Generalized hypergeometric function

For other generalizations of the hypergeometric function, see Hypergeometric function.

Not to be confused with general hypergeometric function.

In mathematics, a generalized hypergeometric series is a power series in which the ratio of successive coefficients indexed by n is a rational function of n. The series, if convergent, defines a generalized hypergeometric function, which may then be defined over a wider domain of the argument by analytic continuation. The generalized hypergeometric series is sometimes just called the hypergeometric series, though this term also sometimes just refers to the Gaussian hypergeometric series. Generalized hypergeometric functions include the (Gaussian) hypergeometric function and the confluent hypergeometric function as special cases, which in turn have many particular special functions as special cases, such as elementary functions, Bessel functions, and the classical orthogonal polynomials.

Notation

A hypergeometric series is formally defined as a power series

\beta_0 + \beta_1 z + \beta_2 z^2 + \dots = \sum_{n \geqslant 0} \beta_n z^n

in which the ratio of successive coefficients is a rational function of n. That is,

\frac{\beta_{n+1}}{\beta_n} = \frac{A(n)}{B(n)}

where A(n) and B(n) are polynomials in n.

For example, in the case of the series for the exponential function,

1+\frac{z}{1!}+\frac{z^2}{2!}+\frac{z^3}{3!}+c\dots,

we have:

\beta_n = \frac{1}{n!}, \qquad \frac{\beta_{n+1}}{\beta_n} = \frac{1}{n+1}.

So this satisfies the definition with $A (n) = 1$ and $B (n) = n + 1$ .

It is customary to factor out the leading term, so β₀ is assumed to be 1. The polynomials can be factored into linear factors of the form (a_j + n) and (b_k + n) respectively, where the a_j and b_k are complex numbers.

For historical reasons, it is assumed that (1 + n) is a factor of B. If this is not already the case then both A and B can be multiplied by this factor; the factor cancels so the terms are unchanged and there is no loss of generality.

The ratio between consecutive coefficients now has the form

\frac{c(a_1+n)\dots(a_p+n)}{d(b_1+n)\dots(b_q+n)(1+n)}

where c and d are the leading coefficients of A and B. The series then has the form

1 + \frac{a_1\dots a_p}{b_1\dots b_q.1}\frac{cz}{d} + \frac{a_1\dots a_p}{b_1\dots b_q.1} \frac{(a_1+1)\dots(a_p+1)}{(b_1+1)\dots (b_q+1).2}\left(\frac{cz}{d}\right)^2+\dots

or, by scaling z by the appropriate factor and rearranging,

1 + \frac{a_1\dots a_p}{b_1\dots b_q}\frac{z}{1!} + \frac{a_1(a_1+1)\dots a_p(a_p+1)}{b_1(b_1+1)\dots b_q(b_q+1)}\frac{z^2}{2!}+\dots

This has the form of an exponential generating function. The standard notation for this series is usually denoted by:

{}_pF_q(a_1,\ldots,a_p;b_1,\ldots,b_q;z)

\,{}_pF_q \left[\begin{matrix} a_1 & a_2 & \ldots & a_{p} \\ b_1 & b_2 & \ldots & b_q \end{matrix} ; z \right]

Using the rising factorial or Pochhammer symbol:

\begin{align} (a)_0 &= 1, \\ (a)_n &= a(a+1)(a+2)...(a+n-1), && n \geq 1 \end{align}

this can be written

\,{}_pF_q(a_1,\ldots,a_p;b_1,\ldots,b_q;z) = \sum_{n=0}^\infty \frac{(a_1)_n\dots(a_p)_n}{(b_1)_n\dots(b_q)_n} \, \frac {z^n} {n!}

(Note that this use of the Pochhammer symbol is not standard, however it is the standard usage in this context.)

Special cases

Many of the special functions in mathematics are special cases of the confluent hypergeometric function or the hypergeometric function; see the corresponding articles for examples.

