DLMF:11.10.E14 (Q4032)

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DLMF:11.10.E14
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    Statements

    sin ( π ν ) 𝐄 ν ( z ) = 𝐉 - ν ( z ) - cos ( π ν ) 𝐉 ν ( z ) . 𝜋 𝜈 Weber-E 𝜈 𝑧 Anger-J 𝜈 𝑧 𝜋 𝜈 Anger-J 𝜈 𝑧 {\displaystyle{\displaystyle\sin\left(\pi\nu\right)\,\mathbf{E}_{\nu}\left(z% \right)=\mathbf{J}_{-\nu}\left(z\right)-\cos\left(\pi\nu\right)\,\mathbf{J}_{% \nu}\left(z\right).}}
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    DLMF:11.10.E14
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    𝐉 ν ( z ) Anger-J 𝜈 𝑧 {\displaystyle{\displaystyle\mathbf{J}_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C11.S10.E1.m2ahdec
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    𝐄 ν ( z ) Weber-E 𝜈 𝑧 {\displaystyle{\displaystyle\mathbf{E}_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C11.S10.E2.m2ahdec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2aidec
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    cos z 𝑧 {\displaystyle{\displaystyle\cos\NVar{z}}}
    C4.S14.E2.m2afdec
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    sin z 𝑧 {\displaystyle{\displaystyle\sin\NVar{z}}}
    C4.S14.E1.m2agdec
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    z 𝑧 {\displaystyle{\displaystyle z}}
    C11.S1.XMD2.m1mdec
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    ν 𝜈 {\displaystyle{\displaystyle\nu}}
    C11.S1.XMD3.m1qdec
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