Theorem 3.3 stated at the beginning of this section.

    Proof of Theorem 3.3. Based on relation (2.26) and taking α=2p+12, we obtain

    +k=0(12p)k(12+p)k(k+2p+1)=3F2(1α,1,2α;α+1,2α+1;1)2α=3F2(12p,1,1+2p;32+p,2p+2;1)2p+1. (3.62)

    By identifying the right-hand sides of relations (3.59) and (3.62), we obtain

    Kp(2a2p+1ln(2)+2a2p+1(Ep+Bp)+2pj=1ajBj)=3F2(12p,1,1+2p;32+p,2p+2;1)2p+1,

    that is,

    (2p+1)Kp(2a2p+1ln(2)+2a2p+1(Ep+Bp)+2pj=1ajBj)=3F2(12p,1,1+2p;32+p,2p+2;1).

    The proof is complete.

    We now state and prove the following two results of Theorem 3.3 corresponding to the special cases p=2 and p=3.

    For p=2, Theorem 3.3 yields the first new special result.

    Corollary 3.1.

    3F2(32,1,5;72,6;1)=40456006+101001ln(2). (3.63)

    Proof of corollary 3.1. Let p=2. Then, from Theorem 3.3, we easily compute the following quantities:

    K2=45, E2=2524, B1=13, B2=43, B3=13, B4=0, a1=1528,a2=1288, a3=1336, a4=1960, a5=145045, 4j=1ajBj=258316.

    Thus, to derive relation (3.63), we simply substitute the values above into Theorem 3.3. The proof is complete.

    Also, for p=3, Theorem 3.3 yields the second new special result.

    Corollary 3.2.

    3F2(52,1,7;92,8;1)=22115841570170138567ln(2). (3.64)

    Proof of Corollary 3.2. The proof follows similar lines of argument to that of Corollary 3.1. Let p=3. Then, from Theorem 3.3, we easily compute the following quantities:

    B1=15, B2=815, B3=2315, B4=815, B5=315, B6=0,a1=165280, a2=123040, a3=114976, a4=116896, a5=134560,a6=1161280, a7=143648605, K3=1575, E3=4940, 6j=1ajBj=3716563700. (3.65)

    Thus, to derive relation (3.64), we simply substitute the values above into Theorem 3.3. The proof is complete.

    This section is devoted to giving our new evaluation of a certain class of fractional integrals whose values are written in terms of hypergeometric functions 3F2 which we obtained in the previous sections.

    Theorem 4.1. For all τstη, and α>1/2, the following integral representations for the Gauss hypergeometric function hold true.

    (1)

    Iα1(t):=tτ(ts)α1(ηs)α1 ds=[(ητ)α1(tτ)αα]2F1(1α,1;α+1;g(t)), (4.1)

    where g(t):=tτητ.

    (2)

    ητIα1(t)dt=[(ητ)2αα(α+1)]3F2(1α,1,α+1;α+1,α+2;1) (4.2)
    =(ητ)2α2α2. (4.3)

    Proof of Theorem 4.1.

    (1) Let s=τ+x(tτ). By changing the integration variable from s to x, the integral Iα1(t) becomes

    Iα1(t)=(tτ)10((tτ)x(tτ))α1((ητ)x(tτ))α1dx=(tτ)(tτ)α110(1x)α1((ητ)(ητ)(tτ)(ητ)x)α1dx=(ητ)α1(tτ)α10(1x)α1(1(tτ)(ητ)x)α1dx.

    Above, we have the Euler integral representation of 2F1(a,b;c;z) with a=1α, b=1, c=α+1, and z=g(t)=tτητ. Thus,

    Iα1(t)=(ητ)α1(tτ)αα2F1(1α,1;α+1;g(t)).

    This completes the proof of (4.1).

    (2) Now we are in a position to evaluate the integral (4.2), so denoting the left-hand side of (4.2) by λ1, we have

    λ1:=(ητ)α1αητ(tτ)α2F1(1α,1;α+1;g(t))dt. (4.4)

    Now, expressing 2F1 as a series and changing the order of integration and summation, which is justified by Lemma 2.2, we have

    λ1:=[(ητ)α1α]k=0(1α)k(α+1)kητ(tτ)α(tτητ)kdt=[(ητ)α1α]k=0(1α)k(α+1)k(1ητ)kητ(tτ)k+αdt=[(ητ)2αα]k=0(1α)k(α+1)k1(k+α+1).

    Now, by Lemma 3.1, we obtain (4.2), that is

    λ1:=[(ητ)2αα(α+1)]3F2(1α,1,α+1;α+1,α+2;1),

    and Theorem 3.1 gives (4.3). This completes the proof.

