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 HarmonicNumber

Introduction to the differentiated gamma functions

General

Almost simultaneously with the development of the mathematical theory of factorials, binomials, and gamma functions in the 18th century, some mathematicians introduced and studied related special functions that are basically derivatives of the gamma function. These functions appeared in coefficients of the series expansions of the solutions in the logarithmic cases of some important differential equations. They appear in the Bessel differential equation for example. So functions in this group are called the differentiated gamma functions.

The harmonic numbers for integer have a very long history. The famous Pythagoras of Samos (569–475 B.C.) was the first to encounter the harmonic series

in connection with string vibrations and his special interest in music. Richard Suiseth (14th century) and Nicole d’Oresme (1350) studied the harmonic series and discovered that it diverges. Pietro Mengoli (1647) proved the divergence of the harmonic series. Nicolaus Mercator (1668) studied the harmonic series corresponding to the series of and Jacob Bernoulli (1689) again proved the divergence of the harmonic series. The harmonic numbers with integer also appeared in an article of G. W. Leibniz (1673).

In his famous work, J. Stirling (1730) not only found the asymptotic formula for factorial , but used the digamma psi function (related to the harmonic numbers), which is equal to the derivative of the logarithm from the gamma function (). Later L. Euler (1740) also used harmonic numbers and introduced the generalized harmonic numbers .

The digamma function and its derivatives of positive integer orders were widely used in the research of A. M. Legendre (1809), S. Poisson (1811), C. F. Gauss (1810), and others. M. A. Stern (1847) proved the convergence of the Stirling series for the digamma function:

At the end of the 20th century, mathematicians began to investigate extending the function to all complex values of (B. Ross (1974), N. Grossman (1976)). R. W. Gosper (1997) defined and studied the cases and . V. S. Adamchik (1998) suggested the definition for complex using Liouville's fractional integration operator. A natural extension of for the complex order was recently suggested by O. I. Marichev (2001) during the development of subsections with fractional integro‐differentiation for the Wolfram Functions website and the technical computing system Mathematica:

Definitions of the differentiated gamma functions

The digamma function , polygamma function , harmonic number , and generalized harmonic number are defined by the following formulas (the first formula is a general definition for complex arguments and the second formula is for positive integer arguments):

Here is the Euler gamma constant:

Remark: This formula presents the (not unique) continuation of the classical definition of from positive integer values of to its arbitrary complex values.

For positive integer and arbitrary complex , , the following definitions are commonly used:

The previous definition for uses the Mathematica definition for the Hurwitz zeta function . Branch cuts and related properties are thus inherited from .

The previous functions are interconnected and belong to the differentiated gamma functions group. These functions are widely used in the coefficients of series expansions for many mathematical functions (especially the so‐called logarithmic cases).

A quick look at the differentiated gamma functions

Here is a quick look at the graphics for the differentiated gamma functions along the real axis.

Connections within the group of differentiated gamma functions and with other function groups

Representations through more general functions

The differentiated gamma functions , , , and are particular cases of the more general hypergeometric and Meijer G functions. Although the arguments of these functions do not depend on the variable , it is included in their parameters.

For example, , , , and can be represented through generalized hypergeometric functions by the following formulas:

The aforementioned general formulas can be rewritten using the classical Meijer G functions as follows:

Representations through related equivalent functions

The differentiated gamma functions , , , and can be represented through derivatives of the gamma function :

The differentiated gamma functions , , , and can also be represented through derivatives of the logarithm of the gamma function :

The functions and are intimately related to the Hurwitz zeta function and the Bernoulli polynomials and numbers , by the formulas:

Representations through other differentiated gamma functions

The differentiated gamma functions , , , and are interconnected through the following formulas:

The best-known properties and formulas for differentiated gamma functions

Real values for real arguments

For real values of the argument and nonnegative integer , the differentiated gamma functions , , , and are real (or infinity). The function is real (or infinity) for real values of argument and integer .

Simple values at zero

The differentiated gamma functions , , , and have simple values for zero arguments:

Values at fixed points

The differentiated gamma functions , , , and with rational arguments can sometimes be evaluated through classical constants and logarithms, for example:

Specific values for specialized variables

The previous relations are particular cases of the following general formulas:

The differentiated gamma functions and with integer parameters and have the following representations:

Analyticity

The digamma function and the harmonic number are defined for all complex values of the variable . The functions and are analytical functions of and over the whole complex ‐ and ‐planes. For fixed , the generalized harmonic number is an entire function of .

Poles and essential singularities

The differentiated gamma functions and have an infinite set of singular points , where for and for . These points are the simple poles with residues . The point is the accumulation point of poles for the functions , , and (with fixed nonnegative integer ), which means that is an essential singular point.

For fixed nonnegative integer , the function has an infinite set of singular points: are the simple poles with residues ; and are the poles of order with residues .

For fixed , the function does not have poles and the function has only one singular point at , which is an essential singular point.

Branch points and branch cuts

The functions and do not have branch points and branch cuts.

For integer , the function does not have branch points and branch cuts.

For fixed noninteger , the function has two singular branch points and , and it is a single‐valued function on the ‐plane cut along the interval , where it is continuous from above:

For fixed , the functions and do not have branch points and branch cuts.

Periodicity

The differentiated gamma functions , , , and do not have periodicity.

Parity and symmetry

The differentiated gamma functions , , , and have mirror symmetry:

Series representations

The differentiated gamma functions , , and have the following series expansions near regular points:

Near singular points, the differentiated gamma functions , , , and can be expanded through the following series:

Here is the Euler gamma constant .

Except for the generalized power series, there are other types of series through which differentiated gamma functions , , , and can be represented, for example:

Asymptotic series expansions

The asymptotic behavior of the differentiated gamma functions , , , and can be described by the following formulas (only the main terms of the asymptotic expansions are given):

Integral representations

The differentiated gamma functions , , , and can also be represented through the following equivalent integrals:

Transformations

The following formulas describe some of the transformations that change the differentiated gamma functions into themselves:

Transformations with arguments that are integer multiples take the following forms:

The following transformations represent summation theorems:

Identities

The differentiated gamma functions , , , and satisfy the following recurrence identities:

The previous formulas can be generalized to the following recurrence identities with a jump of length :

Representations of derivatives

The derivatives of the differentiated gamma functions , , , and have rather simple representations:

The corresponding symbolic -order derivatives of all the differentiated gamma functions , , , and can be expressed by the following formulas:

Applications of differentiated gamma functions

Applications of differentiated gamma functions include discrete mathematics, number theory, and calculus.