This work is licensed under the Creative Commons Attribution 4.0 International License.
Introduction
The classical Pochhammer symbol (λ )ν is given as follows: [1, 4, 14, 23, 26, 34]
\matrix{ {{{\left( \lambda \right)}_\nu }} \hfill & { = {{\Gamma \left( {\lambda + \nu } \right)} \over {\Gamma \left( \lambda \right)}}} \hfill & {\left( {\lambda ,\nu \in \backslash _0^ - } \right)} \hfill \cr {} \hfill & { = \left\{ {\matrix{ 1 \hfill \cr {\lambda \left( {\lambda + 1} \right) \cdots \left( {\lambda + n - 1} \right)} \hfill \cr } } \right.} \hfill & {\matrix{ {\left( {\nu = 0} \right)} \hfill \cr {\left( {\nu = n \in } \right)} \hfill \cr } } \hfill \cr }
and Γ(λ ) is the familiar Gamma function whose Euler’s integral is (see, e.g., [1, 4, 14, 23, 26])
\Gamma \left( z \right) = \int\limits_0^\infty {{e^{ - t}}{t^{z - 1}}dt} \,\,\left( {\Re \left( z \right) > 0} \right).
From (1) and (2), it is easy to see the following integral formula
{\left( \lambda \right)_v} = {1 \over {\Gamma \left( \lambda \right)}}\int\limits_0^\infty {{e^{ - t}}{t^{\lambda + v - 1}}dt} \left( {\Re \left( {\lambda + \nu } \right) > 0} \right).
Throughout this paper, let ℂ, \mathbb{Z}_0^ - , and ℕ be the sets of complex numbers, non-positive integers and positive integers respectively, and assume that min{ℜ(p),ℜ(q),ℜ(κ),ℜ(μ)} > 0. Recently, various generalization of beta functions have been introduced and investigated (see, e.g., [7, 8, 9, 10, 13, 16, 17, 21, 22, 27, 29, 37] and the references cited therein). In [37], Şahin et al. introduced and studied following generalization of the extended gamma function as follows:
\matrix{ {\Gamma _{p,q}^{\left( {\kappa ,\mu } \right)}\left( z \right) = \int_0^\infty {{t^{z - 1}}{\rm{exp}}\left( { - {{{t^\kappa }} \over p} - {q \over {{t^\mu }}}} \right)dt} ,} \cr {\left( {\Re \left( z \right) > 0,\Re \left( p \right) > 0,\Re \left( q \right) > 0,\Re \left( \kappa \right) > 0,\Re \left( \mu \right) > 0} \right).} \cr }
It is easily seen that the special cases of (4) returns to other forms of gamma functions. For example, \Gamma _{1,0}^{\left( {1,1} \right)}\left( z \right) = \Gamma \left( z \right),\Gamma _{1,q}^{\left( {1,1} \right)}\left( z \right) = {\Gamma _q}\left( z \right)..
Using the above (4), Şahin et. al. [38] defined a new generalization of the extended Pochhammer symbol such as;
{\left( {\lambda ;p,q;\kappa ,\mu } \right)_\nu }: = \left\{ {\matrix{ {{{\Gamma _{p,q}^{\left( {\kappa ,\mu } \right)}\left( {\lambda + \nu } \right)} \over {\Gamma \left( \lambda \right)}}} & {,\Re \left( p \right) > 0,\Re \left( q \right) > 0,\Re \left( \kappa \right) > 0,\Re \left( \mu \right) > 0} \cr {{{\left( \lambda \right)}_\nu }} & {,p = 1\,q = 0\,\kappa = 1\,\mu = 0} \cr } } \right.
