DLMF:28.28.E26 (Q8453)

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DLMF:28.28.E26
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    cosh z π 2 0 2 π sin t me ν ( t , h 2 ) me - ν - 2 m - 1 ( t , h 2 ) sinh 2 z + sin 2 t d t = ( - 1 ) m + 1 i h α ν , m ( 1 ) D 0 ( ν , ν + 2 m + 1 , z ) , 𝑧 superscript 𝜋 2 superscript subscript 0 2 𝜋 𝑡 Mathieu-me 𝜈 𝑡 superscript 2 Mathieu-me 𝜈 2 𝑚 1 𝑡 superscript 2 2 𝑧 2 𝑡 𝑡 superscript 1 𝑚 1 imaginary-unit subscript superscript 𝛼 1 𝜈 𝑚 Mathieu-D 0 𝜈 𝜈 2 𝑚 1 𝑧 {\displaystyle{\displaystyle\dfrac{\cosh z}{\pi^{2}}\int_{0}^{2\pi}\dfrac{\sin t% \mathrm{me}_{\nu}\left(t,h^{2}\right)\mathrm{me}_{-\nu-2m-1}\left(t,h^{2}% \right)}{{\sinh^{2}}z+{\sin^{2}}t}\mathrm{d}t=(-1)^{m+1}\mathrm{i}h\alpha^{(1)% }_{\nu,m}\mathrm{D}_{0}\left(\nu,\nu+2m+1,z\right),}}
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    DLMF:28.28.E26
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    D j ( ν , μ , z ) Mathieu-D 𝑗 𝜈 𝜇 𝑧 {\displaystyle{\displaystyle\mathrm{D}_{\NVar{j}}\left(\NVar{\nu},\NVar{\mu},% \NVar{z}\right)}}
    C28.S28.E24.m1abdec
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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.m2aedec
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