DLMF:11.10.E17 (Q4035)

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DLMF:11.10.E17
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    𝐉 ν ( z ) = sin ( π ν ) π ( s 0 , ν ( z ) - ν s - 1 , ν ( z ) ) , Anger-J 𝜈 𝑧 𝜋 𝜈 𝜋 Lommel-s 0 𝜈 𝑧 𝜈 Lommel-s 1 𝜈 𝑧 {\displaystyle{\displaystyle\mathbf{J}_{\nu}\left(z\right)=\frac{\sin\left(\pi% \nu\right)}{\pi}(s_{{0},{\nu}}\left(z\right)-\nu s_{{-1},{\nu}}\left(z\right))% ,}}
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    DLMF:11.10.E17
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    𝐉 ν ( z ) Anger-J 𝜈 𝑧 {\displaystyle{\displaystyle\mathbf{J}_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C11.S10.E1.m2ajdec
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    s μ , ν ( z ) Lommel-s 𝜇 𝜈 𝑧 {\displaystyle{\displaystyle s_{{\NVar{\mu}},{\NVar{\nu}}}\left(\NVar{z}\right% )}}
    C11.S9.E3.m2adec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2aldec
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    sin z 𝑧 {\displaystyle{\displaystyle\sin\NVar{z}}}
    C4.S14.E1.m2aidec
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    z 𝑧 {\displaystyle{\displaystyle z}}
    C11.S1.XMD2.m1pdec
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