DLMF:10.9.E24 (Q3094)

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DLMF:10.9.E24
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    H ν ( 1 ) ( z ) = - e - 1 2 ν π i 2 π 2 c - i c + i Γ ( t ) Γ ( t - ν ) ( - 1 2 i z ) ν - 2 t d t , Hankel-H-1-Bessel-third-kind 𝜈 𝑧 superscript 𝑒 1 2 𝜈 𝜋 𝑖 2 superscript 𝜋 2 superscript subscript 𝑐 𝑖 𝑐 𝑖 Euler-Gamma 𝑡 Euler-Gamma 𝑡 𝜈 superscript 1 2 𝑖 𝑧 𝜈 2 𝑡 𝑡 {\displaystyle{\displaystyle{H^{(1)}_{\nu}}\left(z\right)=-\frac{e^{-\frac{1}{% 2}\nu\pi i}}{2\pi^{2}}\*\int_{c-i\infty}^{c+i\infty}\Gamma\left(t\right)\Gamma% \left(t-\nu\right)(-\tfrac{1}{2}iz)^{\nu-2t}\mathrm{d}t,}}
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    DLMF:10.9.E24
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    0 < ph z < π 0 phase 𝑧 𝜋 {\displaystyle{\displaystyle 0<\operatorname{ph}z<\pi}}
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    Γ ( z ) Euler-Gamma 𝑧 {\displaystyle{\displaystyle\Gamma\left(\NVar{z}\right)}}
    C5.S2.E1.m2agdec
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    H ν ( 1 ) ( z ) Hankel-H-1-Bessel-third-kind 𝜈 𝑧 {\displaystyle{\displaystyle{H^{(1)}_{\NVar{\nu}}}\left(\NVar{z}\right)}}
    C10.S2.E5.m2addec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2awdec
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    d x 𝑥 {\displaystyle{\displaystyle\mathrm{d}\NVar{x}}}
    C1.S4.SS4.m1awdec
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    e {\displaystyle{\displaystyle\mathrm{e}}}
    C4.S2.E11.m2amdec
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