DLMF:11.10.E19 (Q4037)

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DLMF:11.10.E19
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    𝐉 - 1 2 ( z ) = 𝐄 1 2 ( z ) = ( 1 2 π z ) - 1 2 ( A + ( χ ) cos z - A - ( χ ) sin z ) , Anger-J 1 2 𝑧 Weber-E 1 2 𝑧 superscript 1 2 𝜋 𝑧 1 2 subscript 𝐴 𝜒 𝑧 subscript 𝐴 𝜒 𝑧 {\displaystyle{\displaystyle\mathbf{J}_{-\frac{1}{2}}\left(z\right)=\mathbf{E}% _{\frac{1}{2}}\left(z\right)\\ =(\tfrac{1}{2}\pi z)^{-\frac{1}{2}}(A_{+}(\chi)\cos z-A_{-}(\chi)\sin z),}}
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    DLMF:11.10.E19
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    𝐉 ν ( z ) Anger-J 𝜈 𝑧 {\displaystyle{\displaystyle\mathbf{J}_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C11.S10.E1.m2akdec
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    𝐄 ν ( z ) Weber-E 𝜈 𝑧 {\displaystyle{\displaystyle\mathbf{E}_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C11.S10.E2.m2akdec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2andec
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    cos z 𝑧 {\displaystyle{\displaystyle\cos\NVar{z}}}
    C4.S14.E2.m2aidec
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    sin z 𝑧 {\displaystyle{\displaystyle\sin\NVar{z}}}
    C4.S14.E1.m2ajdec
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    z 𝑧 {\displaystyle{\displaystyle z}}
    C11.S1.XMD2.m1rdec
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