DLMF:18.12.E6 (Q5648)

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DLMF:18.12.E6
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    Γ ( λ + 1 2 ) e z cos θ ( 1 2 z sin θ ) 1 2 - λ J λ - 1 2 ( z sin θ ) = n = 0 C n ( λ ) ( cos θ ) ( 2 λ ) n z n , Euler-Gamma 𝜆 1 2 superscript 𝑒 𝑧 𝜃 superscript 1 2 𝑧 𝜃 1 2 𝜆 Bessel-J 𝜆 1 2 𝑧 𝜃 superscript subscript 𝑛 0 ultraspherical-Gegenbauer-polynomial 𝜆 𝑛 𝜃 Pochhammer 2 𝜆 𝑛 superscript 𝑧 𝑛 {\displaystyle{\displaystyle\Gamma\left(\lambda+\tfrac{1}{2}\right)e^{z\cos% \theta}(\tfrac{1}{2}z\sin\theta)^{\frac{1}{2}-\lambda}J_{\lambda-\frac{1}{2}}% \left(z\sin\theta\right)=\sum_{n=0}^{\infty}\frac{C^{(\lambda)}_{n}\left(\cos% \theta\right)}{{\left(2\lambda\right)_{n}}}z^{n},}}
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    DLMF:18.12.E6
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    0 θ π 0 𝜃 𝜋 {\displaystyle{\displaystyle 0\leq\theta\leq\pi}}
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    J ν ( z ) Bessel-J 𝜈 𝑧 {\displaystyle{\displaystyle J_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C10.S2.E2.m2aadec
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    Γ ( z ) Euler-Gamma 𝑧 {\displaystyle{\displaystyle\Gamma\left(\NVar{z}\right)}}
    C5.S2.E1.m2aadec
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    ( a ) n Pochhammer 𝑎 𝑛 {\displaystyle{\displaystyle{\left(\NVar{a}\right)_{\NVar{n}}}}}
    C5.S2.SS3.m1abdec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2adec
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    cos z 𝑧 {\displaystyle{\displaystyle\cos\NVar{z}}}
    C4.S14.E2.m2adec
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    e {\displaystyle{\displaystyle\mathrm{e}}}
    C4.S2.E11.m2adec
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    sin z 𝑧 {\displaystyle{\displaystyle\sin\NVar{z}}}
    C4.S14.E1.m2adec
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    C n ( λ ) ( x ) ultraspherical-Gegenbauer-polynomial 𝜆 𝑛 𝑥 {\displaystyle{\displaystyle C^{(\NVar{\lambda})}_{\NVar{n}}\left(\NVar{x}% \right)}}
    C18.S3.T1.t1.r3.m2abdec
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    z 𝑧 {\displaystyle{\displaystyle z}}
    C18.S1.XMD2.m1edec
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