DLMF:14.17.E20 (Q4901)

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DLMF:14.17.E20
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    Statements

    1 ( Q ν ( x ) ) 2 d x = ψ ( ν + 1 ) 2 ν + 1 , superscript subscript 1 superscript shorthand-Legendre-Q-second-kind 𝜈 𝑥 2 𝑥 diffop digamma 1 𝜈 1 2 𝜈 1 {\displaystyle{\displaystyle\int_{1}^{\infty}(Q_{\nu}\left(x\right))^{2}% \mathrm{d}x=\frac{\psi'\left(\nu+1\right)}{2\nu+1},}}
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    DLMF:14.17.E20
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    ν > - 1 2 𝜈 1 2 {\displaystyle{\displaystyle\Re\nu>-\tfrac{1}{2}}}
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    d x 𝑥 {\displaystyle{\displaystyle\mathrm{d}\NVar{x}}}
    C1.S4.SS4.m1asdec
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    ψ ( z ) digamma 𝑧 {\displaystyle{\displaystyle\psi\left(\NVar{z}\right)}}
    C5.S2.E2.m2agdec
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    {\displaystyle{\displaystyle\int}}
    C1.S4.SS4.m3asdec
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    absent {\displaystyle{\displaystyle\Re}}
    C1.S9.E2.m1aedec
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    Q ν ( z ) = Q ν 0 ( z ) shorthand-Legendre-Q-second-kind 𝜈 𝑧 Legendre-Q-second-kind 0 𝜈 𝑧 {\displaystyle{\displaystyle Q_{\NVar{\nu}}\left(\NVar{z}\right)=Q^{0}_{\nu}% \left(z\right)}}
    C14.S2.SS2.p2.m5abdec
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