Some of the functions related to more complicated hypergeometric functions include:

Dilogarithm:^[1]

\operatorname{Li}_2(x) = \sum_{n>0}\,{x^n}{n^{-2}} = x \; {}_3F_2(1,1,1;2,2;x)

Hahn polynomials:

Q_n(x;a,b,N)= {}_3F_2(-n,-x,n+a+b+1;a+1,-N+1;1).\

Wilson polynomials:

p_n(t^2)=(a+b)_n(a+c)_n(a+d)_n \; {}_4F_3\left( \begin{matrix} -n&a+b+c+d+n-1&a-t&a+t \\ a+b&a+c&a+d \end{matrix} ;1\right).

Terminology

When all the terms of the series are defined and it has a non-zero radius of convergence, then the series defines an analytic function. Such a function, and its analytic continuations, is called the hypergeometric function.

The case when the radius of convergence is 0 yields many interesting series in mathematics, for example the incomplete gamma function has the asymptotic expansion

\Gamma(a,z) \sim z^{a-1}e^{-z}\left(1+\frac{a-1}{z}+\frac{(a-1)(a-2)}{z^2}\dots\right)

which could be written z^a−1e^−z ₂F₀(1−a,1;;−z⁻¹). However, the use of the term hypergeometric series is usually restricted to the case where the series defines an actual analytic function.

The ordinary hypergeometric series should not be confused with the basic hypergeometric series, which, despite its name, is a rather more complicated and recondite series. The "basic" series is the q-analog of the ordinary hypergeometric series. There are several such generalizations of the ordinary hypergeometric series, including the ones coming from zonal spherical functions on Riemannian symmetric spaces.

The series without the factor of n! in the denominator (summed over all integers n, including negative) is called the bilateral hypergeometric series.

Convergence conditions

There are certain values of the a_j and b_k for which the numerator or the denominator of the coefficients is 0.

If any a_j is a non-positive integer (0, −1, −2, etc.) then the series only has a finite number of terms and is, in fact, a polynomial of degree −a_j.
If any b_k is a non-positive integer (excepting the previous case with −b_k < a_j) then the denominators become 0 and the series is undefined.

Excluding these cases, the ratio test can be applied to determine the radius of convergence.

If p < q + 1 then the ratio of coefficients tends to zero. This implies that the series converges for any finite value of z. An example is the power series for the exponential function.
If p = q + 1 then the ratio of coefficients tends to one. This implies that the series converges for |z| < 1 and diverges for |z| > 1. Whether it converges for |z| = 1 is more difficult to determine. Analytic continuation can be employed for larger values of z.
If p > q + 1 then the ratio of coefficients grows without bound. This implies that, besides z = 0, the series diverges. This is then a divergent or asymptotic series, or it can be interpreted as a symbolic shorthand for a differential equation that the sum satisfies.

The question of convergence for p=q+1 when z is on the unit circle is more difficult. It can be shown that the series converges absolutely at z = 1 if

\Re\left(\sum b_k - \sum a_j\right)>0

Further, if p=q+1, $\sum_{i=1}^{p}a_{i}\geq\sum_{j=1}^{q}b_{j}$ and z is real, then the following convergence result holds (Quigley et al 2013):

\lim_{z\rightarrow 1}(1-z)\frac{d\log(_{p}F_{q}(a_{1},\ldots,a_{p};b_{1},\ldots,b_{q};z^{p}))}{dz}=\sum_{i=1}^{p}a_{i}-\sum_{j=1}^{q}b_{j}

Basic properties

It is immediate from the definition that the order of the parameters a_j, or the order of the parameters b_k can be changed without changing the value of the function. Also, if any of the parameters a_j is equal to any of the parameters b_k, then the matching parameters can be "cancelled out", with certain exceptions when the parameters are non-positive integers. For example,

\,{}_2F_1(3,1;1;z) = \,{}_2F_1(1,3;1;z) = \,{}_1F_0(3;;z)

