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# Inequalities involving hypergeometric and related functions

*Journal of Inequalities and Applications*
**volume 2018**, Article number: 253 (2018)

## Abstract

An inequality is being proved which is connected to cost-effective numerical density estimation of the hyper-gamma probability distribution. The left-hand side of the inequality is a combination of two in the third parameter distinct versions of the hypergeometric function at the point one. All three parameters are functions of the distribution’s terminal shape. The first and second are equal. The distinct third parameters of the two hypergeometric functions depend on terminal and initial shape. The other side of the inequality is determined by the quotient of two infinite series, which are related to the first derivatives with respect to terminal shape of the hypergeometric functions which appear in its left-hand side.

## Introduction

Certain inequalities shall be considered, which involve combinations of gamma and psi functions of one positive variable *β* and one parameter *x* greater than unity. The basic functions involved are particular values of the hypergeometric function \(F(a,b,c;s)\) [1, 9.122.1], namely:

where \(\Gamma (s)\) is the gamma function, \(y_{\nu }= \nu \beta + x\), \(\nu = 0,1,2,\dots \), with \(\beta \in (0, \infty)\), \(x \in (1, \infty)\) throughout. The product representations of \(A(\beta; x)\) and \(B(\beta; x)\) are given is [1, 8.325.1]. Associated with these functions is their product

Since \(a+b-c < 0\) for each of the hypergeometric functions in (1.1), (1.2), and (1.3), each of their series expansions converges throughout the entire closed unit circle of the complex plane [1, 9.102.2], and the gamma function expressions are justified [1, 9.122.1].

For the sake of simplicity we shall from now on omit the arguments *β* and *x* whenever there is no chance for confusion, keeping in mind, however, that *β* in the actual independent variable, and that *x* is a parameter. If we attach an argument to a symbol of a dependent variable, it will be a particular value of *β*. For example, \(A(1) = A(1;x)\). Furthermore, derivatives will always be with respect to *β* and will be denoted by a prime.

The functions *A*, *B*, and *C* satisfy the inequalities

The infinite product representations of *A*, *B*, and *C* show that

and

as \(\beta \uparrow \infty \). (The down-arrow means that the function at its left decreases toward the value at its right as its argument decreases. The up-arrow indicates the opposite.) We note the particular values

The *β*-derivatives of *A*, *B*, and *C* are

with

\(\psi_{\nu }= \psi ((x+\nu -2)/\beta)\), \(\nu = 1, \dots,4, \psi (s)\) being the *ψ* function, \(\psi (s) = d\log \Gamma (s)/ds\) [1, 8.360].

If we consider instead of (1.1), (1.2), and (1.3) the more general function

with differentiable functions \(\varphi_{\nu }= \varphi_{\nu }(\beta)\), \(\nu = 1,2,3\), then

provided that Re\((\varphi_{1} + \varphi_{2} - \varphi_{3}) < 0\) in some region *R* of the complex *β*-plane. For \(\varphi_{1} = 1/\beta\), \(\varphi_{2} = -1/\beta\), \(\varphi_{3} = x/\beta \) this formula reduces to \(A' = 2AS\) with *S* given in (1.8).

Related to *S* and *T* is the function

The series expansion of the psi function [1, 8.362, 1],

where *γ* is Euler’s constant, leads to the series representations of *T*, *Q*, and *S*,

(Cancellation of the respective factors \(y_{\nu }+ \alpha\) (\(\alpha = -1, 0, 1, 2\)) in (1.11) would not bring any advantage. In fact, it would hamper comparison of equally numbered terms of these series and related expressions.)

Under the restrictions on *β* and *x*, each of the series in (1.11) is positive, and

Therefore, the derivatives \(A'\), \(B'\), and \(C'\) in (1.7) are positive, i.e., the functions *A*, *B*, and *C* are strictly monotonically increasing for \(\beta > 0\) and, by (1.5a), (1.5b), bounded. (This belatedly justifies the direction of the arrows in the limit relations (1.5a), (1.5b).)

