DLMF:28.10.E2 (Q8281)

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DLMF:28.10.E2
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    2 π 0 π / 2 cosh ( 2 h sin z sin t ) ce 2 n ( t , h 2 ) d t = A 0 2 n ( h 2 ) ce 2 n ( 0 , h 2 ) ce 2 n ( z , h 2 ) , 2 𝜋 superscript subscript 0 𝜋 2 2 𝑧 𝑡 Mathieu-ce 2 𝑛 𝑡 superscript 2 𝑡 superscript subscript 𝐴 0 2 𝑛 superscript 2 Mathieu-ce 2 𝑛 0 superscript 2 Mathieu-ce 2 𝑛 𝑧 superscript 2 {\displaystyle{\displaystyle\frac{2}{\pi}\int_{0}^{\ifrac{\pi}{2}}\cosh\left(2% h\sin z\sin t\right)\mathrm{ce}_{2n}\left(t,h^{2}\right)\mathrm{d}t=\frac{A_{0% }^{2n}(h^{2})}{\mathrm{ce}_{2n}\left(0,h^{2}\right)}\mathrm{ce}_{2n}\left(z,h^% {2}\right),}}
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    DLMF:28.10.E2
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    ce n ( z , q ) Mathieu-ce 𝑛 𝑧 𝑞 {\displaystyle{\displaystyle\mathrm{ce}_{\NVar{n}}\left(\NVar{z},\NVar{q}% \right)}}
    C28.S2.SS6.p1.m7aadec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2aadec
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    d x 𝑥 {\displaystyle{\displaystyle\mathrm{d}\NVar{x}}}
    C1.S4.SS4.m1aadec
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    cosh z 𝑧 {\displaystyle{\displaystyle\cosh\NVar{z}}}
    C4.S28.E2.m2adec
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    {\displaystyle{\displaystyle\int}}
    C1.S4.SS4.m3aadec
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    sin z 𝑧 {\displaystyle{\displaystyle\sin\NVar{z}}}
    C4.S14.E1.m2adec
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    h {\displaystyle{\displaystyle h}}
    C28.S1.XMD11.m1adec
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    n 𝑛 {\displaystyle{\displaystyle n}}
    C28.S1.XMD2.m1adec
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    z 𝑧 {\displaystyle{\displaystyle z}}
    C28.S1.XMD6.m1adec
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    A m ( q ) subscript 𝐴 𝑚 𝑞 {\displaystyle{\displaystyle A_{m}(q)}}
    C28.S4.XMD1.m1adec
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