Introduction to the Struve functions
General
The Struve functions and appeared as special solutions of the inhomogeneous Bessel secondorder differential equations:
where and are arbitrary constants and , , , and are Bessel functions.
The last two differential equations are very similar and can be converted into each other by changing to . Their solutions can be constructed in the form of a series with arbitrary coefficients:
Substitution of this series into the first equation gives the following partial solution of the inhomogeneous equation:
This solution, which appeared in an article by H. Struve (1882), was later ascribed Struve's name and the special notation .
A similar procedure carried out for the second inhomogeneous equation leads to the function , which was introduced by J. W. Nicholson (1911).
Definitions of Struve functions
The Struve functions and are defined as sums of the following infinite series:
A quick look at the Struve functions Here is a quick look at the graphics for the Struve functions along the real axis.
Connections within the group of Struve functions and with other function groups
Representations through more general functions
The Struve functions and are particular cases of the more general hypergeometric and Meijer G functions.
For example, they can be represented through regularized hypergeometric functions :
In the cases when , the previous formulas degenerate into the following:
For general values of parameter , the Struve functions and cannot be represented through classical hypergeometric functions without restrictions on parameter :
Similar conclusion can be drawn from the following representations of the Struve functions and through generalized and classical Meijer G functions:
The first two formulas are simpler than the last two classical representations that include factors like .
Transformation inside the group (Interconnections)
The Struve functions and are connected to each other by the formulas:
The bestknown properties and formulas for Struve functions
Real values for real arguments
For real values of parameter and positive argument , the values of the Struve functions and are real.
Simple values at zero
The Struve functions and have rather simple values for the argument :
Specific values for specialized parameter
In the cases when parameter is equal to , the Struve functions and can be expressed through the sine and cosine (or hyperbolic sine and cosine) multiplied by rational and sqrt functions, for example:
The previous formulas are the particular cases of the following general formulas:
Analyticity
The Struve functions and are defined for all complex values of their parameter and variable . They are analytical functions of and over the whole complex ‐ and ‐planes excluding the branch cuts. For fixed integer , the functions and are entire functions of . For fixed , the functions and are entire functions of .
Poles and essential singularities
For fixed , the functions and have an essential singularity at . At the same time, the point is a branch point (except cases for integer ).
With respect to , the Struve functions have only one essential singular point at .
Branch points and branch cuts.
For fixed noninteger , the functions and have two branch points: and .
If functions and have branch cuts, they are single‐valued functions on the ‐plane cut along the interval , where they are continuous from above:
From below, functions have discontinuities that are described by the formulas:
Periodicity
The Struve functions and do not have periodicity.
Parity and symmetry
The Struve functions and have mirror symmetry (except on the branch cut interval (∞, 0)):
The Struve functions and have generalized parity (either odd or even) with respect to variable :
Series representations
The Struve functions and have the following series expansions through series that converge on the whole ‐plane:
Interestingly, closedform expressions for the truncated version of the Taylor series at the origin can be expressed through the generalized hypergeometric function , for example:
Asymptotic series expansions
The asymptotic behavior of the Struve functions and can be described by the following formulas (only the main terms of asymptotic expansion are given):
The previous formulas are valid in any directions approaching point to infinity (z∞). In particular cases when or , these formulas can be simplified to the following relations:
Integral representations
The Struve functions and have simple integral representations through the sine (or hyperbolic sine) and power functions:
Transformations
Arguments of the Struve functions and with square root arguments can sometimes be simplified:
Identities
The Struve functions and satisfy the following recurrence identities:
The previous identities can be generalized to the following recurrence identities with a jump of length n:
Simple representations of derivatives
The derivatives of the Struve functions and have simple representations that can also be expressed through Struve functions with different indices:
The symbolic order derivatives have the following representations:
Differential equations
The Struve functions and appeared as special solutions of the special inhomogeneous Bessel secondorder linear differential equations:
where and are arbitrary constants and , , , and are Bessel functions.
The previous equations are very similar and can be converted into each other by changing to .
Applications of Struve functions
Applications of Struve functions include electrodynamics, potential theory, and optics.