We now introduce the gamma function combination

with *A* and *B* defined in (1.1) and (1.2), respectively. The main objective of this paper is to establish the inequality

It is a crucial prerequisite to an efficient numerical solution routine of the four-parameter hyper-gamma density estimation problem for a given statistical data set (observations) [2, Chap. 9.3]. The hyper-gamma distribution has important applications in chemical, biological, and physical processes. The four parameters of the distribution are shift, scale, initial shape \(x>1\) (in the statistical four-parameter case \(x > 2\)), and terminal shape \(\beta > 0\). The statistical parameters *β* and *x* are to be determined from a set of two simultaneous equations [2, (9.33), (9.34)]. These are derived from the first four moments of the four-parameter hyper-gamma probability density function [2, (9.3.1)], which are defined by combinations of gamma functions as they appear in (1.1) and (1.2). A considerable computational cost advantage is achieved if it is known that for every fixed value of *x*, say, one of these equations has exactly one solution *β*. This will be the case if (1.15) holds. (See [2, Chaps. 9.2, 9.3], equation (9.3.34) and the discussion preceding (9.3.36).)

## Approximating sequences for \(Q/S\) and \(T/S\)

The series (1.11) and their *β*-derivatives converge (absolutely and) uniformly as functions of *β* on every closed subinterval \([a, b] \subset (0, \infty)\) for any fixed \(x > 1\). To show this, we look at *Q*, for example,

(Here the common factor \(y_{\nu }\) in numerator and denominator has been canceled.) We have \(0 < q_{\nu }< 1 /\nu^{2} \beta^{3} < 1 / \nu^{2} a ^{3}\). Thus, by the Weierstraßcriterion,

where \(\zeta (s)\) is Riemann’s zeta function [1, 9.522.1]. The terms of the *β*-derivative \(Q'\) of *Q* are

with

Now, \(0 < \gamma_{\mu \nu } < 1 / \nu^{4} \beta^{4}\), \(\mu = 1, 2, 3\), \(\nu = 1, 2, \dots\), and, hence, \(|q'_{\nu }| < 3 / a^{4} \nu^{2}\). Therefore, \(|Q'| < 3 \zeta (2) / a^{4}\), i.e., the series \(Q' = \sum q'_{\nu }\) is absolutely and uniformly convergent on \([a, b]\). Since \(Q' < 0\), *Q* is strictly monotonically decreasing as *β* increases. The second derivative of *Q* is positive. This follows immediately from (2.1). Thus, with \(Q'' > 0\), the function *Q* is concave from above, and \(|Q'|\) is strictly monotonically decreasing. Corresponding facts are true for *T* and *S*. Note that *T*, *Q*, and \(S \uparrow \infty \) (monotonically) as \(\beta \downarrow 0\), and that *T*, *Q*, and \(S \downarrow 0\) (monotonically) as \(\beta \uparrow \infty \).

The following particular values of these functions for \(\beta = 1\) are of interest:

They are obtained from (1.9), (1.10a), (1.10b), and (1.8), respectively, and from the functional relation [1, 8.365.3] of the psi function.

We now define the sequence \(\{ F_{n} (\beta; x)\}\) with elements

where \(Q_{n}\) and \(S_{n}\) are the partial sums of *Q* and *S*,

with

We observe that \(r_{n}\) and \(p_{n}\) (both polynomials in *β* of degree \(4(n-1)\)) can be expressed as

and that the positive series

converge uniformly (for any \(x \in (1, \infty)\)) on every interval \([a, b] \subset (0, \infty)\). This follows immediately by the Weierstraßcriterion since

so that

Furthermore,

so that

and, consequently,

The series

converge absolutely and uniformly on every interval \([a, b] \subset (0, \infty)\). Note that the series (2.7) are strictly monotonically decreasing functions of \(\beta \in (0, \infty)\).

We return to the functions \(F_{n}\) defined by (2.3) and show that

i.e., that

By (1.11)

\(u_{\nu }\) given in (2.8), so that (2.12) may be replaced by

Here we replace \(S_{n} - Q_{n}\) by \(2 \sum_{\nu =1}^{n} u_{ \nu }\) and obtain, after dropping the common factor 2,

Comparing equally numbered terms of the two infinite series, we get

or, with \(q_{n+k} = (n+k) y_{n+k} / \rho_{n+k}\) and \(u_{n+k} = (n+k) / \rho_{n+k}\),

This difference is positive since \(y_{n+k} > y_{\nu }\) for \(\nu = 1, \dots, n\). Therefore, (2.13) is correct, and, consequently, (2.11) holds. With this result, and

we see that

(the upward arrow will be justified in Sect. 3), and that

Next, we show that

By means of (2.4a), (2.4b), the rational functions \(F_{n}\) defined in (2.3) can be written as

With this expression for \(F_{n}\), inequality (2.16) changes into \(r_{n} p_{n+1} > r_{n+1} p_{n}\). The recurrence relations for \(r_{n}\) and \(p_{n}\) in (2.5) lead to \((n+1) r_{n} > p_{n}\), which is correct. Thus (2.16) holds.