and, also they obtained integral representation of (5) as follows:
Moreover, they gave the generalization of the extended Gauss hypergeometric function, confluent hypergeomtric function and Appell hypergeometric functions as follows [38]:
F_{p,q}^{\kappa ,\mu }\left( {a,b,c;z} \right): = \sum\limits_{n = 0}^\infty {{{{{\left( {a;p,q;\kappa ,\mu } \right)}_n}{{\left( b \right)}_n}} \over {{{\left( c \right)}_n}}}} \cdot {{{z^n}} \over {n!}},\Phi _{p,q}^{\kappa ,\mu }\left( {a,b;z} \right): = \sum\limits_{n = 0}^\infty {{{{{\left( {a;p,q;\kappa ,\mu } \right)}_n}} \over {{{\left( b \right)}_n}}}} \cdot {{{z^n}} \over {n!}},\matrix{ {{}_{p,q}F_1^{\left( {\kappa ,\mu } \right)}\left[ {a;b,c;d;x,y} \right] = \sum\limits_{m,n = 0}^\infty {{{{{\left( {a;p,q;\kappa ,\mu } \right)}_{m + n}}{{\left( b \right)}_m}{{\left( c \right)}_n}} \over {{{\left( d \right)}_{m + n}}}}{{{x^m}} \over {m!}}{{{y^n}} \over {n!}}} } \cr {\max \left( {\left| x \right|,\left| y \right|} \right) < 1} \cr }
and
\matrix{ {{}_{p,q}F_2^{\left( {\kappa ,\mu } \right)}\left[ {a;b,c;d,e;x,y} \right] = \sum\limits_{m,n = 0}^\infty {{{{{\left( {a;p,q;\kappa ,\mu } \right)}_{m + n}}{{\left( b \right)}_m}{{\left( c \right)}_n}} \over {{{\left( d \right)}_m}{{\left( e \right)}_n}}}{{{x^m}} \over {m!}}{{{y^n}} \over {n!}}} } \cr {\left| x \right| + \left| y \right| < 1,} \cr }
respectively.
In our work, we have to recall the following fractional integral operators [13,18,19,36]. For x > 0, λ , ν, σ, ∈ ℂ and ℜ(λ ) > 0, we have
\left( {I_{0,x}^{\lambda ,\sigma ,\nu }f\left( t \right)} \right)\left( x \right) = {{{x^{ - \lambda - \sigma }}} \over {\Gamma \left( \lambda \right)}}\int_0^x {{{\left( {x - t} \right)}^{\lambda - 1}}{}_2{F_1}\left[ {\lambda + \sigma , - \nu ;\lambda ;1 - {t \over x}} \right]f\left( t \right)dt}
and
\left( {J_{0,\infty }^{\lambda ,\sigma ,\nu }f\left( t \right)} \right)\left( x \right) = {1 \over {\Gamma \left( \lambda \right)}}\int_x^\infty {{{\left( {t - x} \right)}^{\lambda - 1}}{t^{ - \lambda - \sigma }}{}_2{F_1}\left[ {\lambda + \sigma , - \nu ;\lambda ;1 - {t \over x}} \right]f\left( t \right)dt}
where the 2F1[.] is the Gauss hypergeometric function [1, 4, 14, 23, 26].
The Erdelyi-Kober type fractional integral operators are defined as follows [20]:
\left( {E_{0,x}^{\lambda ,\nu }f} \right)\left( x \right) = {{{x^{ - \lambda - \nu }}} \over {\Gamma \left( \lambda \right)}}\int_0^x {{{\left( {x - t} \right)}^{\lambda - 1}}f\left( t \right)dt} \,\,\,\,\,\,\,\,\,\,\left( {\Re \left( \lambda \right) > 0} \right)
and
\left( {K_{x,\infty }^{\lambda ,\nu }f} \right)\left( x \right) = {{{x^\nu }} \over {\Gamma \left( \lambda \right)}}\int_x^\infty {{{\left( {t - x} \right)}^{\lambda - 1}}{t^{ - \lambda - \nu }}f\left( t \right)dt} \,\,\,\,\,\,\,\,\,\,\left( {\Re \left( \lambda \right) > 0} \right).
The Riemann-Liouville fractional integral and the Weyl fractional integral operators defined as the follows [13, 18, 19, 36]:
\left( {R_{0,x}^\lambda f} \right)\left( x \right) = {1 \over {\Gamma \left( \lambda \right)}}\int_0^x {{{\left( {x - t} \right)}^{\lambda - 1}}f\left( t \right)dt}
and
\left( {W_{x,\infty }^\lambda f} \right)\left( x \right) = {1 \over {\Gamma \left( \lambda \right)}}\int_x^\infty {{{\left( {t - x} \right)}^{\lambda - 1}}f\left( t \right)dt.}
In [36], the operator I_{0,x}^{\lambda ,\sigma ,\nu }\left( \cdot \right) contains both the Riemann-Liouville and Erdelyi-Kober fractional integral operators by means of the following relationships:
\left( {R_{0,x}^\lambda f} \right)\left( x \right) = \left( {I_{0,x}^{\lambda , - \lambda ,\nu }f} \right)\left( x \right)
and
\left( {E_{0,x}^{\lambda ,\nu }f} \right)\left( x \right) = \left( {I_{0,x}^{\lambda ,0,\nu }f} \right)\left( x \right)
While the operator I_{0,x}^{\lambda ,\sigma ,\nu }\left( \cdot \right) unifies the Weyl and Erdelyi-Kober fractional integral operators as follows [36]:
\left( {W_{x,\infty }^\lambda f} \right)\left( x \right) = \left( {J_{x,\infty }^{\lambda , - \lambda ,\nu }f} \right)\left( x \right)
and
\left( {K_{x,\infty }^{\lambda ,\nu }f} \right)\left( x \right) = \left( {J_{x,\infty }^{\lambda ,0,\nu }f} \right)\left( x \right).
