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28 Mathieu Functions and Hill’s EquationModified Mathieu Functions

§28.25 Asymptotic Expansions for Large \realpart{z}

For fixed h(\neq 0) and fixed \nu,

28.25.1\mathop{{\mathrm{M}^{{(3,4)}}_{{\nu}}}\/}\nolimits\!\left(z,h\right)\sim\frac{%
e^{{\pm i\left(2h\mathop{\cosh\/}\nolimits z-\left(\frac{1}{2}\nu+\frac{1}{4}%
\right)\pi\right)}}}{\left(\pi h(\mathop{\cosh\/}\nolimits z+1)\right)^{{\frac%
{1}{2}}}}\*\sum_{{m=0}}^{{\infty}}\dfrac{D^{{\pm}}_{m}}{\left(\mp 4ih(\mathop{%
\cosh\/}\nolimits z+1)\right)^{m}},

where the coefficients are given by

28.25.2
D_{{-1}}^{{\pm}}=0,
D_{{0}}^{{\pm}}=1,

and

28.25.3(m+1)D^{{\pm}}_{{m+1}}+{\left((m+\tfrac{1}{2})^{2}\pm(m+\tfrac{1}{4})8ih+2h^{2%
}-a\right)D^{{\pm}}_{m}}\pm(m-\tfrac{1}{2})\left(8ihm\right)D_{{m-1}}^{{\pm}}=0,m\geq 0.

The upper signs correspond to \mathop{{\mathrm{M}^{{(3)}}_{{\nu}}}\/}\nolimits\!\left(z,h\right) and the lower signs to \mathop{{\mathrm{M}^{{(4)}}_{{\nu}}}\/}\nolimits\!\left(z,h\right). The expansion (28.25.1) is valid for \mathop{{\mathrm{M}^{{(3)}}_{{\nu}}}\/}\nolimits\!\left(z,h\right) when

and for \mathop{{\mathrm{M}^{{(4)}}_{{\nu}}}\/}\nolimits\!\left(z,h\right) when

where \delta again denotes an arbitrary small positive constant.

For proofs and generalizations see Meixner and Schäfke (1954, §2.63).