    Theorem 4.2. For all τstη and α>1/2, the following integral representations for the Gauss hypergeometric function hold true.

    (1)

    Iα2(t):=tτ(tτ)(ts)α1(ηs)α1 ds=[(ητ)α1(tτ)α+1α]2F1(1α,1;α+1;g(t)), (4.5)

    where g(t):=tτητ.

    (2)

    ητIα2(t)dt=[(ητ)2α+1α(α+2)]3F2(1α,1,α+2;α+1,α+3;1) (4.6)
    =(ητ)2α+1α[1α+1+12α22α+1]. (4.7)

    Proof of Theorem 4.2.

    (1) The proof is similar to the proof of Theorem 4.1, and so we just sketch the basic idea. In exactly the same manner, the integral Iα2(t) can be obtained.

    (2) Now denoting the left-hand side of (4.6) by λ2, we have

    λ2:=(ητ)α1αητ(tτ)α+12F1(1α,1;α+1;g(t))dt. (4.8)

    Now, expressing 2F1 as a series and changing the order of integration and summation, which is justified by Lemma 2.2, we have

    λ2:=[(ητ)α1α]k=0(1α)k(α+1)kητ(tτ)α+1(tτητ)kdt=[(ητ)α1α]k=0(1α)k(α+1)k(1ητ)kητ(tτ)k+α+1dt=[(ητ)2α+1α]k=0(1α)k(α+1)k1(k+α+2).

    Now, by Lemma 3.2, we obtain (4.6), that is

    λ2:=[(ητ)2α+1α(α+2)]3F2(1α,1,α+2;α+1,α+3;1),

    and Theorem 3.2 gives (4.7). This completes the proof.

    Theorem 4.3. For all τstη, and α>1/2, the following integral representations for the Gauss hypergeometric function hold true.

    (1)

    Iα3(t):=tτ(tτ)α1(ts)α1(ηs)α1ds=[(ητ)α1(tτ)2α1α]2F1(1α,1,α+1;g(t)), (4.9)

    where g(t):=tτητ.

    (2)

    ητIα3(t)dt=[(ητ)3α12α2]3F2(1α,1,2α;α+1,2α+1;1). (4.10)

    Proof of Theorem 4.3.

    (1) The proof is similar to the proof of Theorem 4.1, and so we just sketch the basic idea. In exactly the same manner, the integral Iα3(t) can be obtained.

    (2) Now, denoting the left-hand side of (4.10) by λ3, we have

    λ3:=(ητ)α1αητ(tτ)2α12F1(1α,1;α+1;g(t))dt. (4.11)

    By expressing 2F1 as a series and change the order of integration and summation, which is justified by justified by Lemma 2.2, we have

    λ3=[(ητ)α1α]k=0(1α)k(α+1)k(1ητ)kητ(tτ)k+2α1dt=[(ητ)3α1α]k=0(1α)k(α+1)k1(k+2α). (4.12)

    Thus, the result of Lemma 2.5 gives (4.10). This completes the proof.

    Remark 4.1. Note that when α=2, the results of Theorems 4.2 and 4.3 coincide. Therefore, the right-hand terms of relations (4.6) and (4.10) are equal when α=2, which can be justified by Lemma 2.1. Thus,

    ητI22(t)dt=ητI23(t)dt=11(ητ)5120. (4.13)

    For the choices α=2p+12 and pN, we have the following new explicit evaluation of a certain class of integrals as a special case from our Theorem 4.3.

    Theorem 4.4. For all τstη and pN, the following integral holds true.

    (1)

    ητI2p+123(t)dt=[2(ητ)6p+12(2p+1)2]3F2(12p,1,1+2p;32+p,2p+2;1) (4.14)
    =Kp[2(ητ)6p+12(2p+1)](2a2p+1ln(2)+2a2p+1(Ep+Bp)+2pj=1ajBj), (4.15)

    where I2p+123 is defined in (4.9) with α=2p+12, and Kp, a2p+1, Ep, Bj, and aj are defined in (3.5).

    Proof of Theorem 4.4. By letting α=2p+12 and pN in the integral (4.10), we obtain (4.14) and (4.15) is obtained by replacing the explicit evaluation of the fucntion 3F2(12p,1,1+2p;32+p,2p+2;1) given by Theorem 3.3. The proof is complete.

    The following result presents the integrals of Iα3(t) for some α when α=3/2, α=5/2, and α=7/2.

    Corollary 4.1. For all τstη, the following integrals hold true.