The facts established so far show that \(\{ F_{n} \}\) is a positive, increasing, bounded above sequence that converges for every \(\beta \in (0, \infty)\) and any fixed \(x \in (1, \infty)\) as \(n \uparrow \infty \). We want to show now that it converges to \(Q/S\) uniformly on every subinterval \([a, b]\) of \((0, \infty)\).

Observing (2.12), we have to show that for every \(\varepsilon > 0\) there exists \(n_{0} = n_{0} (\varepsilon)\) such that

Now,

Since \(q_{\nu }< s_{\nu }= \nu (y_{\nu }+ 2) / \rho_{\nu }\), we have

Here

The right-hand side of this inequality is strictly monotonically decreasing as stated earlier in connection with (2.8) and (2.10). Thus

Therefore, we may continue inequality (2.19) as follows:

Uniform convergence of *S* on \([a, b]\) implies that, given \(\varepsilon /K\), there exists \(n_{0} = n_{0}(\varepsilon)\) such that

This proves (2.18). So \(\{ F_{n} \}\) is a uniformly convergent approximating sequence for \(Q/S\) from below, and

This shows that \((Q/S) (0) = F_{1}(0) = x/(x+2)\), so that (2.15) may be sharpened to

(The downward arrow will be justified in Sect. 3.)

Along the same lines analogous results can be established for the function \(T/S\) and its approximating from below sequence

Note that

and

## Monotonicity of \(Q/S\) and \(T/S\)

The functions \(Q/S\) and \(T/S\) are strictly monotonically increasing for \(\beta \in (0, \infty)\). It is sufficient to show this for \(Q/S\) since, by (1.10a), \(T/S = (3Q/S-1)/2\).

We introduce the rational functions

\(r_{n}\) and \(p_{n}\) defined by (2.6). Note that \(f_{n+1} < f_{n}\) because \(\{ u_{\nu }/ v_{\nu }\} = \{ 1 / \nu \}\) is a decreasing sequence [3, p. 10, Problem 28]. The approximating functions \(F_{n}\) in (2.17) can now be written as

The *β*-derivative of \(F_{n}\) is

and

This immediately shows that \(F'_{n} > 0\) for small positive values of *β*. We want to show that \(F'_{n} > 0\) for \(\beta \in (0, \infty)\). But first we must establish certain facts about the rational functions \(f_{n} = r_{n} / p_{n}\). By (2.5) and with \(\rho_{\nu }= ( \nu \beta + x - 1)(\nu \beta + x)(\nu \beta + x + 1) (\nu \beta + x +2)\) the constituent terms of \(r_{n}\) and \(p_{n}\) are products of \(n-1\) Hurwitz polynomials, each of degree 4, so that each of those terms is a Huwitz polynomial of degree \(4(n-1)\). The *β*-derivative of \(f_{n}\) is

Using (2.8) and (2.9) in (3.4b), we arrive at

Here

the positive functions \(\alpha_{\nu }\) (\(\nu = 1,\dots, 4\)) being defined in connection with (1.12). Thus, by (3.5), \(f'_{n} > 0\), \(\beta > 0\), \(x>1\). This establishes strict monotonicity of the functions \(f_{n}\) defined in (3.1). Note that \(0 < f_{n} < 1\), \(n \geq 2\), \(\beta > 0\) and

We also note the following facts about \(f'_{n}\), which follow from (3.4a),

Furthermore, (2.5) together with (1.12) and with the notation used in (3.6) shows that

so that

Consequently,

where \(c_{n}\) is a positive constant. Since

we see that \(f'_{n}\) as given in (3.4a) behaves like \(\beta^{-2}\) as \(\beta \uparrow \infty \). In other words, \(f'_{n}\) and \(\beta^{-2}\) are asymptotically proportional. Consequently,

