DLMF:10.54.E4 (Q3762)

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DLMF:10.54.E4
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    𝗃 n ( z ) = ( - i ) n + 1 2 π i ( - 1 + , 1 + ) e i z t Q n ( t ) d t , spherical-Bessel-J 𝑛 𝑧 superscript 𝑖 𝑛 1 2 𝜋 superscript subscript 𝑖 limit-from 1 limit-from 1 superscript 𝑒 𝑖 𝑧 𝑡 shorthand-Legendre-Q-second-kind 𝑛 𝑡 𝑡 {\displaystyle{\displaystyle\mathsf{j}_{n}\left(z\right)=\frac{(-i)^{n+1}}{2% \pi}\int_{i\infty}^{(-1+,1+)}e^{izt}Q_{n}\left(t\right)\mathrm{d}t,}}
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    DLMF:10.54.E4
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    | ph z | < 1 2 π . phase 𝑧 1 2 𝜋 {\displaystyle{\displaystyle|\operatorname{ph}z|<\tfrac{1}{2}\pi.}}
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2acdec
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    d x 𝑥 {\displaystyle{\displaystyle\mathrm{d}\NVar{x}}}
    C1.S4.SS4.m1acdec
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    e {\displaystyle{\displaystyle\mathrm{e}}}
    C4.S2.E11.m2abdec
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    i imaginary-unit {\displaystyle{\displaystyle\mathrm{i}}}
    C1.S9.E1.m2aadec
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    {\displaystyle{\displaystyle\int}}
    C1.S4.SS4.m3acdec
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    ( a , b ) 𝑎 𝑏 {\displaystyle{\displaystyle(\NVar{a},\NVar{b})}}
    introduction.Sx4.p1.t1.r29.m6adec
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    ph phase {\displaystyle{\displaystyle\operatorname{ph}}}
    C1.S9.E7.m1aadec
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    Q ν ( z ) = Q ν 0 ( z ) shorthand-Legendre-Q-second-kind 𝜈 𝑧 Legendre-Q-second-kind 0 𝜈 𝑧 {\displaystyle{\displaystyle Q_{\NVar{\nu}}\left(\NVar{z}\right)=Q^{0}_{\nu}% \left(z\right)}}
    C14.S2.SS2.p2.m5adec
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    𝗃 n ( z ) spherical-Bessel-J 𝑛 𝑧 {\displaystyle{\displaystyle\mathsf{j}_{\NVar{n}}\left(\NVar{z}\right)}}
    C10.S47.E3.m2abdec
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    n 𝑛 {\displaystyle{\displaystyle n}}
    C10.S1.XMD2.m1cdec
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    z 𝑧 {\displaystyle{\displaystyle z}}
    C10.S1.XMD6.m1cdec
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