DLMF:11.7.E12 (Q4002)

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DLMF:11.7.E12
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    0 t - μ - ν 𝐇 μ ( t ) 𝐇 ν ( t ) d t = π Γ ( μ + ν ) 2 μ + ν Γ ( μ + ν + 1 2 ) Γ ( μ + 1 2 ) Γ ( ν + 1 2 ) , superscript subscript 0 superscript 𝑡 𝜇 𝜈 Struve-H 𝜇 𝑡 Struve-H 𝜈 𝑡 𝑡 𝜋 Euler-Gamma 𝜇 𝜈 superscript 2 𝜇 𝜈 Euler-Gamma 𝜇 𝜈 1 2 Euler-Gamma 𝜇 1 2 Euler-Gamma 𝜈 1 2 {\displaystyle{\displaystyle\int_{0}^{\infty}t^{-\mu-\nu}\mathbf{H}_{\mu}\left% (t\right)\mathbf{H}_{\nu}\left(t\right)\mathrm{d}t=\frac{\sqrt{\pi}\Gamma\left% (\mu+\nu\right)}{2^{\mu+\nu}\Gamma\left(\mu+\nu+\tfrac{1}{2}\right)\Gamma\left% (\mu+\tfrac{1}{2}\right)\Gamma\left(\nu+\tfrac{1}{2}\right)},}}
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    DLMF:11.7.E12
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    ( μ + ν ) > 0 𝜇 𝜈 0 {\displaystyle{\displaystyle\Re(\mu+\nu)>0}}
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    Γ ( z ) Euler-Gamma 𝑧 {\displaystyle{\displaystyle\Gamma\left(\NVar{z}\right)}}
    C5.S2.E1.m2afdec
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    𝐇 ν ( z ) Struve-H 𝜈 𝑧 {\displaystyle{\displaystyle\mathbf{H}_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C11.S2.E1.m2aidec
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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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    absent {\displaystyle{\displaystyle\Re}}
    C1.S9.E2.m1aedec
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    ν 𝜈 {\displaystyle{\displaystyle\nu}}
    C11.S1.XMD3.m1jdec
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