DLMF:28.10.E9 (Q8288)

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DLMF:28.10.E9
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    0 π / 2 J 0 ( 2 q ( cos 2 τ - sin 2 ζ ) ) ce 2 n ( τ , q ) d τ = w II ( 1 2 π ; a 2 n ( q ) , q ) ce 2 n ( ζ , q ) , superscript subscript 0 𝜋 2 Bessel-J 0 2 𝑞 2 𝜏 2 𝜁 Mathieu-ce 2 𝑛 𝜏 𝑞 𝜏 subscript 𝑤 II 1 2 𝜋 Mathieu-eigenvalue-a 2 𝑛 𝑞 𝑞 Mathieu-ce 2 𝑛 𝜁 𝑞 {\displaystyle{\displaystyle\int_{0}^{\ifrac{\pi}{2}}J_{0}\left(2\sqrt{q({\cos% ^{2}}\tau-{\sin^{2}}\zeta)}\right)\mathrm{ce}_{2n}\left(\tau,q\right)\mathrm{d% }\tau=w_{\mbox{\tiny II}}(\tfrac{1}{2}\pi;a_{2n}\left(q\right),q)\mathrm{ce}_{% 2n}\left(\zeta,q\right),}}
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    DLMF:28.10.E9
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    J ν ( z ) Bessel-J 𝜈 𝑧 {\displaystyle{\displaystyle J_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C10.S2.E2.m2adec
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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.m7addec
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    a n ( q ) Mathieu-eigenvalue-a 𝑛 𝑞 {\displaystyle{\displaystyle a_{\NVar{n}}\left(\NVar{q}\right)}}
    C28.S2.SS5.p1.m3adec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2ahdec
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    cos z 𝑧 {\displaystyle{\displaystyle\cos\NVar{z}}}
    C4.S14.E2.m2afdec
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    d x 𝑥 {\displaystyle{\displaystyle\mathrm{d}\NVar{x}}}
    C1.S4.SS4.m1ahdec
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    {\displaystyle{\displaystyle\int}}
    C1.S4.SS4.m3ahdec
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    sin z 𝑧 {\displaystyle{\displaystyle\sin\NVar{z}}}
    C4.S14.E1.m2agdec
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    q = h 2 𝑞 superscript 2 {\displaystyle{\displaystyle q=h^{2}}}
    C28.S1.XMD10.m1dec
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    n 𝑛 {\displaystyle{\displaystyle n}}
    C28.S1.XMD2.m1hdec
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