    (1)

    ητI3/23(t)dt=[2(ητ)7232](3335635ln(2)), (4.16)

    where I3/23 is defined in (4.9) with α=3/2.

    (2)

    ητI5/23(t)dt=[2(ητ)13252](40456006+101001ln(2)), (4.17)

    where I5/23 is defined in (4.9) with α=5/2.

    (3)

    ητI7/23(t)dt=[2(ητ)19272](22115841570170138567ln(2)), (4.18)

    where I7/23 is defined in (4.9) with α=7/2.

    Proof of corollary 4.1.

    (1) Let p=1. Then, from Theorem 4.4 (4.14), we obtain

    ητI3/23(t)dt=[2(ητ)7232]3F2(12,1,3;52,4;1). (4.19)

    From Lemma 3.3, we have

    3F2(12,1,3;52,4;1)=3335635ln(2), (4.20)

    and so substituting (4.20) into (4.19), we obtain (4.31). This completes the proof of (4.31).

    (2) Similarly, let p=2. Then, from Theorem 4.4 (4.14), we obtain

    ητI5/23(t)dt=[2(ητ)13252]3F2(32,1,5;72,6;1). (4.21)

    From Corollary 3.1, we have

    3F2(32,1,5;72,6;1)=40456006+101001ln(2), (4.22)

    and so substituting (4.22) into (4.21), we obtain (4.32). This completes the proof of (4.32).

    (3) Also, if we let p=2, then from Theorem 4.4 (4.14), we obtain

    ητI7/23(t)dt=[2(ητ)19272]3F2(52,1,7;92,8;1). (4.23)

    From Corollary 3.2, we have

    3F2(52,1,7;92,8;1)=22115841570170138567ln(2), (4.24)

    and so substituting (4.24) into (4.23), we obtain (4.33). This completes the proof.

    Theorem 4.5. For all τstη and α>1, the following integral representations for the Gauss hypergeometric functions hold true.

    (1)

    Iα4(t):=tτ(tτ)α1(ts)α1(ηs)α2ds=[(ητ)α2(tτ)2α1α]2F1(2α,1;α+1;g(t)), (4.25)

    where g(t):=tτητ.

    (2)

    ητIα4(t)dt=(ητ)3α2(1α)(2α1)+[(13α)(ητ)3α22α2(1α)]3F2(1α,1,2α;α+1,2α+1;1). (4.26)

    Proof of Theorem 4.5.

    (1) The proof follows similar lines of argument to that of the above theorems and so we just sketch the basic idea. In exactly the same manner, we have

    Iα4(t)=(ητ)α2(tτ)2α110(1x)α1(1(tτ)(ητ)x)α2dx.

    Above, we have the Euler integral representation of 2F1(a,b;c;z) with a=2α, b=1, c=α+1, and z=g(t)=tτητ, thus

    Iα4(t)=(ητ)α2(tτ)2α1α2F1(2α,1;α+1;g(t)). (4.27)

    This completes the proof of (4.25).

    (2) Now denoting the left-hand side of (4.26) by λ4, we have

    λ4:=(ητ)α2αητ(tτ)2α12F1(2α,1;α+1;g(t))dt, (4.28)

    and by expressing 2F1 as a series and change the order of integration and summation, which is justified by justified by Lemma 2.2, we have

    λ4=[(ητ)α2α]k=0(2α)k(α+1)k(1ητ)kητ(tτ)k+2α1dt=[(ητ)3α2α]k=0(2α)k(α+1)k1(k+2α). (4.29)

    Thus, the result of Lemma 2.1 gives (4.26). This completes the proof.

    For the choices α=2p+12 and pN, we have also the following new explicit evaluation of a certain class of Integrals as special case from our Theorem 4.5.

    Theorem 4.6. For all τstη and pN, the following integral holds true.

    ητI2p+124(t)dt=(ητ)6p12p(12p)+[(6p+1)(ητ)6p12(2p1)(2p+1)2]3F2(12p,1,1+2p;32+p,2p+2;1)=(ητ)6p12p(12p)[Kp(6p+1)(ητ)6p12(2p1)(2p+1)](2a2p+1ln(2)+2a2p+1(Ep+Bp)+2pj=1ajBj), (4.30)

    where I2p+124 is defined in (4.25) with α=2p+12, and Kp, a2p+1, Ep, Bj, and aj are defined in (3.5)

    Proof of Theorem 4.6. The proof is similar to the proof of Theorem 4.4, so we omit the proof for brevity.

    The following result presents the values of Iα4 for some α that are when α=3/2, α=5/2, and α=7/2.