Euler's integral transform

The following basic identity is very useful as it relates the higher-order hypergeometric functions in terms of integrals over the lower order ones^[2]

{}_{A+1}F_{B+1}\left[ \begin{array}{c} a_{1},\ldots ,a_{A},c \\ b_{1},\ldots ,b_{B},d \end{array} ;z\right] =\frac{\Gamma (d)}{\Gamma (c)\Gamma (d-c)} \int_{0}^{1}t^{c-1}(1-t)_{{}}^{d-c-1}\ {}_{A}F_{B}\left[ \begin{array}{c} a_{1},\ldots ,a_{A} \\ b_{1},\ldots ,b_{B} \end{array} ; tz\right] dt

Differentiation

The generalized hypergeometric function satisfies

\begin{align} \left (z\frac{{\rm{d}}}{{\rm{d}}z} + a_j \right ){}_pF_q\left[ \begin{array}{c} a_1,\dots,a_j,\dots,a_p \\ b_1,\dots,b_q\end{array} ;z\right] &= a_j \; {}_pF_q\left[ \begin{array}{c} a_1,\dots,a_j+1,\dots,a_p \\ b_1,\dots,b_q \end{array} ;z\right] \\ \left (z\frac{{\rm{d}}}{{\rm{d}}z} + b_k - 1 \right ){}_pF_q\left[ \begin{array}{c} a_1,\dots,a_p \\ b_1,\dots,b_k,\dots,b_q\end{array} ;z\right] &= (b_k - 1) \; {}_pF_q\left[ \begin{array}{c} a_1,\dots,a_p \\ b_1,\dots,b_k-1,\dots,b_q \end{array} ;z \right] \\ \frac{{\rm{d}}}{{\rm{d}}z} \; {}_pF_q\left[ \begin{array}{c} a_1,\dots,a_p \\ b_1,\dots,b_q \end{array} ;z \right] &= \frac{\prod_{i=1}^p a_i}{\prod_{j=1}^q b_j}\; {}_pF_q\left[ \begin{array}{c} a_1+1,\dots,a_p+1 \\ b_1+1,\dots,b_q+1 \end{array} ;z \right] \end{align}

Combining these gives a differential equation satisfied by w = _pF_q:

z\prod_{n=1}^{p}\left(z\frac{{\rm{d}}}{{\rm{d}}z} + a_n\right)w = z\frac{{\rm{d}}}{{\rm{d}}z}\prod_{n=1}^{q}\left(z\frac{{\rm{d}}}{{\rm{d}}z} + b_n-1\right)w

Contiguous function and related identities

Take the following operator:

\vartheta = z\frac{{\rm{d}}}{{\rm{d}}z}.

From the differentiation formulas given above, the linear space spanned by

{}_pF_q(a_1,\dots,a_p;b_1,\dots,b_q;z), \vartheta\; {}_pF_q(a_1,\dots,a_p;b_1,\dots,b_q;z)

contains each of

{}_pF_q(a_1,\dots,a_j+1,\dots,a_p;b_1,\dots,b_q;z),

{}_pF_q(a_1,\dots,a_p;b_1,\dots,b_k-1,\dots,b_q;z),

z\; {}_pF_q(a_1+1,\dots,a_p+1;b_1+1,\dots,b_q+1;z),

{}_pF_q(a_1,\dots,a_p;b_1,\dots,b_q;z).

Since the space has dimension 2, any three of these p+q+2 functions are linearly dependent. These dependencies can be written out to generate a large number of identities involving ${}_pF_q$ .