The following equations obtained by Kilbas [18] are also required for our work.
From its birth to its today’s wide use in a great number of scientific fields fractional calculus has come a long way. Despite the fact that its nearly as old as classical calculus itself, it flourished mainly over the last decades because of its good applicability on models describing complex real life problems (see. [5, 6, 28, 41]).
Here, by choosing a known generalization of the extended Gauss hypergeometric function in (7) we aim to establish certain formulas and representations for this extended Gauss hypergeometric function such as fractional derivative operators, integral transforms, fractional kinetic equations and generating functions. Also, we give some generating functions for extended Appell hypergemetric functions (9) and (10).
In this section, we will present some fractional integral formulas for the generalization of the extended Gauss hypergeometric function F_{p,q}^{\kappa ,\mu }\left( {a,b,c;z} \right) (7) by using several general pair of fractional calculus operators.
We begin by recalling a known concept of Hadamard products [18, 19]
Definition 1
Let f\left( z \right): = \sum\nolimits_{n = 0}^\infty {{a_n}{z^n}} and g\left( z \right): = \sum\nolimits_{n = 0}^\infty {{b_n}{z^n}} be two power series whose radii of convergence are given by Rf and Rg, respectively. Then their Hadamard product is power series defined by\left( {f*g} \right): = \sum\limits_{n = 0}^\infty {{a_n}{b_n}{z^n}}
whose radius of convergence R satifies Rf. Rg≤ R.
Especially, if one of the power series defines an entire function and the radius of convergence of the grater than zero, then the Hadamard product to seperate a newly-emerged function into two known functions. For example,
\matrix{ {{}_r{F_{s + m}}\left[ {\matrix{ {\left( {{a_1};p,q;\kappa ,\mu } \right),{a_2} \cdots {a_r}} \hfill & ; \hfill \cr {{b_1},{b_2}, \cdots ,{b_{s + m}}} \hfill & {;z} \hfill \cr } } \right]} \hfill \cr {\,\,: = {}_0{F_m}\left[ {\matrix{ { - - - } & ; \cr {{b_1},{b_2}, \cdots ,{b_m}} & {;z} \cr } } \right]*{}_r{F_s}\left[ {\matrix{ {\left( {{a_1};p,q;\kappa ,\mu } \right),{a_2} \cdots {a_r}} \hfill & ; \hfill \cr {{b_{1 + m}},{b_{2 + m}}, \cdots ,{b_{s + m}}} \hfill & {;z} \hfill \cr } } \right].} \hfill \cr {\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\left( {\left| z \right| < \infty } \right)} \hfill \cr }
The main results are obtained in the following theorems.
