DLMF:10.22.E22 (Q3396)

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DLMF:10.22.E22
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    0 1 2 π J μ ( z sin 2 θ ) J ν ( z cos 2 θ ) ( sin θ ) 2 μ + 1 ( cos θ ) 2 ν + 1 d θ = Γ ( μ + 1 2 ) Γ ( ν + 1 2 ) J μ + ν + 1 2 ( z ) ( 8 π z ) 1 2 Γ ( μ + ν + 1 ) , superscript subscript 0 1 2 𝜋 Bessel-J 𝜇 𝑧 2 𝜃 Bessel-J 𝜈 𝑧 2 𝜃 superscript 𝜃 2 𝜇 1 superscript 𝜃 2 𝜈 1 𝜃 Euler-Gamma 𝜇 1 2 Euler-Gamma 𝜈 1 2 Bessel-J 𝜇 𝜈 1 2 𝑧 superscript 8 𝜋 𝑧 1 2 Euler-Gamma 𝜇 𝜈 1 {\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\mu+1}(\cos% \theta)^{2\nu+1}\mathrm{d}\theta=\frac{\Gamma\left(\mu+\tfrac{1}{2}\right)% \Gamma\left(\nu+\tfrac{1}{2}\right)J_{\mu+\nu+\frac{1}{2}}\left(z\right)}{(8% \pi z)^{\frac{1}{2}}\Gamma\left(\mu+\nu+1\right)},}}
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    DLMF:10.22.E22
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    μ > - 1 2 , ν > - 1 2 formulae-sequence 𝜇 1 2 𝜈 1 2 {\displaystyle{\displaystyle\Re\mu>-\tfrac{1}{2},\Re\nu>-\tfrac{1}{2}}}
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    J ν ( z ) Bessel-J 𝜈 𝑧 {\displaystyle{\displaystyle J_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C10.S2.E2.m2andec
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