For example, in the simplest non-trivial case,

\; {}_0F_1(;a;z) = (1) \; {}_0F_1(;a;z)

\; {}_0F_1(;a-1;z) = (\frac{\vartheta}{a-1}+1) \; {}_0F_1(;a;z)

z \; {}_0F_1(;a+1;z) = (a\vartheta) \; {}_0F_1(;a;z)

\; {}_0F_1(;a-1;z)- \; {}_0F_1(;a;z) = \frac{z}{a(a-1)} \; {}_0F_1(;a+1;z)

This, and other important examples,

\; {}_1F_1(a+1;b;z)- \, {}_1F_1(a;b;z) = \frac{z}{b} \; {}_1F_1(a+1;b+1;z)

\; {}_1F_1(a;b-1;z)- \, {}_1F_1(a;b;z) = \frac{az}{b(b-1)} \; {}_1F_1(a+1;b+1;z)

\; {}_1F_1(a;b-1;z)- \, {}_1F_1(a+1;b;z) = \frac{(a-b+1)z}{b(b-1)} \; {}_1F_1(a+1;b+1;z)

\; {}_2F_1(a+1,b;c;z)- \, {}_2F_1(a,b;c;z) = \frac{bz}{c} \; {}_2F_1(a+1,b+1;c+1;z)

\; {}_2F_1(a+1,b;c;z)- \, {}_2F_1(a,b+1;c;z) = \frac{(b-a)z}{c} \; {}_2F_1(a+1,b+1;c+1;z)

\; {}_2F_1(a,b;c-1;z)- \, {}_2F_1(a+1,b;c;z) = \frac{(a-c+1)bz}{c(c-1)} \; {}_2F_1(a+1,b+1;c+1;z)

can be used to generate continued fraction expressions known as Gauss's continued fraction.

Similarly, by applying the differentiation formulas twice, there are $\binom{p+q+3}{2}$ such functions contained in

\{1, \vartheta, \vartheta^2\}\; {}_p F_q (a_1,\dots,a_p;b_1,\dots,b_q;z),

which has dimension three so any four are linearly dependent. This generates more identities and the process can be continued. The identities thus generated can be combined with each other to produce new ones in a different way.

A function obtained by adding ±1 to exactly one of the parameters a_j, b_k in

{}_pF_q(a_1,\dots,a_p;b_1,\dots,b_q;z)

is called contiguous to

{}_pF_q(a_1,\dots,a_p;b_1,\dots,b_q;z).

Using the technique outlined above, an identity relating ${}_0F_1(;a;z)$ and its two contiguous functions can be given, six identities relating ${}_1F_1(a;b;z)$ and any two of its four contiguous functions, and fifteen identities relating ${}_2F_1(a,b;c;z)$ and any two of its six contiguous functions have been found. (The first one was derived in the previous paragraph. The last fifteen were given by Gauss in his 1812 paper.)

Identities

For identities involving the Gauss hypergeometric function ₂F₁, see Hypergeometric function.

A number of other hypergeometric function identities were discovered in the nineteenth and twentieth centuries. A 20th century contribution to the methodology of proving these identities is the Egorychev method.

Saalschütz's theorem

Saalschütz's theorem^[3] (Saalschütz 1890) is

{}_3F_2 (a,b, -n;c, 1+a+b-c-n;1)= \frac{(c-a)_n(c-b)_n}{(c)_n(c-a-b)_n}.

For extension of this theorem, see a research paper by Rakha & Rathie.

Dixon's identity

Main article: Dixon's identity

Dixon's identity,^[4] first proved by Dixon (1902), gives the sum of a well-poised ₃F₂ at 1:

{}_3F_2 (a,b,c;1+a-b,1+a-c;1)= \frac{\Gamma(1+\frac{a}{2})\Gamma(1+\frac{a}{2}-b-c)\Gamma(1+a-b)\Gamma(1+a-c)}{\Gamma(1+a)\Gamma(1+a-b-c)\Gamma(1+\frac{a}{2}-b)\Gamma(1+\frac{a}{2}-c)}.

For generalization of Dixon's identity, see a paper by Lavoie, et al.

