DLMF:33.16.E11 (Q9639)

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DLMF:33.16.E11
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    Statements

    h ( ϵ , ; r ) = ( - 1 ) ν + 1 A ( ϵ , ) ( sin ( π ν ) ζ ( ν , r ) Γ ( + 1 + ν ) + cos ( π ν ) Γ ( ν - ) ξ ( ν , r ) π ) . Coulomb-h italic-ϵ 𝑟 superscript 1 superscript 𝜈 1 𝐴 italic-ϵ 𝜋 𝜈 subscript 𝜁 𝜈 𝑟 Euler-Gamma 1 𝜈 𝜋 𝜈 Euler-Gamma 𝜈 subscript 𝜉 𝜈 𝑟 𝜋 {\displaystyle{\displaystyle h\left(\epsilon,\ell;r\right)=(-1)^{\ell}\nu^{% \ell+1}A(\epsilon,\ell)\left(\frac{\sin\left(\pi\nu\right)\zeta_{\ell}(\nu,r)}% {\Gamma\left(\ell+1+\nu\right)}+\frac{\cos\left(\pi\nu\right)\Gamma\left(\nu-% \ell\right)\xi_{\ell}(\nu,r)}{\pi}\right).}}
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    DLMF:33.16.E11
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    h ( ϵ , ; r ) Coulomb-h italic-ϵ 𝑟 {\displaystyle{\displaystyle h\left(\NVar{\epsilon},\NVar{\ell};\NVar{r}\right% )}}
    C33.S14.E7.m2acdec
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    Γ ( z ) Euler-Gamma 𝑧 {\displaystyle{\displaystyle\Gamma\left(\NVar{z}\right)}}
    C5.S2.E1.m2aadec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2agdec
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    cos z 𝑧 {\displaystyle{\displaystyle\cos\NVar{z}}}
    C4.S14.E2.m2aadec
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    sin z 𝑧 {\displaystyle{\displaystyle\sin\NVar{z}}}
    C4.S14.E1.m2aadec
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    {\displaystyle{\displaystyle\ell}}
    C33.S1.XMD2.m1hdec
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    r 𝑟 {\displaystyle{\displaystyle r}}
    C33.S1.XMD3.m1fdec
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    ϵ italic-ϵ {\displaystyle{\displaystyle\epsilon}}
    C33.S1.XMD6.m1gdec
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    A ( ϵ , ) 𝐴 italic-ϵ {\displaystyle{\displaystyle A(\epsilon,\ell)}}
    C33.S14.XMD4.m1ddec
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    ν 𝜈 {\displaystyle{\displaystyle\nu}}
    C33.S16.XMD2.m1cdec
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    ζ ( ν , r ) subscript 𝜁 𝜈 𝑟 {\displaystyle{\displaystyle\zeta_{\ell}(\nu,r)}}
    C33.S16.XMD3.m1bdec
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    ξ ( ν , r ) subscript 𝜉 𝜈 𝑟 {\displaystyle{\displaystyle\xi_{\ell}(\nu,r)}}
    C33.S16.XMD4.m1bdec
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