DLMF:10.16.E7 (Q3166)

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DLMF:10.16.E7
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    J ν ( z ) = e ( 2 ν + 1 ) π i / 4 2 2 ν Γ ( ν + 1 ) ( 2 z ) - 1 2 M 0 , ν ( ± 2 i z ) , Bessel-J 𝜈 𝑧 superscript 𝑒 minus-or-plus 2 𝜈 1 𝜋 𝑖 4 superscript 2 2 𝜈 Euler-Gamma 𝜈 1 superscript 2 𝑧 1 2 Whittaker-confluent-hypergeometric-M 0 𝜈 plus-or-minus 2 𝑖 𝑧 {\displaystyle{\displaystyle J_{\nu}\left(z\right)=\frac{e^{\mp(2\nu+1)\pi i/4% }}{2^{2\nu}\Gamma\left(\nu+1\right)}(2z)^{-\frac{1}{2}}M_{0,\nu}\left(\pm 2iz% \right),}}
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    DLMF:10.16.E7
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    2 ν - 1 , - 2 , - 3 , 2 𝜈 1 2 3 {\displaystyle{\displaystyle 2\nu\neq-1,-2,-3,\ldots}}
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    J ν ( z ) Bessel-J 𝜈 𝑧 {\displaystyle{\displaystyle J_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C10.S2.E2.m2addec
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    Γ ( z ) Euler-Gamma 𝑧 {\displaystyle{\displaystyle\Gamma\left(\NVar{z}\right)}}
    C5.S2.E1.m2aadec
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    M κ , μ ( z ) Whittaker-confluent-hypergeometric-M 𝜅 𝜇 𝑧 {\displaystyle{\displaystyle M_{\NVar{\kappa},\NVar{\mu}}\left(\NVar{z}\right)}}
    C13.S14.E2.m2adec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2aedec
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    e {\displaystyle{\displaystyle\mathrm{e}}}
    C4.S2.E11.m2acdec
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    i imaginary-unit {\displaystyle{\displaystyle\mathrm{i}}}
    C1.S9.E1.m2acdec
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    z 𝑧 {\displaystyle{\displaystyle z}}
    C10.S1.XMD6.m1fdec
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    ν 𝜈 {\displaystyle{\displaystyle\nu}}
    C10.S1.XMD7.m1bdec
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