DLMF:10.22.E23 (Q3397)

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DLMF:10.22.E23
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    0 1 2 π J μ ( z sin 2 θ ) J ν ( z cos 2 θ ) ( sin θ ) 2 α - 1 sec θ d θ = ( μ + ν + α ) Γ ( μ + α ) 2 α - 1 ν Γ ( μ + 1 ) z α J μ + ν + α ( z ) , superscript subscript 0 1 2 𝜋 Bessel-J 𝜇 𝑧 2 𝜃 Bessel-J 𝜈 𝑧 2 𝜃 superscript 𝜃 2 𝛼 1 𝜃 𝜃 𝜇 𝜈 𝛼 Euler-Gamma 𝜇 𝛼 superscript 2 𝛼 1 𝜈 Euler-Gamma 𝜇 1 superscript 𝑧 𝛼 Bessel-J 𝜇 𝜈 𝛼 𝑧 {\displaystyle{\displaystyle\int_{0}^{\frac{1}{2}\pi}J_{\mu}\left(z{\sin^{2}}% \theta\right)J_{\nu}\left(z{\cos^{2}}\theta\right)(\sin\theta)^{2\alpha-1}\sec% \theta\mathrm{d}\theta=\frac{(\mu+\nu+\alpha)\Gamma\left(\mu+\alpha\right)2^{% \alpha-1}}{\nu\Gamma\left(\mu+1\right)z^{\alpha}}J_{\mu+\nu+\alpha}\left(z% \right),}}
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    DLMF:10.22.E23
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    ( μ + α ) > 0 𝜇 𝛼 0 {\displaystyle{\displaystyle\Re(\mu+\alpha)>0}}
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    ν > 0 𝜈 0 {\displaystyle{\displaystyle\Re\nu>0}}
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    J ν ( z ) Bessel-J 𝜈 𝑧 {\displaystyle{\displaystyle J_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C10.S2.E2.m2aodec
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    Γ ( z ) Euler-Gamma 𝑧 {\displaystyle{\displaystyle\Gamma\left(\NVar{z}\right)}}
    C5.S2.E1.m2afdec
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