Dougall's formula

Dougall's formula (Dougall 1907) gives the sum of a terminating well-poised series:

\begin{align} {}_7F_6 & \left(\begin{matrix}a&1+\frac{a}{2}&b&c&d&e&-m\\&\frac{a}{2}&1+a-b&1+a-c&1+a-d&1+a-e&1+a+m\\ \end{matrix};1\right) = \\ &=\frac{(1+a)_m(1+a-b-c)_m(1+a-c-d)_m(1+a-b-d)_m}{(1+a-b)_m(1+a-c)_m(1+a-d)_m(1+a-b-c-d)_m} \end{align}

provided that m is a non-negative integer (so that the series terminates) and

1+2a=b+c+d+e-m.

Many of the other formulas for special values of hypergeometric functions can be derived from this as special or limiting cases.

Generalization of Kummer's transformations and identities for ₂F₂

Identity 1.

e^{-x} \; {}_2F_2(a,1+d;c,d;x)= {}_2F_2(c-a-1,f+1;c,f;-x)

where

f=\frac{d(a-c+1)}{a-d}

;

Identity 2.

e^{-\frac x 2} \, {}_2F_2 \left(a, 1+b; 2a+1, b; x\right)= {}_0F_1 \left(;a+\tfrac{1}{2}; \tfrac {x^2} {16}\right) - \frac{x\left(1-\tfrac{2a} b\right)}{2(2a+1)}\; {}_0F_1 \left(;a+\tfrac 3 2; \tfrac {x^2} {16}\right),

which links Bessel functions to ₂F₂; this reduces to Kummer's second formula for b = 2a:

Identity 3.

e^{-\frac x 2} \, {}_1F_1(a,2a,x)= {}_0F_1 \left (;a+\tfrac 1 2; \tfrac{x^2}{16} \right )

Identity 4.

\begin{align} {}_2F_2(a,b;c,d;x)=& \sum_{i=0} \frac{{b-d \choose i}{a+i-1 \choose i}}{{c+i-1 \choose i}{d+i-1 \choose i}} \; {}_1F_1(a+i;c+i;x)\frac{x^i}{i!} \\ =& e^x \sum_{i=0} \frac{{b-d \choose i}{a+i-1 \choose i}}{{c+i-1 \choose i}{d+i-1 \choose i}} \; {}_1F_1(c-a;c+i;-x)\frac{x^i}{i!}, \end{align}

which is a finite sum if b-d is a non-negative integer.

Kummer's relation

Kummer's relation is

{}_2F_1\left(2a,2b;a+b+\tfrac 1 2;x\right)= {}_2F_1\left(a,b; a+b+\tfrac 1 2; 4x(1-x)\right).

Clausen's formula

Main article: Clausen's formula

Clausen's formula

{}_3F_2(2c-2s-1, 2s, c-\tfrac 1 2; 2c-1, c; x)=\, {}_2F_1(c-s-\tfrac 1 2,s; c; x)^2

was used by de Branges to prove the Bieberbach conjecture.

Special cases

The series ₀F₀

Main article: Exponential function

As noted earlier, ${}_0F_0(;;z) = e^z$ . The differential equation for this function is $\frac{d}{dz}w = w$ , which has solutions $w = ke^z$ where k is a constant.

The series ₁F₀

Also as noted earlier,

{}_1F_0(a;;z) = (1-z)^{-a}.

The differential equation for this function is

\frac{d}{dz}w =\left (z\frac{d}{dz}+a \right )w,

(1-z)\frac{dw}{dz} = aw,

which has solutions

w=k(1-z)^{-a}

where k is a constant.

{}_1F_0(1;;z) = (1-z)^{-1}

is the geometric series with ratio z and coefficient 1.

The series ₀F₁

The functions of the form ${}_0F_1(;a;z)$ are called confluent hypergeometric limit functions and are closely related to Bessel functions. The relationship is:

J_\alpha(x)=\frac{(\tfrac{x}{2})^\alpha}{\Gamma(\alpha+1)} {}_0F_1\left (;\alpha+1; -\tfrac{1}{4}x^2 \right ).

