DLMF:28.23.E4 (Q8388)

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DLMF:28.23.E4
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    me ν ( 1 2 π , h 2 ) M ν ( j ) ( z , h ) = e i ν π / 2 n = - c 2 n ν ( h 2 ) 𝒞 ν + 2 n ( j ) ( 2 h sinh z ) , Mathieu-me 𝜈 1 2 𝜋 superscript 2 modified-Mathieu-M 𝑗 𝜈 𝑧 superscript 𝑒 imaginary-unit 𝜈 𝜋 2 superscript subscript 𝑛 superscript subscript 𝑐 2 𝑛 𝜈 superscript 2 superscript subscript 𝒞 𝜈 2 𝑛 𝑗 2 𝑧 {\displaystyle{\displaystyle\mathrm{me}_{\nu}\left(\tfrac{1}{2}\pi,h^{2}\right% ){\mathrm{M}^{(j)}_{\nu}}\left(z,h\right)=e^{\mathrm{i}\nu\ifrac{\pi}{2}}\sum_% {n=-\infty}^{\infty}c_{2n}^{\nu}(h^{2}){\cal C}_{\nu+2n}^{(j)}(2h\sinh z),}}
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    DLMF:28.23.E4
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    me n ( z , q ) Mathieu-me 𝑛 𝑧 𝑞 {\displaystyle{\displaystyle\mathrm{me}_{\NVar{n}}\left(\NVar{z},\NVar{q}% \right)}}
    C28.S12.SS2.p2.m2abdec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2adec
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    e {\displaystyle{\displaystyle\mathrm{e}}}
    C4.S2.E11.m2adec
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    sinh z 𝑧 {\displaystyle{\displaystyle\sinh\NVar{z}}}
    C4.S28.E1.m2adec
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    i imaginary-unit {\displaystyle{\displaystyle\mathrm{i}}}
    C1.S9.E1.m2aadec
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    M ν ( j ) ( z , h ) modified-Mathieu-M 𝑗 𝜈 𝑧 {\displaystyle{\displaystyle{\mathrm{M}^{(\NVar{j})}_{\NVar{\nu}}}\left(\NVar{% z},\NVar{h}\right)}}
    C28.S20.SS3.p1.m4abdec
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    h {\displaystyle{\displaystyle h}}
    C28.S1.XMD11.m1bdec
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    n 𝑛 {\displaystyle{\displaystyle n}}
    C28.S1.XMD2.m1bdec
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