Theorem 4
Let λ , σ, ν, ρ ∈ ℂ be such that ℜ(λ ) > 0, ℜ(ρ) > max[0,ℜ(σ − ν)]; min{ℜ(p),ℜ(q),ℜ(κ),ℜ(μ) > 0};ℜ(c) > ℜ(b) > 0, then
Let’s denote the left-hand side of the equation (29) by L. Using the definition of the generalized hypergeometric function (7) and arranging order of integration and summation, which is applicable under the conditions Theorem 1, we get
L = \sum\limits_{n = 0}^\infty {{{{{\left( {a;p,q;\kappa ,\mu } \right)}_n}{{\left( b \right)}_n}} \over {{{\left( c \right)}_n}}}} \cdot {1 \over {n!}}\left[ {I_{0,x}^{\lambda ,\sigma ,\nu }{t^{\rho + n - 1}}} \right]\left( x \right),
taking advantage of the (21) in the above equality (30), we have
L = {x^{\rho - \sigma - 1}}\sum\limits_{n = 0}^\infty {{{{{\left( {a;p,q;\kappa ,\mu } \right)}_n}{{\left( b \right)}_n}} \over {{{\left( c \right)}_n}}}{{\Gamma \left( {\rho + n} \right)\Gamma \left( {\rho + \nu - \sigma + n} \right)} \over {\Gamma \left( {\rho - \sigma + n} \right)\Gamma \left( {\rho + \lambda + \nu + n} \right)}}{{{x^n}} \over {n!}}} ,
after simplfying the equation (31), we obtain
L = {x^{\rho - \sigma - 1}}{{\Gamma \left( \rho \right)\Gamma \left( {\rho + \nu - \sigma } \right)} \over {\Gamma \left( {\rho - \sigma } \right)\Gamma \left( {\rho + \lambda + \nu } \right)}}\sum\limits_{n = 0}^\infty {{{{{\left( {a;p,q;\kappa ,\mu } \right)}_n}{{\left( b \right)}_n}} \over {{{\left( c \right)}_n}}}{{{{\left( \rho \right)}_n}{{\left( {\rho + \nu - \sigma } \right)}_n}} \over {{{\left( {\rho - \sigma } \right)}_n}{{\left( {\rho + \lambda + \nu } \right)}_n}}}{{{x^n}} \over {n!}}} ,
further comment in the view of (7), we obtain
L = {x^{\rho - \sigma - 1}}{{\Gamma \left( \rho \right)\Gamma \left( {\rho + \nu - \sigma } \right)} \over {\Gamma \left( {\rho - \sigma } \right)\Gamma \left( {\rho + \lambda + \nu } \right)}}{}_2F_{p,q,2}^{\kappa ,\mu }\left( {a,b,\rho ,\rho + \nu - \sigma ;c,\rho - \sigma ,\rho + \lambda + \nu ;x} \right).
Finally, we have the desired result (29) in consinderation of the equation (28).
Theorem 5
Let λ , σ, ν, ρ ∈ ℂ be such that ℜ(λ ) > 0, ℜ(ρ) > max[0,ℜ(σ − ν)]; min{ℜ(p),ℜ(q),ℜ(κ),ℜ(μ) > 0};ℜ(c) > ℜ(b) > 0, then
In this section, we prensent some integral transforms for example, Pδ transform, Laplace transform, Sumudu transform, Hankel transform and Laguerre transform for the generalization of the extended hypergeometric function (7).
Pδ and Related Integral Transforms
The Pδ transform of f (t) is defined as [14, 24]
{P_\delta }\left\{ {f\left( t \right);s} \right\} = {F_P}\left( s \right) = \int_0^\infty {{{\left[ {1 + \left( {\delta - 1} \right)s} \right]}^{ - {t \over {\delta - 1}}}}f\left( t \right)dt} \,\,\,\,\,\,\,\,\,\,\,\,\left( {\delta > 1} \right),
on condition that the convenient existence condition given by Lemma 4 below are satisfied.
Lemma 10
Let the function f(t) be integrable over any finite interval (a,b) (0 < a < t < b). Suppose also that there exists a real number c such that each of the following assertions holds true:
For any arbitrary b > 0, \int_b^\iota {{e^{ - ct}}f\left( t \right)}tends to a finite limit as ι → ∞;
For any arbitrary a > 0, \int_\varepsilon ^a {\left| {f\left( t \right)} \right|dt}tends to a finite limit as ε → 0+.
Let’s denote the left-hand side given in equation (40) by 𝔓 and using the definition of the Pδ-transform (39), we get;
\mathfrak{P}= \mathop \smallint \limits_0^\infty {z^{\upsilon - 1}}{\left[ {1 + \left( {\delta - 1} \right)s} \right]^{ - {z \over {\delta - 1}}}}\left( {I_{0,x}^{\lambda ,\sigma ,\nu }{t^{\rho - 1}}F_{p,q}^{\kappa ,\mu }\left( {a,b,c;tz} \right)\left( x \right)} \right)dz,
taking advantage of the equation (29) and arranging order of integration and summation, which is applicable under conditions Theorem 3, we have
The proof of the Theorem 4 is parallel to the proof of Theorem 3
Upon letting δ → 1+ in the equation (39) is immediately reduced to the classic Laplace transform.
