DLMF:28.10.E3 (Q8282)

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DLMF:28.10.E3
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    2 π 0 π / 2 sin ( 2 h cos z cos t ) ce 2 n + 1 ( t , h 2 ) d t = - h A 1 2 n + 1 ( h 2 ) ce 2 n + 1 ( 1 2 π , h 2 ) ce 2 n + 1 ( z , h 2 ) , 2 𝜋 superscript subscript 0 𝜋 2 2 𝑧 𝑡 Mathieu-ce 2 𝑛 1 𝑡 superscript 2 𝑡 superscript subscript 𝐴 1 2 𝑛 1 superscript 2 diffop Mathieu-ce 2 𝑛 1 1 1 2 𝜋 superscript 2 Mathieu-ce 2 𝑛 1 𝑧 superscript 2 {\displaystyle{\displaystyle\frac{2}{\pi}\int_{0}^{\ifrac{\pi}{2}}\sin\left(2h% \cos z\cos t\right)\mathrm{ce}_{2n+1}\left(t,h^{2}\right)\mathrm{d}t=-\frac{hA% _{1}^{2n+1}(h^{2})}{\mathrm{ce}_{2n+1}'\left(\frac{1}{2}\pi,h^{2}\right)}% \mathrm{ce}_{2n+1}\left(z,h^{2}\right),}}
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    DLMF:28.10.E3
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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.m7abdec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2abdec
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