    Corollary 4.2. For all τstη, the following integrals hold true.

    (1)

    ητI3/24(t)dt=(ητ)52+7(ητ)529(3335635ln(2)), (4.31)

    where I3/23 is defined in (4.25) with α=3/2.

    (2)

    ητI5/24(t)dt=(ητ)1126+12(ητ)11275(40456006+101001ln(2)), (4.32)

    where I5/23 is defined in (4.25) with α=5/2.

    (3)

    ητI7/24(t)dt=(ητ)17215+19(ητ)172245(22115841570170138567ln(2)), (4.33)

    where I7/23 is defined in (4.25) with α=7/2.

    Proof of Corollary 4.2. The proof is similar to the proof of Theorem 4.1, so we omit the proof for brevity.

    In this study, we expressed four families of fractional integrals, denoted as Fα1={Iα1(α),Iα2(α);α>12}, Fα2={Iα3(α),;α>12} and Fα3={Iα4(α);α>1}, using the class of hypergeometric functions 3F2(1). The series representation of the hypergeometric functions allowed us to derive explicit forms for the integrals of the family Fα1 for all α>12, as well as for the integrals of the subfamily F2p+122 and F2p+123 for all pN.

    For the integrals of the family Fα2 and Fα3, we have only calculated the explicit forms of those of the subfamily F2p+122 and F2p+123. However, by examining other subfamilies of Fα2 and Fα3, we could derive more interesting formulas relating fractional integrals to the family of functions 3F2(1).

    Saleh S. Almuthaybiri: Conceptualization, supervision, validation, investigation, writing original draft preparation, formal analysis, writing review and editing. Abdelhamid Zaidi: Investigation, validation, writing original draft preparation, methodology, formal analysis, writing review and editing, doing the revision, funding acquisition. All authors have read and agreed to the published version of the manuscript.

    The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    The Researchers would like to thank the Deanship of Graduate Studies and Scientific Research at Qassim University for financial support (QU-APC-2025).

    The authors declare that they have no conflicts of interest.