The Laplace transform of f (z) is defined as [14, 26, 35]:
\left\{\mathfrak{L} {f\left( z \right)} \right\}\int_0^\infty {{e^{ - sz}}f\left( z \right)dz} .
The folowing theorem is a limit case of Theorem 3 and Theorem 4 when δ → 1+
Theorem 13
Let λ , ρ ∈ ℂ be such that ℜ(λ ) > 0, ℜ(ρ) > max[0,ℜ(σ − ν)]; min{ℜ(p),ℜ(q),ℜ(κ),ℜ(μ) > 0};ℜ(c) > ℜ(b) > 0, then
The Hankel transform of f (z) is given as follows [14, 24]:
{H_\alpha }\left\{ {f\left( z \right)} \right\}\left( u \right) = \int_0^\infty {z{J_\alpha }} \left( {uz} \right)f\left( z \right)dz,
where Jα(z) is the first kind of Bessel function [14, 24, 35, 40].
The proof of the Theorem 8 is similar to the proof of Theorem 7.
Laguerre Transform
The Laguerre transform of f (z) is given as follows [14, 24]:
{{\cal L}^{\left( \alpha \right)}}\left\{ {f\left( z \right);\left( m \right)} \right\} = \int_0^\infty {{e^{ - z}}{z^\alpha }L_m^\alpha } \left( z \right)f\left( z \right)dz,
where L_m^\alpha \left( z \right) is the Laguerre polynomial [14, 24, 35].
Let’s denote the left-hand side of the equation (63) by M. Using the definition of the Laguerre transform in the above equation, we have
\matrix{ {{\bf{M}} = {x^{\rho - \sigma - 1}}{{\Gamma \left( \rho \right)\Gamma \left( {\rho + \nu - \sigma } \right)} \over {\Gamma \left( {\rho - \sigma } \right)\Gamma \left( {\rho + \lambda + \nu } \right)}}\sum\limits_{n = 0}^\infty {{{{{\left( {a;p,q;\kappa ,\mu } \right)}_n}{{\left( b \right)}_n}} \over {{{\left( c \right)}_n}}}} } \hfill \cr {\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\, \times {{{{\left( \rho \right)}_n}{{\left( {\rho + \nu - \sigma } \right)}_n}} \over {{{\left( {\rho - \sigma } \right)}_n}{{\left( {\rho + \lambda + \nu } \right)}_n}}}{{{x^n}} \over {n!}}\int_0^\infty {{e^z}{z^{\alpha + \beta + n - 1}}L_m^\alpha \left( z \right)dz,} } \hfill \cr }
Now, applying well-knowns integral formula for power function including Laguerre polynomial [14, 24],
\int_0^\infty {{e^z}{z^{\beta - 1}}{z^{\alpha + \beta + n - 1}}L_m^\alpha \left( z \right)dz} = {{\Gamma \left( {\alpha + \beta + n} \right)\Gamma \left( {m - \beta + 1} \right)} \over {m!\Gamma \left( {1 - \beta } \right)}},
after simplfying equation (65) and using the definition of (7), we obtain
In this section, we will present certain generating functions involving new generalization of extended Gauss hypergeometric function and extended Appell hypergeometric functions.
Let N be the left side of (73), using the (9) and interchanging the order of summations, we have that
{\bf{N}}=\sum\limits_{m,n = 0}^\infty {\sum\limits_{k = 0}^\infty {{{\left( \alpha \right)}_k}} {{\left( {\alpha + k} \right)}_m}} {{{{\left( {a;p,q;\kappa ,\mu } \right)}_{m + n}}{{\left( c \right)}_n}} \over {{{\left( d \right)}_{m + n}}}}{{{x^m}} \over {m!}}{{{y^n}} \over {n!}}.
Applying the equation (71) in the equation (74), we can be easily seen to lead to right-hand side of (73).
Theorem 24
The following generating function for (10) holds true:
The proof of the Theorem 14 is same as the proof of Theorem 13.
Fractional Differential Equations
The importance of the fractional differential equations in the field of applied sciences gained more attention not in mathematics but also in physics, dynamical systems, control systems and engineering, to create the mathematical model of physical phenomena. Specially, the kinetic equations describe the contiunity of motion of substance. The extension and generalisation of fractional kinetic equations involving many fractional operators were found in [2, 3, 9, 11, 12, 15, 31, 32, 33].
