DLMF:11.4.E18 (Q3950)

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DLMF:11.4.E18
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    𝐇 ν ( z ) = 4 π 1 / 2 Γ ( ν + 1 2 ) k = 0 ( 2 k + ν + 1 ) Γ ( k + ν + 1 ) k ! ( 2 k + 1 ) ( 2 k + 2 ν + 1 ) J 2 k + ν + 1 ( z ) , Struve-H 𝜈 𝑧 4 superscript 𝜋 1 2 Euler-Gamma 𝜈 1 2 superscript subscript 𝑘 0 2 𝑘 𝜈 1 Euler-Gamma 𝑘 𝜈 1 𝑘 2 𝑘 1 2 𝑘 2 𝜈 1 Bessel-J 2 𝑘 𝜈 1 𝑧 {\displaystyle{\displaystyle\mathbf{H}_{\nu}\left(z\right)=\frac{4}{\pi^{1/2}% \Gamma\left(\nu+\tfrac{1}{2}\right)}\*\sum_{k=0}^{\infty}\frac{(2k+\nu+1)% \Gamma\left(k+\nu+1\right)}{k!(2k+1)(2k+2\nu+1)}J_{2k+\nu+1}\left(z\right),}}
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    DLMF:11.4.E18
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    ν - 1 , - 2 , - 3 , 𝜈 1 2 3 {\displaystyle{\displaystyle\nu\neq-1,-2,-3,\dots}}
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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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    𝐇 ν ( z ) Struve-H 𝜈 𝑧 {\displaystyle{\displaystyle\mathbf{H}_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C11.S2.E1.m2ahdec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2amdec
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    ! {\displaystyle{\displaystyle!}}
    introduction.Sx4.p1.t1.r15.m5abdec
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    z 𝑧 {\displaystyle{\displaystyle z}}
    C11.S1.XMD2.m1pdec
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    ν 𝜈 {\displaystyle{\displaystyle\nu}}
    C11.S1.XMD3.m1edec
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    k 𝑘 {\displaystyle{\displaystyle k}}
    C11.S1.XMD5.m1dec
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