We now remember the fact that the polynomials \(\rho_{\nu }\) are Hurwitzian and that, consequently, the constituent terms of the polynomials \(r_{n}\) and \(p_{n}\) in (2.5) are Hurwitzian. By Theorem IV of [4] (in conjunction with the specification of terminology concerning *circular regions* and *circles* on p. 164 of [4]) the sum of any two of these constituent polynomials of degree \(4(n-1)\) is Hurwitzian. Thus, \(r_{n}\) and \(p_{n}\) are Hurwitz polynomials. Their zeros are located in the open left-hand half of the complex *β*-plane, which we denote by *L*. By another theorem [5, p. 115], all zeros of \(f'_{n}\) (and all its poles) are located in *L*. In other words, \(f'_{n} > 0\) for real \(\beta > 0\), a fact which has been established earlier already by direct means. Applying the theorem of [5] again, this time to the rational function \(f'_{n}\), we arrive at the result that \(f''_{n}\) has all its zeros (and poles) in *L*, i.e., \(f''_{n} \neq 0\) for real \(\beta > 0\). Limit relation (3.7) shows that \(f'_{n}\) decreases somewhere in the interval \((0, \infty)\). Thus, the *β*-derivative \(f''_{n}\) of \(f'_{n}\) must be negative somewhere. Since \(f''_{n} \neq 0\) for \(\beta > 0\), if follows that \(f''_{n} < 0\) for all \(\beta > 0\). In other words, \(f_{n}\), defined by (3.1) is concave from below on \(0 < \beta < \infty \), i.e., the tangent at any point \((\beta_{0}, f_{n}(\beta_{0}))\), \(\beta_{0} > 0\), lies above the graph of \(f_{n}\) for every \(\beta > 0\), \(\beta \neq \beta_{0}\).

Since, by (3.2), \(F'_{n} (0) > 0\), if follows that \(F' > 0\) at least for small positive values of *β*. This means that \(f_{n} - \beta f'_{n} > 0\) for small positive values of *β* as can be seen from (3.3). This can also be verified by means of (3.6), (3.7), and (3.8), respectively. By (3.6) and (3.8) we see that \(f_{n} - \beta f'_{n} > 0\) also for large values of *β*, so that \(F'_{n} > 0\) for large *β*. Suppose now that \(f_{n} - \beta f'_{n} < 0\) at some point \(\beta > 0\). Then there exist points \(\beta_{1}\) and \(\beta_{2}\), \(0 < \beta_{1} < \beta_{2}\), such that

\(f_{n} - \beta f'_{n} > 0\) for \(0 < \beta < \beta_{1}\) and \(\beta_{2} < \beta < \infty \), and \(f_{n} - \beta f'_{n} < 0\) for \(\beta_{1} < \beta < \beta_{2}\). Consequently, there would exist a continuous function \(\alpha (\beta)\) such that \(\alpha (\beta_{\nu }) = 0\), \(\nu = 1, 2\), \(\alpha (\beta) > 0\), \(\beta_{1} < \beta < \beta_{2}\), and

This inhomogeneous linear differential equation has the unique solution

with initial condition \((\beta_{1}, f_{n} (\beta_{1}))\). Its derivative is

Observing (3.9) for \(\nu =2\) and noting that \(\alpha (\beta_{2}) =0\), we have at \(\beta_{2}\)

since the integral is positive. Now, the tangent to the integral curve defined by (3.10) at the point \((\beta_{1}, f_{n} (\beta_{1}))\) is given by \(y(\beta) = f_{n} (\beta_{1}) + (\beta - \beta_{1}) f'_{n} (\beta _{1})\) with \(f'_{n} (\beta_{1}) = f_{n}(\beta_{1}) / \beta_{1}\) by (3.9).

Thus,

Since \(f_{\nu }\) is concave from below it follows that

or

in contradiction to (3.11). Consequently, \(f_{n} - \beta f'_{n} > 0\) for all \(\beta \in (0, \infty)\), and, hence, as (2.3) shows, \(F'_{n} > 0\) for \(0 < \beta < \infty \), which means that \(F_{n} = Q_{n} / S_{n}\), or \(F_{n} = (xf_{n} + \beta) / [ (x+2)f_{n} + \beta ]^{-1}\), is a strictly monotonically increasing function of \(\beta \in (0, \infty)\). A corresponding result holds for \(G_{n} = T_{n} / S_{n}\).