The differential equation for this function is

w = \left (z\frac{d}{dz}+a \right )\frac{dw}{dz}

z\frac{d^2w}{dz^2}+a\frac{dw}{dz}-w = 0.

When a is not a positive integer, the substitution

w = z^{1-a}u,

gives a linearly independent solution

z^{1-a}\;{}_0F_1(;2-a;z),

so the general solution is

k\;{}_0F_1(;a;z)+l z^{1-a}\;{}_0F_1(;2-a;z)

where k, l are constants. (If a is a positive integer, the independent solution is given by the appropriate Bessel function of the second kind.)

The series ₁F₁

Main article: Confluent hypergeometric function

The functions of the form ${}_1F_1(a;b;z)$ are called confluent hypergeometric functions of the first kind, also written $M(a;b;z)$ . The incomplete gamma function $\gamma(a,z)$ is a special case.

The differential equation for this function is

\left (z\frac{d}{dz}+a \right )w = \left (z\frac{d}{dz}+b \right )\frac{dw}{dz}

z\frac{d^2w}{dz^2}+(b-z)\frac{dw}{dz}-aw = 0.

When b is not a positive integer, the substitution

w = z^{1-b}u,

gives a linearly independent solution

z^{1-b}\;{}_1F_1(1+a-b;2-b;z),

so the general solution is

k\;{}_1F_1(a;b;z)+l z^{1-b}\;{}_1F_1(1+a-b;2-b;z)

where k, l are constants.

When a is a non-positive integer, −n, ${}_1F_1(-n;b;z)$ is a polynomial. Up to constant factors, these are the Laguerre polynomials. This implies Hermite polynomials can be expressed in terms of ₁F₁ as well.

The series ₂F₀

This occurs in connection with the exponential integral function Ei(z).

The series ₂F₁

Main article: Hypergeometric function

Historically, the most important are the functions of the form ${}_2F_1(a,b;c;z)$ . These are sometimes called Gauss's hypergeometric functions, classical standard hypergeometric or often simply hypergeometric functions. The term Generalized hypergeometric function is used for the functions _pF_q if there is risk of confusion. This function was first studied in detail by Carl Friedrich Gauss, who explored the conditions for its convergence.

The differential equation for this function is

\left (z\frac{d}{dz}+a \right ) \left (z\frac{d}{dz}+b \right )w =\left (z\frac{d}{dz}+c \right )\frac{dw}{dz}

z(1-z)\frac{d^2w}{dz^2}+(c-(a+b+1)z)\frac{dw}{dz}-abw = 0.

It is known as the hypergeometric differential equation. When c is not a positive integer, the substitution

w = z^{1-c}u

gives a linearly independent solution

z^{1-c}\; {}_2F_1(1+a-c,1+b-c;2-c;z),

so the general solution for |z| < 1 is

k\; {}_2F_1(a,b;c;z)+l z^{1-c}\; {}_2F_1(1+a-c,1+b-c;2-c;z)

where k, l are constants. Different solutions can be derived for other values of z. In fact there are 24 solutions, known as the Kummer solutions, derivable using various identities, valid in different regions of the complex plane.

When a is a non-positive integer, −n,

{}_2F_1(-n,b;c;z)

is a polynomial. Up to constant factors and scaling, these are the Jacobi polynomials. Several other classes of orthogonal polynomials, up to constant factors, are special cases of Jacobi polynomials, so these can be expressed using ₂F₁ as well. This includes Legendre polynomials and Chebyshev polynomials.

A wide range of integrals of elementary functions can be expressed using the hypergeometric function, e.g.:

\int_0^x\sqrt{1+y^\alpha}\,\mathrm{d}y=\frac{x}{2+\alpha}\left \{\alpha\;{}_2F_1\left(\tfrac{1}{\alpha},\tfrac{1}{2};1+\tfrac{1}{\alpha};-x^\alpha \right) +2\sqrt{x^\alpha+1} \right \},\qquad \alpha\neq0.

