DLMF:28.22.E5 (Q8370)

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DLMF:28.22.E5
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    g e , 2 m ( h ) = ( - 1 ) m 2 π ce 2 m ( 1 2 π , h 2 ) A 0 2 m ( h 2 ) , subscript 𝑔 𝑒 2 𝑚 superscript 1 𝑚 2 𝜋 Mathieu-ce 2 𝑚 1 2 𝜋 superscript 2 superscript subscript 𝐴 0 2 𝑚 superscript 2 {\displaystyle{\displaystyle g_{\mathit{e},2m}(h)=(-1)^{m}\sqrt{\dfrac{2}{\pi}% }\dfrac{\mathrm{ce}_{2m}\left(\frac{1}{2}\pi,h^{2}\right)}{A_{0}^{2m}(h^{2})},}}
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