DLMF:1.17.E14 (Q673)

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DLMF:1.17.E14
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    Statements

    δ ( x - a ) = 2 x a π 0 t 2 𝗃 ( x t ) 𝗃 ( a t ) d t , Dirac-delta 𝑥 𝑎 2 𝑥 𝑎 𝜋 superscript subscript 0 superscript 𝑡 2 spherical-Bessel-J 𝑥 𝑡 spherical-Bessel-J 𝑎 𝑡 𝑡 {\displaystyle{\displaystyle\delta\left(x-a\right)=\frac{2xa}{\pi}\int_{0}^{% \infty}t^{2}\mathsf{j}_{\ell}\left(xt\right)\mathsf{j}_{\ell}\left(at\right)% \mathrm{d}t,}}
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    DLMF:1.17.E14
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    a > 0 𝑎 0 {\displaystyle{\displaystyle a>0}}
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    δ ( x - a ) Dirac-delta 𝑥 𝑎 {\displaystyle{\displaystyle\delta\left(\NVar{x-a}\right)}}
    C1.S17.SS1.p1.m2aedec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2ahdec
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    d x 𝑥 {\displaystyle{\displaystyle\mathrm{d}\NVar{x}}}
    C1.S4.SS4.m1ajdec
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    {\displaystyle{\displaystyle\int}}
    C1.S4.SS4.m3ajdec
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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.m2adec
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