The fractional differential equation between rate of change of the reaction, the destruction rate and the production rate was established by Haubold and Mathai [15] given as follows:
{{dN} \over {dt}} = - d\left( {{N_t}} \right) + p\left( {{N_t}} \right)
where N = N(t) the rate of the reaction, d = d(N) the rate of destruction, p = p(N) the rate of production and Nt denotes the function defined by Nt(t<sup>⋆</sup>) = N(t − t<sup>⋆</sup>),t<sup>⋆ </sup>> 0.
The special case of equation (76) for spatial fluctuations and inhomogeneities in N(t) the quantities are neglected, that is the equation{{dN} \over {dt}} = - {c_i}{N_i}\left( t \right)
with the initial condition that Ni(t = 0) = N0 is the number of density of the species i at time t = 0 and ci > 0. If we shift the index i and integrate the standard kinetic equation (77), we have
N\left( t \right) - {N_0} = - {c_0}D_t^{ - 1}N\left( t \right)
where _0D_t^{ - 1} is the special case of the Riemann-Liouville integral operator _0D_t^{ - V} given as
{}_0D_t^{ - \nu }f\left( t \right) = {1 \over {\Gamma \left( \nu \right)}}\int_0^t {{{\left( {t - s} \right)}^{\nu - 1}}f\left( s \right)ds} ,\,\,\,\,\left( {t > 0,\Re \left( \nu \right) > 0.} \right)
The fractional generalisation of the standart kinetic equation (78) is given by Haubold and Mathai as follows [31, 32]:
N\left( t \right) - {N_0} = - {c^\nu }{}_0D_t^{ - 1}N\left( t \right)
and obtained the solution of (77) as follows:
N\left( t \right) = {N_0}\sum\limits_{k = 0}^\infty {{{\left( { - {1^k}} \right)} \over {\Gamma \left( {\nu k + 1} \right)}}{{\left( {ct} \right)}^{\nu k}}.}
Furthermore, Saxena and Kalla [33] considered the following fractional kinetic equation:
N\left( t \right) - {N_0}f\left( t \right) = - {c^\nu }{}_0D_t^{ - 1}N\left( t \right)\left( {\Re \left( \nu \right) > 0} \right),
where N(t) denotes the number density of a given species at time t, N0 = N(0) is the number of density of that species at time t = 0, c is a constant and f ∈ L(0,∞).
By applying the Laplace transform (46) to the equation (82),
\mathcal{L}\left\{ {N\left( t \right);p} \right\} = {N_0}{{F\left( p \right)} \over {1 + {c^\nu }{p^{ - \nu }}}} = {N_0}\left( {\sum\limits_{n = 0}^\infty {{{\left( { - {c^\nu }} \right)}^n}{p^{ - \nu n}}} } \right)F\left( p \right),\left( {n \in {N_0},\left| {{c \over p}} \right| < 1} \right).
Solution of the generalised fractional kinetic equations
In this section, we will present the solution of the generalised fractional kinetic equations which by considering generalised Gauss hypergeometric function (7).
Theorem 25
If d > 0, ν > 0; p,q,κ, μ,a,b,c,δ ∈ ℂ be such that ℜ(c) > ℜ(b) > 0;min{ℜ(p),ℜ(q),ℜ(κ),ℜ(μ) > 0}, then the solution of the following fractional equationN\left( t \right) - {N_0}F_{p,q}^{\kappa ,\mu }\left( {a,b,c;{d^\nu }{t^\nu }} \right) = - {\delta ^\nu }{}_0D_t^{ - \nu }N\left( t \right)is given byN\left( t \right) = {N_0}\sum\limits_{n = 0}^\infty {{{{{\left( {a;p,q;\kappa ,\mu } \right)}_n}{{\left( b \right)}_n}} \over {{{\left( c \right)}_n}}}{{\Gamma \left( {\nu n + 1} \right){{\left( {{d^\nu }{t^\nu }} \right)}^n}} \over {n!}}} {E_{\nu ,\nu n + 1}}\left( { - {\delta ^\nu }{t^\nu }} \right)where Eν,νn+1(−δ <sup>ν</sup>t<sup>ν</sup>) is the Mittag-Leffler function [25].
