DLMF:14.25.E2 (Q4959)

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DLMF:14.25.E2
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    𝑸 ν μ ( z ) = π 1 / 2 ( z 2 - 1 ) μ / 2 2 μ Γ ( μ + 1 2 ) Γ ( ν - μ + 1 ) 0 ( sinh t ) 2 μ ( z + ( z 2 - 1 ) 1 / 2 cosh t ) ν + μ + 1 d t , associated-Legendre-black-Q 𝜇 𝜈 𝑧 superscript 𝜋 1 2 superscript superscript 𝑧 2 1 𝜇 2 superscript 2 𝜇 Euler-Gamma 𝜇 1 2 Euler-Gamma 𝜈 𝜇 1 superscript subscript 0 superscript 𝑡 2 𝜇 superscript 𝑧 superscript superscript 𝑧 2 1 1 2 𝑡 𝜈 𝜇 1 𝑡 {\displaystyle{\displaystyle\boldsymbol{Q}^{\mu}_{\nu}\left(z\right)=\frac{\pi% ^{1/2}\left(z^{2}-1\right)^{\mu/2}}{2^{\mu}\Gamma\left(\mu+\frac{1}{2}\right)% \Gamma\left(\nu-\mu+1\right)}\*\int_{0}^{\infty}\frac{(\sinh t)^{2\mu}}{\left(% z+(z^{2}-1)^{1/2}\cosh t\right)^{\nu+\mu+1}}\mathrm{d}t,}}
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    DLMF:14.25.E2
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    ( ν + 1 ) > μ > - 1 2 𝜈 1 𝜇 1 2 {\displaystyle{\displaystyle\Re(\nu+1)>\Re\mu>-\tfrac{1}{2}}}
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    Γ ( z ) Euler-Gamma 𝑧 {\displaystyle{\displaystyle\Gamma\left(\NVar{z}\right)}}
    C5.S2.E1.m2aadec
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    𝑸 ν μ ( z ) associated-Legendre-black-Q 𝜇 𝜈 𝑧 {\displaystyle{\displaystyle\boldsymbol{Q}^{\NVar{\mu}}_{\NVar{\nu}}\left(% \NVar{z}\right)}}
    C14.S21.SS1.p1.m3adec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2adec
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    d x 𝑥 {\displaystyle{\displaystyle\mathrm{d}\NVar{x}}}
    C1.S4.SS4.m1aadec
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    cosh z 𝑧 {\displaystyle{\displaystyle\cosh\NVar{z}}}
    C4.S28.E2.m2aadec
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    sinh z 𝑧 {\displaystyle{\displaystyle\sinh\NVar{z}}}
    C4.S28.E1.m2aadec
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    {\displaystyle{\displaystyle\int}}
    C1.S4.SS4.m3aadec
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    absent {\displaystyle{\displaystyle\Re}}
    C1.S9.E2.m1aadec
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    z 𝑧 {\displaystyle{\displaystyle z}}
    C14.S1.XMD4.m1adec
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    μ 𝜇 {\displaystyle{\displaystyle\mu}}
    C14.S1.XMD7.m1adec
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    ν 𝜈 {\displaystyle{\displaystyle\nu}}
    C14.S1.XMD8.m1adec
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