We now show that the sequence \(\{ F'_{n} \}\) converges uniformly on every closed interval \([a, b] \subset (0, \infty)\). Differentiating \(F_{n} = Q_{n} / S_{n}\), we form

With \(Q = \sum q_{\nu }\), \(S = \sum s_{\nu }\), equation (3.12), after some manipulations, can be brought into the form

Here, we replace all negative terms between the absolute value bars by their absolute values. Since *Q*, \(|Q'|\), *S*, \(|S'|\) are series with positive terms, we increase the right-hand side of (3.13) by replacing their partial sums by the entire series. Then we remember the fact that these series are monotonically decreasing functions of *β*. Therefore, we increase the right-hand side of (3.13) further by setting \(Q_{n} < Q < Q(a)\), \(|Q'_{n}| < |Q'| < |Q'(a)|\), \(S_{n} < S(a)\), \(|S'_{n}| < |S'(a)|\) for \(\beta \in [a,b]\). We may also replace \(\sum q_{\nu }\) by \(\sum s_{\nu }\) since \(0 < q_{\nu }< s_{\nu }\). Thus, there exist positive constants \(K_{\nu }\) (\(\nu = 1,\dots,5\)) such that equality (3.13) may be replaced by the inequality

Furthermore, by (1.11),

so that

Now, since *S*, \(S'\), and \(Q'\) converge uniformly on \([a, b] \in (0, \infty)\), given \(\varepsilon > 0\) there exists a number \(n_{0}( \varepsilon)\) such that each of the five finite sums in (3.14) is less than \(B^{-4} (\sum_{\nu =1}^{5} K_{\nu })^{-1} \varepsilon \) for every \(n \geq n_{0}\) and for all \(k \geq 1\). Thus (3.14) together with (3.15) leads to \(|F'_{n+k} - F'_{n}| < \varepsilon \) for every \(n \geq n_{0}\) and for all \(k \geq 1\) on every \([a, b] \subset (0, \infty)\). The final result is that \(\{ F'_{n} \}\) converges uniformly for \(\beta \in [a,b]\) to the function \((Q/S)' > 0\), and this means that \(Q/S\) is strictly monotonically increasing. (This result justified the direction of the arrows in (2.14) and (2.20), and in (2.21) and (2.22) for \(T/S\).)

## Properties of *σ*

The function

together with (1.1) and (1.2), evidently satisfies the inequality \(0 < \sigma < A\), \(\beta > 0\) and by (1.5a), (1.5b), the limit relations

(The downward arrows in (4.2) will be justified momentarily.) Furthermore, observing (1.6), we see that at \(\beta = 1\)

The *β*-derivative of *σ* is given by

This shows that \(\sigma < Q/S\) whenever \(\sigma '\) is nonpositive. For, if \(\sigma ' \le 0\), then \(\sigma \le CT/S < T/S < Q/S\), if we observe (1.3) and (1.4). The function \(\sigma '\) is negative somewhere. To see this, we note that for \(\beta = 1\), (4.4) becomes

Here (1.6) and (2.2) have been used. Continuity of *σ* implies that \(\sigma (1 + \varepsilon) > \sigma (1) = \sigma_{\infty }\) at least for sufficiently small values of \(\varepsilon > 0\). Inequality (4.5) and the second limit relation (4.2) show that *σ* has a local maximum at some point \(\beta^{\star }> 1\). Suppose *σ* had more than one maximum in \((0, \infty)\). Let \(0 < \beta_{1} < \beta _{2}\) be points at which maxima are attained. Then *σ* must have a minimum at some point \(\beta_{0}\), \(\beta_{1} < \beta_{0} < \beta _{2}\). We have

and \(\sigma ' (\beta_{1}) = \sigma ' (\beta_{0}) = 0\), so that, according to (4.4)

Since *C* and \(T/S\) are both monotonically increasing, it would follow that \(\sigma (\beta_{1}) < \sigma (\beta_{0})\), in contradiction to (4.6). Consequently, there exists one and only one point \(\beta^{ \star }\) at which \(\sigma ' = 0\) and at which *σ* takes its maximum. We have \(\sigma ' \geq 0\) if \(\beta \in (0, \beta^{\star }]\), \(\sigma ' < 0\) if \(\beta \in (\beta^{\star }, \infty)\). In other words, *σ* is strictly monotonically decreasing on \((\beta^{\star }, \infty)\). (This result belatedly justifies the direction of the arrows in the limit relations (4.2).)