Proof
The Laplace transform of the Riemann-Liouville fractional integral operator is defined by [14, 36]:
{\frak{L}}\left\{ {{}_0D_t^{ - \nu }f\left( t \right);s} \right\} = {s^{ - \nu }}F\left( s \right)
where F(p) is given in (46). Now, applying the Laplace transform to the both sides of (84), we obtain
If d > 0, ν > 0; p,q,κ, μ,a,b,c,δ ∈ ℂ be such that ℜ(c) > ℜ(b) > 0;min{ℜ(p),ℜ(q),ℜ(κ),ℜ(μ) > 0}, then the solution of the following fractional equation:N\left( t \right) - {N_0}F_{p,q}^{\kappa ,\mu }\left( {a,b,c;{d^\nu }{t^\nu }} \right) = - {d^\nu }{}_0D_t^{ - v}N\left( t \right)is given byN\left( t \right) = {N_0}\sum\limits_{n = 0}^\infty {{{{{\left( {a;p,q;\kappa ,\mu } \right)}_n}{{\left( b \right)}_n}} \over {{{\left( c \right)}_n}}}{{\Gamma \left( {\nu n + 1} \right){{\left( {{d^\nu }{t^\nu }} \right)}^n}} \over {n!}}} {E_{\nu ,\nu n + 1}}\left( { - {d^\nu }{t^\nu }} \right).
Proof
Choosing δ = d in equation (84), we can be easily yield the desired result (90).
Theorem 27
If d > 0; p,q,κ, μ,a,b,c,δ ∈ ℂ be such that ℜ(c) > ℜ(b) > 0;min{ℜ(p),ℜ(q),ℜ(κ),ℜ(μ) > 0}, then the solution of the following fractional equation
N\left( t \right) - {N_0}F_{p,q}^{\kappa ,\mu }\left( {a,b,c;t} \right) = - \delta {}_0D_t^{ - 1}N\left( t \right)is given byN\left( t \right) = {N_0}\sum\limits_{n = 0}^\infty {{{{{\left( {a;p,q;\kappa ,\mu } \right)}_n}{{\left( b \right)}_n}} \over {{{\left( c \right)}_n}}}} {{\Gamma \left( {n + 2} \right){{\left( t \right)}^n}} \over {n!}}{E_{1,n + 2}}\left( { - \delta t} \right).
Proof
Choosing ν = d = 1 in equation (84), we can be easily yield the desired result (90).
Corollary 28
If d > 0; p,q,κ, μ,a,b,c,δ ∈ ℂ be such that ℜ(c) > ℜ(b) > 0;min{ℜ(p),ℜ(q),ℜ(κ),ℜ(μ) > 0}, then the solution of the following fractional equationN\left( t \right) - {N_0}F_{p,q}^{\kappa ,\mu }\left( {a,b,c;t} \right) = - \delta {}_0D_t^{ - 1}N\left( t \right)is given by\eqalign{ & N\left( t \right) = {N_0} - \sum\limits_{n = 0}^\infty {{{{{\left( {a;p,q;\kappa ,\mu } \right)}_n}{{\left( b \right)}_n}} \over {{{\left( c \right)}_n}}}{{\left( {n + 1} \right){{\left( t \right)}^{n - 1}}} \over \delta }{E_{1,n + 1}}\left( { - \delta t} \right)} \cr & \,\,\,\,\,\,\,\,\,\,\,\,\,\,\, + {1 \over {\delta t}}F_{p,q}^{\kappa ,\mu }\left( {a,b,c;t} \right) + {{a.b} \over {c.\delta }}F_{p,q}^{\kappa ,\mu }\left( {a + 1,b + 1,c + 1;t} \right). \cr}
Proof
Applying the above Mittag-Leffler function properties [14, 24]
{E_{\alpha ,\beta }}\left( z \right) = {1 \over z}{E_{\alpha ,\beta - \alpha }}\left( z \right) - {1 \over {z\Gamma \left( {\beta - \alpha } \right)}},
in the equation (93). Then, making some simple arrangment, we can be easily yield the desired result (95)
Conclusions
We may also give point to that results obtained in this work are of general character and can appropriate to give farther interesting and potentially practical formulas involving integral transform, fractional calculus and generating functions. Also we give a new fractional generalization of the standard kinetic equation and obtained solution for the same. From the close relationship of family of extended generalized Gauss hypergeometric functions with many special functions, we can easily construct various known and new fractional kinetic equations.