DLMF:10.22.E54 (Q3428)

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DLMF:10.22.E54
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    0 J ν ( b t ) exp ( - p 2 t 2 ) t μ - 1 d t = ( 1 2 b / p ) ν Γ ( 1 2 ν + 1 2 μ ) 2 p μ exp ( - b 2 4 p 2 ) 𝐌 ( 1 2 ν - 1 2 μ + 1 , ν + 1 , b 2 4 p 2 ) , superscript subscript 0 Bessel-J 𝜈 𝑏 𝑡 superscript 𝑝 2 superscript 𝑡 2 superscript 𝑡 𝜇 1 𝑡 superscript 1 2 𝑏 𝑝 𝜈 Euler-Gamma 1 2 𝜈 1 2 𝜇 2 superscript 𝑝 𝜇 superscript 𝑏 2 4 superscript 𝑝 2 Kummer-confluent-hypergeometric-bold-M 1 2 𝜈 1 2 𝜇 1 𝜈 1 superscript 𝑏 2 4 superscript 𝑝 2 {\displaystyle{\displaystyle\int_{0}^{\infty}J_{\nu}\left(bt\right)\exp\left(-% p^{2}t^{2}\right)t^{\mu-1}\mathrm{d}t=\frac{(\tfrac{1}{2}b/p)^{\nu}\Gamma\left% (\tfrac{1}{2}\nu+\tfrac{1}{2}\mu\right)}{2p^{\mu}}\exp\left(-\frac{b^{2}}{4p^{% 2}}\right)\*{\mathbf{M}}\left(\tfrac{1}{2}\nu-\tfrac{1}{2}\mu+1,\nu+1,\frac{b^% {2}}{4p^{2}}\right),}}
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    DLMF:10.22.E54
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    ( μ + ν ) > 0 𝜇 𝜈 0 {\displaystyle{\displaystyle\Re(\mu+\nu)>0}}
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    ( p 2 ) > 0 superscript 𝑝 2 0 {\displaystyle{\displaystyle\Re(p^{2})>0}}
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    J ν ( z ) Bessel-J 𝜈 𝑧 {\displaystyle{\displaystyle J_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C10.S2.E2.m2aandec
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    Γ ( z ) Euler-Gamma 𝑧 {\displaystyle{\displaystyle\Gamma\left(\NVar{z}\right)}}
    C5.S2.E1.m2apdec
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