DLMF:10.22.E55 (Q3429)

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DLMF:10.22.E55
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    0 t - 1 J ν + 2 + 1 ( t ) J ν + 2 m + 1 ( t ) d t = δ , m 2 ( 2 + ν + 1 ) , superscript subscript 0 superscript 𝑡 1 Bessel-J 𝜈 2 1 𝑡 Bessel-J 𝜈 2 𝑚 1 𝑡 𝑡 Kronecker 𝑚 2 2 𝜈 1 {\displaystyle{\displaystyle\int_{0}^{\infty}t^{-1}J_{\nu+2\ell+1}\left(t% \right)J_{\nu+2m+1}\left(t\right)\mathrm{d}t=\frac{\delta_{\ell,m}}{2(2\ell+% \nu+1)},}}
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    DLMF:10.22.E55
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    ν + + m > - 1 𝜈 𝑚 1 {\displaystyle{\displaystyle\nu+\ell+m>-1}}
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    J ν ( z ) Bessel-J 𝜈 𝑧 {\displaystyle{\displaystyle J_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C10.S2.E2.m2aaodec
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    δ j , k Kronecker 𝑗 𝑘 {\displaystyle{\displaystyle\delta_{\NVar{j},\NVar{k}}}}
    introduction.Sx4.p1.t1.r4.m5abdec
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    d x 𝑥 {\displaystyle{\displaystyle\mathrm{d}\NVar{x}}}
    C1.S4.SS4.m1abbdec
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    {\displaystyle{\displaystyle\int}}
    C1.S4.SS4.m3abbdec
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