We now turn to the relation between *σ* given by (4.1) and \(C = AB\) defined by (1.3). By (4.3), \(\sigma (1) = C(1)\). Furthermore, by (4.2) and (1.5b) \(\sigma_{\infty }< C_{\infty }\). Thus, *σ* and *C* are not identical, and \(\sigma < C\) for large values of *β* since *σ* is strictly monotonically decreasing after it reaches its single maximum at \(\beta^{\star }> 1\), and *C* is strictly monotonically increasing. More can be obtained by comparing the derivatives of *σ* and *C* at \(\beta = 1\). Using the particular value of *C* at \(\beta = 1\) given in (1.6) and those of *S* and *T* for \(\beta = 1\) given in (2.2) and the definition of \(C'\) given in (1.7), we find that

Comparing this with \(\sigma ' (1)\) in (4.5), we see that

This and \(\sigma (1) = C(1)\) imply that for sufficiently small \(\varepsilon > 0\),

and

We show first that (4.7) holds for \(\beta \in (1, \infty)\). Observing (4.1) and setting \(C = AB\), we transform the desired inequality (4.7) into

Here, we set \(A = \kappa B\), \(0 < \kappa = \kappa (\beta; x) < 1\), \(\beta \in [1, \infty)\), \(x \in (1, \infty)\), noting that *κ* has a positive *β*-derivative (by (1.7) and (1.13)),

so that *κ* is strictly monotonically increasing, and by (1.6) and (1.5b),

Furthermore, since by (1.1) and (1.2), the factors of the infinite product for \(\kappa = A/B\) go to \((x+1)^{3} (x-1) / x^{3} (x+2) < 1\) as \(\beta \downarrow 0\), *κ* diverges toward 0 as \(\beta \downarrow 0\).

With \(A = \kappa B\), inequality (4.9) takes the form

The equation \(g(B) = 0\) has the two roots,

\(0 < B_{1} < 1 < B_{2}\). Since \(B < B_{\infty }= x(x+2) / (x+1)^{2} < B_{2}\) by (1.5b), the root \(B_{2}\) is outside the range of *B*. At \(B_{\infty }\), *g* takes the negative value \(g(B_{\infty }) = -2 [x(x+1)]^{-1}\). Consequently, as stipulated by (4.10), \(g(B) < 0\) for \(B_{1} < B < B_{\infty }\), i.e., for \(1 < \beta < \infty \), and \(g(B) = 0\) if and only if \(\beta = 1\), i.e., for \(B(1) = B_{1} ( \kappa (1))\). Thus (4.7) holds for \(\beta \in (1, \infty)\).

For \(\beta \in (0,1)\) we have \(0 < B < B(1) = B_{1} (\kappa (1))\), and the function \(g(B)\) in (4.10) is positive, i.e., the inequality sign in (4.10) is reversed. This proves (4.8) for the entire interval \(0 < \beta < 1\).

Our results are these:

and

Finally, for \(\beta = 1\), \(g(B(1)) = 0\), i.e.,

## The inequality \(\sigma < Q/S\)

We turn now to our main objective and prove the inequality \(\sigma < Q/S\), \(\beta \in (0, \infty)\), fixed \(x \in (1, \infty)\). We know that \(\sigma < Q/S\) holds for small positive values of *β* since, by (4.2), \(\sigma \downarrow 0\) as \(\beta \downarrow 0\), and \(Q/S > x/(x+2)\) as \(\beta \downarrow 0\) by (2.15). Furthermore, \(\sigma < Q/S\) as \(\beta \uparrow \infty \) since *σ* decreases monotonically toward \(\sigma_{\infty }= (x-1)/(x+1) < 1\) as \(\beta \uparrow \infty \) by (4.2), whereas \(Q/S \uparrow 1\) by (2.14). (The fact that \(\sigma_{\infty }< 1\) also follows directly from \(\sigma < A < A_{ \infty }< 1\) for \(\beta \in (0, \infty)\).) Therefore, if the desired inequality \(\sigma < Q/S\) should not hold throughout, it must be violated somewhere in the interval \((0, \infty)\).

