DLMF:10.9.E17 (Q3085)

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DLMF:10.9.E17
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    Statements

    J ν ( z ) = 1 2 π i - π i + π i e z sinh t - ν t d t , Bessel-J 𝜈 𝑧 1 2 𝜋 𝑖 superscript subscript 𝜋 𝑖 𝜋 𝑖 superscript 𝑒 𝑧 𝑡 𝜈 𝑡 𝑡 {\displaystyle{\displaystyle J_{\nu}\left(z\right)=\frac{1}{2\pi i}\int_{% \infty-\pi i}^{\infty+\pi i}e^{z\sinh t-\nu t}\mathrm{d}t,}}
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    DLMF:10.9.E17
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    J ν ( z ) Bessel-J 𝜈 𝑧 {\displaystyle{\displaystyle J_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C10.S2.E2.m2ahdec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2apdec
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    d x 𝑥 {\displaystyle{\displaystyle\mathrm{d}\NVar{x}}}
    C1.S4.SS4.m1apdec
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    e {\displaystyle{\displaystyle\mathrm{e}}}
    C4.S2.E11.m2ajdec
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    sinh z 𝑧 {\displaystyle{\displaystyle\sinh\NVar{z}}}
    C4.S28.E1.m2afdec
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    i imaginary-unit {\displaystyle{\displaystyle\mathrm{i}}}
    C1.S9.E1.m2aedec
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    {\displaystyle{\displaystyle\int}}
    C1.S4.SS4.m3apdec
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    z 𝑧 {\displaystyle{\displaystyle z}}
    C10.S1.XMD6.m1mdec
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    ν 𝜈 {\displaystyle{\displaystyle\nu}}
    C10.S1.XMD7.m1ldec
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