DLMF:11.10.E27 (Q4049)

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DLMF:11.10.E27
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    ν 𝐉 ν ( z ) | ν = 0 = 1 2 π 𝐇 0 ( z ) , evaluated-at partial-derivative 𝜈 Anger-J 𝜈 𝑧 𝜈 0 1 2 𝜋 Struve-H 0 𝑧 {\displaystyle{\displaystyle\left.\frac{\partial}{\partial\nu}\mathbf{J}_{\nu}% \left(z\right)\right|_{\nu=0}=\tfrac{1}{2}\pi\mathbf{H}_{0}\left(z\right),}}
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    DLMF:11.10.E27
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    𝐉 ν ( z ) Anger-J 𝜈 𝑧 {\displaystyle{\displaystyle\mathbf{J}_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C11.S10.E1.m2andec
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    𝐇 ν ( z ) Struve-H 𝜈 𝑧 {\displaystyle{\displaystyle\mathbf{H}_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C11.S2.E1.m2acdec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2audec
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    f x partial-derivative 𝑓 𝑥 {\displaystyle{\displaystyle\frac{\partial\NVar{f}}{\partial\NVar{x}}}}
    C1.S5.E3.m4adec
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    x 𝑥 {\displaystyle{\displaystyle\partial\NVar{x}}}
    C1.S5.E3.m2adec
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    z 𝑧 {\displaystyle{\displaystyle z}}
    C11.S1.XMD2.m1xdec
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