Mathieu function

In mathematics, Mathieu functions are solutions of Mathieu's differential equation( p {displaystyle p} non-integral) In mathematics, Mathieu functions are solutions of Mathieu's differential equation where a {displaystyle a} and q {displaystyle q} are parameters. They were first introduced by Émile Léonard Mathieu, who encountered them while studying vibrating elliptical drumheads. They have applications in many fields of the physical sciences, such as optics, quantum mechanics, and general relativity. In general, they tend to occur in problems involving some sort of periodic motion or in the analysis of partial differential equation boundary value problems possessing elliptic symmetry. In some usages, Mathieu function refers to solutions of the Mathieu differential equation for arbitrary values of a {displaystyle a} and q {displaystyle q} . When no confusion can arise, other authors use Mathieu function to refer specifically to π {displaystyle pi } - or 2 π {displaystyle 2pi } -periodic solutions, which exist only for special values of a {displaystyle a} and q {displaystyle q} . More precisely, for given (real) q {displaystyle q} such periodic solutions exist for an infinite number of values of a {displaystyle a} , called characteristic numbers, conventionally indexed as two separate sequences a n ( q ) {displaystyle a_{n}(q)} and b n ( q ) {displaystyle b_{n}(q)} , for n = 1 , 2 , 3 , … {displaystyle n=1,2,3,ldots } . The corresponding functions are denoted ce n ( x , q ) {displaystyle { ext{ce}}_{n}(x,q)} and se n ( x , q ) {displaystyle { ext{se}}_{n}(x,q)} , respectively. They are sometimes also referred to as cosine-elliptic and sine-elliptic, or Mathieu functions of the first kind. As a result of assuming that q {displaystyle q} is real, both the characteristic numbers and associated functions are real-valued. ce n ( x , q ) {displaystyle { ext{ce}}_{n}(x,q)} and se n ( x , q ) {displaystyle { ext{se}}_{n}(x,q)} can be further classified by parity and periodicity (both with respect to x {displaystyle x} ), as follows: The indexing with the integer n {displaystyle n} , besides serving to arrange the characteristic numbers in ascending order, is convenient in that ce n ( x , q ) {displaystyle { ext{ce}}_{n}(x,q)} and se n ( x , q ) {displaystyle { ext{se}}_{n}(x,q)} become proportional to cos ⁡ n x {displaystyle cos nx} and sin ⁡ n x {displaystyle sin nx} as q → 0 {displaystyle q ightarrow 0} . With n {displaystyle n} being an integer, this gives rise to the classification of ce n {displaystyle { ext{ce}}_{n}} and se n {displaystyle { ext{se}}_{n}} as Mathieu functions (of the first kind) of integral order. For general a {displaystyle a} and q {displaystyle q} , solutions besides these can be defined, including Mathieu functions of fractional order as well as non-periodic solutions. Closely related are the modified Mathieu functions, which are solutions of Mathieu's modified differential equation which can be related to the original Mathieu equation by taking x → ± x i {displaystyle x o pm xi} . Accordingly, the modified Mathieu functions of the first kind of integral order, denoted by Ce n ( x , q ) {displaystyle { ext{Ce}}_{n}(x,q)} and Se n ( x , q ) {displaystyle { ext{Se}}_{n}(x,q)} , are defined from These functions are real-valued when x {displaystyle x} is real.