The series ₃F₀

This occurs in connection with Mott polynomials.^[5]

The series ₃F₁

This occurs in the theory of Bessel functions. It provides a way to compute Bessel functions of large arguments.

Generalizations

The generalized hypergeometric function is linked to the Meijer G-function and the MacRobert E-function. Hypergeometric series were generalised to several variables, for example by Paul Emile Appell and Joseph Kampé de Fériet; but a comparable general theory took long to emerge. Many identities were found, some quite remarkable. A generalization, the q-series analogues, called the basic hypergeometric series, were given by Eduard Heine in the late nineteenth century. Here, the ratios considered of successive terms, instead of a rational function of n, are a rational function of qⁿ. Another generalization, the elliptic hypergeometric series, are those series where the ratio of terms is an elliptic function (a doubly periodic meromorphic function) of n.

During the twentieth century this was a fruitful area of combinatorial mathematics, with numerous connections to other fields. There are a number of new definitions of general hypergeometric functions, by Aomoto, Israel Gelfand and others; and applications for example to the combinatorics of arranging a number of hyperplanes in complex N-space (see arrangement of hyperplanes).

Special hypergeometric functions occur as zonal spherical functions on Riemannian symmetric spaces and semi-simple Lie groups. Their importance and role can be understood through the following example: the hypergeometric series ₂F₁ has the Legendre polynomials as a special case, and when considered in the form of spherical harmonics, these polynomials reflect, in a certain sense, the symmetry properties of the two-sphere or, equivalently, the rotations given by the Lie group SO(3). In tensor product decompositions of concrete representations of this group Clebsch–Gordan coefficients are met, which can be written as ₃F₂ hypergeometric series.

Bilateral hypergeometric series are a generalization of hypergeometric functions where one sums over all integers, not just the positive ones.

Fox–Wright functions are a generalization of generalized hypergeometric functions where the Pochhammer symbols in the series expression are generalised to gamma functions of linear expressions in the index n.

Notes

↑ Candan, Cagatay. "A Simple Proof of F(1,1,1;2,2;x)=dilog(1-x)/x" (PDF).
↑ (Slater 1966, Equation (4.1.2))
↑ See (Slater 1966, Section 2.3.1) or (Bailey 1935, Section 2.2) for a proof.
↑ See (Bailey 1935, Section 3.1) for a detailed proof. An alternative proof is in (Slater 1966, Section 2.3.3)
↑ See Erdélyi et al. 1955.

References

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Bailey, W.N. (1935). Generalized Hypergeometric Series. Cambridge Tracts in Mathematics and Mathematical Physics 32. London: Cambridge University Press. Zbl 0011.02303.
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Dougall, J. (1907). "On Vandermonde's theorem and some more general expansions". Proc. Edinburgh Math. Soc. 25: 114–132. doi:10.1017/S0013091500033642.
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External links

The book "A = B", this book is freely downloadable from the internet.
MathWorld

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Generalized hypergeometric function

Notation

Special cases

Terminology

Convergence conditions

Basic properties

Euler's integral transform

Differentiation

Contiguous function and related identities

Identities

Saalschütz's theorem

Dixon's identity

Dougall's formula

Generalization of Kummer's transformations and identities for 2F2

Kummer's relation

Clausen's formula

Special cases

The series 0F0

The series 1F0

The series 0F1

The series 1F1

The series 2F0

The series 2F1

The series 3F0

The series 3F1

Generalizations

Notes

References

External links

Generalization of Kummer's transformations and identities for ₂F₂

The series ₀F₀

The series ₁F₀

The series ₀F₁

The series ₁F₁

The series ₂F₀

The series ₂F₁

The series ₃F₀

The series ₃F₁