Observing definition (4.1) of *σ* and setting \(Q/S = z\) for simplicity, the proposed inequality \(\sigma < z\) can be transformed into

Here we set \(B = \lambda A\), \(\lambda = \lambda (\beta; x) > 1\), \(\beta \in (0, \infty)\), \(x \in (1, \infty)\). *λ* has a negative *β*-derivative,

so that *λ* is strictly monotonically decreasing. By (1.6) and (1.5b),

and, by (1.1) and (1.2), the factors of the infinite product \(\lambda = B/A =\kappa^{-1}\) go to \(x^{3} (x+2) / (x+1)^{3} (x-1) > 1\) as \(\beta \downarrow 0\), i.e., *λ* diverges ↑∞, as \(\beta \downarrow 0\).

With \(B = \lambda A\), inequality (5.1) takes the form

Suppose \(h(A)\) as function of *β* were negative somewhere in \((0, \infty)\). Then *h* would have to be zero somewhere in that interval. The roots of the equation \(h = 0\) are

Here \((1+z)/2\lambda < 1\) because \(1 + z < 2\) and \(\lambda > 1\), and the radicant in (5.3)

is negative as \(\beta \downarrow 0\) since \(\lambda \uparrow \infty \), and, as \(\beta \uparrow \infty \), by (1.5b) and with \(z \uparrow 1\),

Thus, for small and large values of *β*, \(A_{1,2}\) would be nonreal.

Suppose *j*, given in (5.4), were positive somewhere in \((0, \infty)\). Then it must be zero somewhere in that interval. The equation \(j=0\) has the two roots

The second one is greater than unity since \(\lambda > 1\). It is outside the range of \(z = Q/S < 1\). Then, using the root \(z_{1}\) for *z* in (5.3) and squaring the equality to get rid of the square root, we arrive at the equality \(\lambda A^{2} - 2\lambda A + 1 = 0\), or, if we replace *λA* by *B* and *AB* by *C*, at the equality

which we have encountered before in (4.11). We know that it holds if and only if \(\beta = 1\). But for \(\beta = 1\),

This contradiction shows that \(h(A)\) cannot be negative or zero on the interval \(0 < \beta < \infty \). Thus, (5.2) holds, and \(\sigma < Q/S\) for \(\beta \in (0, \infty)\), fixed \(x \in (1, \infty)\).

## Declarations

### Results and discussions

Inequalities have been proved which involve various combinations of psi- and hypergeometric functions. They add to the wealth of knowledge in the theory of these special function classes of higher analysis.

### Conclusions

The main inequality of this paper guarantees uniqueness of the hyper-gamma parameter estimation and its application. Usefulness of this approach has been demonstrated in [6].

### Methods/experimental

The aim of the study is to prove an inequality made up of functions of higher mathematical analysis. This inequality guarantees monotonicity of the first moment equation function of the four-parameter hyper-gamma probability density estimation problem. Monotonicity guarantees uniqueness of the numerical solution process. Standard analytical methods of higher analysis have been employed to accomplish the proof.

## References

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Knopp, K.: Theorie und Anwendungen der Unendlichen Reihen. Springer, Berlin (1964)

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**12**, 163–180 (1922)Walsh, J.L.: On the location of the roots of the Jacobian of two binary forms, and of the derivative of a rational function. Trans. Am. Math. Soc.

**22**, 101–116 (1921)Dudel, H.P., Hall, C.E., Lehnigk, S.H.: Estimation algorithms for the hyper-gamma distribution class. Commun. Stat., Simul. Comput.

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### Cite this article

Lehnigk, S.H. Inequalities involving hypergeometric and related functions.
*J Inequal Appl* **2018**, 253 (2018). https://doi.org/10.1186/s13660-018-1842-4

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DOI: https://doi.org/10.1186/s13660-018-1842-4

### MSC

- 33C05
- 33B20
- 26D10
- 97K80
- 65C60

### Keywords

- Hypergeometric functions
- Gamma functions
- Inequalities
- Applied statistics
- Computational problems in statistics