    [1] E. Özergin, Some properties of hypergeometric functions, Eastern Mediterranean University, 2011. Available from: http://hdl.handle.net/11129/217
    [2] F. Ouimet, Central and noncentral moments of the multivariate hypergeometric distribution, arXiv, 2024. https://doi.org/10.48550/arXiv.2404.09118
    [3] W. Briggs, R. Zaretzki, A new look at inference for the hypergeometric distribution, 2009.
    [4] P. Sheridan, M. Onsjö, The hypergeometric test performs comparably to TF-IDF on standard text analysis tasks, Multimed. Tools Appl., 83 (2024), 28875–28890. https://doi.org/10.1007/s11042-023-16615-z doi: 10.1007/s11042-023-16615-z
    [5] H. Alzer, K. Richards, Combinatorial identities and hypergeometric functions, Rocky Mountain J. Math., 52 (2022), 1921–1928. https://doi.org/10.1216/rmj.2022.52.1921 doi: 10.1216/rmj.2022.52.1921
    [6] H. Gould, Combinatorial identities: A standardized set of tables listing 500 binomial coefficient summations, Morgantown, 1972.
    [7] E. Diekema, Combinatorial identities and hypergeometric series, arXiv, 2022. https://doi.org/10.48550/arXiv.2204.05647
    [8] J. Borwein, A. Straub, C. Vignat, Densities of short uniform random walks in higher dimensions, J. Math. Anal. Appl., 437 (2016), 668–707. https://doi.org/10.1016/j.jmaa.2016.01.017 doi: 10.1016/j.jmaa.2016.01.017
    [9] J. Borwein, D. Nuyens, A. Straub, J. Wan, Random walks in the plane, Discrete Math. Theor. Comput. Sci., 2010,191–202.
    [10] J. McCrorie, Moments in Pearson's four-step uniform random walk problem and other applications of very well-poised generalized hypergeometric series, Sankhya B, 83 (2021), 244–281. https://doi.org/10.1007/s13571-020-00230-1 doi: 10.1007/s13571-020-00230-1
    [11] S. Janson, D. Knuth, T. Łuczak, B. Pittel, The birth of the giant component, Random Struct. Algor., 4 (1993), 233–358. https://doi.org/10.1002/rsa.3240040303 doi: 10.1002/rsa.3240040303
    [12] E. P. Wigner, On the matrices which reduce the Kronecker products of representations of S. R. groups, In: The collected works of eugene paul wigner, Berlin, Heidelberg: Springer, 1993,608–654. https://doi.org/10.1007/978-3-662-02781-3_42
    [13] K. S. Rao, Symmetries of 3n-j coefficients and generalized hypergeometric functions, In: Symmetries in science X, Boston: Springer, 1998,383–399. https://doi.org/10.1007/978-1-4899-1537-5_24
    [14] M. Harmer, Note on the Schwarz triangle functions, Bull. Aust. Math. Soc., 72 (2005), 38–389. https://doi.org/10.1017/S0004972700035218 doi: 10.1017/S0004972700035218
    [15] A. Ali, M. Islam, A. Noreen, Z. Nisa, Solution of fractional k-hypergeometric differential equation, Int. J. Math. Anal., 14 (2020), 125–132. https://doi.org/10.12988/ijma.2020.91287 doi: 10.12988/ijma.2020.91287
    [16] M. Abul-Ez, M. Zayed, A. Youssef, Further study on the conformable fractional Gauss hypergeometric function, AIMS Mathematics, 6 (2021), 10130–10163. https://doi.org/10.3934/math.2021588 doi: 10.3934/math.2021588
    [17] M. Chen, W. Chu, Yabu's formulae for hypergeometric 3F2-series through Whipple's quadratic transformations, AIMS Mathematics, 9 (2024), 21799–21815. https://doi.org/10.3934/math.20241060 doi: 10.3934/math.20241060
    [18] M. Atia, M. Alkilayh, Extension of Chu–Vandermonde identity and quadratic transformation conditions, Axioms, 13 (2024), 825. https://doi.org/10.3390/axioms13120825 doi: 10.3390/axioms13120825
    [19] M. Atia, On the inverse of the linearization coefficients of Bessel polynomials, Symmetry, 16 (2024), 737. https://doi.org/10.3390/sym16060737 doi: 10.3390/sym16060737
    [20] M. Atia, A. Rathie, On a generalization of the Kummer's quadratic transformation and a resolution of an isolated case, Axioms, 12 (2023), 821. https://doi.org/10.3390/axioms12090821 doi: 10.3390/axioms12090821
    [21] M. Atia, A. Al-Mohaimeed, On a resolution of another isolated case of a Kummer's quadratic transformation for 2F1, Axioms, 12 (2023), 221. https://doi.org/10.3390/axioms12020221 doi: 10.3390/axioms12020221
    [22] A. Shehata, S. Moustafa, Some new results for Horn's hypergeometric functions Γ1 and Γ2, J. Math. Comput. Sci., 23 (2020), 26–35. https://doi.org/10.22436/jmcs.023.01.03 doi: 10.22436/jmcs.023.01.03
    [23] W. Mohammed, C. Cesarano, F. Al-Askar, Solutions to the (4+1)-dimensional time-fractional Fokas equation with M-truncated derivative, Mathematics, 11 (2023), 194. https://doi.org/10.3390/math11010194 doi: 10.3390/math11010194
    [24] F. He, A. Bakhet, M. Hidan, H. Abd-Elmageed, On the construction of (p, k)-hypergeometric function and applications, Fractals, 30 (2022), 2240261. https://doi.org/10.1142/S0218348X22402617 doi: 10.1142/S0218348X22402617
    [25] H. Exton, A new two-term relation for the 3F2 hypergeometric function of unit argument, J. Comput. Appl. Math., 106 (1999), 395–397. https://doi.org/10.1016/S0377-0427(99)00077-1 doi: 10.1016/S0377-0427(99)00077-1
    [26] M. Milgram, On hypergeometrics 3F2(1)-A review, arXiv, 2010. https://doi.org/10.48550/arXiv.1011.4546
    [27] Y. Kim, J. Choi, A. Rathie, Two results for the terminating 3F2(2) with applications, Bull. Korean Math. Soc., 49 (2012), 621–633. https://doi.org/10.4134/BKMS.2012.49.3.621 doi: 10.4134/BKMS.2012.49.3.621
    [28] K. Chen, Explicit formulas for some infinite 3F2(1)-series, Axioms, 10 (2021), 125. https://doi.org/10.3390/axioms10020125 doi: 10.3390/axioms10020125
    [29] M. Chen, W. Chu, Bisection series approach for exotic 3F2(1)-series, Mathematics, 12 (2024), 1915. https://doi.org/10.3390/math12121915 doi: 10.3390/math12121915
    [30] A. Kilbas, H. Srivastava, J. Trujillo, Theory and applications of fractional differential equations, Elsevier, 204 (2006).
    [31] E. D. Rainville, Special functions, New York: Macmillan, 1960.
  • Reader Comments
  • © 2025 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(53) PDF downloads(8) Cited by(0)

Other Articles By Authors

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog