DLMF:10.9.E22 (Q3092)

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DLMF:10.9.E22
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    J ν ( x ) = 1 2 π i - i i Γ ( - t ) ( 1 2 x ) ν + 2 t Γ ( ν + t + 1 ) d t , Bessel-J 𝜈 𝑥 1 2 𝜋 𝑖 superscript subscript 𝑖 𝑖 Euler-Gamma 𝑡 superscript 1 2 𝑥 𝜈 2 𝑡 Euler-Gamma 𝜈 𝑡 1 𝑡 {\displaystyle{\displaystyle J_{\nu}\left(x\right)=\frac{1}{2\pi i}\int_{-i% \infty}^{i\infty}\frac{\Gamma\left(-t\right)(\tfrac{1}{2}x)^{\nu+2t}}{\Gamma% \left(\nu+t+1\right)}\mathrm{d}t,}}
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    DLMF:10.9.E22
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    ν > 0 𝜈 0 {\displaystyle{\displaystyle\Re\nu>0}}
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    ν > 0 𝜈 0 {\displaystyle{\displaystyle\Re\nu>0}}
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