DLMF:31.10.E22 (Q9077)

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DLMF:31.10.E22
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    𝒦 ⁒ ( r , ΞΈ , Ο• ) = r m ⁒ sin 2 ⁒ p ⁑ ΞΈ ⁒ P ⁑ { 0 1 ∞ 0 0 a cos 2 ⁑ ΞΈ 1 2 ⁒ ( 3 - Ξ³ ) c b } ⁒ P ⁑ { 0 1 ∞ 0 0 a β€² cos 2 ⁑ Ο• 1 - Ο΅ 1 - Ξ΄ b β€² } , 𝒦 π‘Ÿ πœƒ italic-Ο• superscript π‘Ÿ π‘š 2 𝑝 πœƒ Riemann-P-symbol 0 1 absent 0 0 π‘Ž 2 πœƒ 1 2 3 𝛾 𝑐 𝑏 absent Riemann-P-symbol 0 1 absent 0 0 superscript π‘Ž β€² 2 italic-Ο• 1 italic-Ο΅ 1 𝛿 superscript 𝑏 β€² absent {\displaystyle{\displaystyle\mathcal{K}(r,\theta,\phi)=r^{m}{\sin^{2p}}\theta P% \begin{Bmatrix}0&1&\infty&\\ 0&0&a&{\cos^{2}}\theta\\ \tfrac{1}{2}(3-\gamma)&c&b&\end{Bmatrix}\*P\begin{Bmatrix}0&1&\infty&\\ 0&0&a^{\prime}&{\cos^{2}}\phi\\ 1-\epsilon&1-\delta&b^{\prime}&\end{Bmatrix},}}
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    DLMF:31.10.E22
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    P ⁑ { Ξ± Ξ² Ξ³ a 1 b 1 c 1 z a 2 b 2 c 2 } Riemann-P-symbol 𝛼 𝛽 𝛾 absent subscript π‘Ž 1 subscript 𝑏 1 subscript 𝑐 1 𝑧 subscript π‘Ž 2 subscript 𝑏 2 subscript 𝑐 2 absent {\displaystyle{\displaystyle P\NVar{\begin{Bmatrix}\alpha&\beta&\gamma&\\ a_{1}&b_{1}&c_{1}&z\\ a_{2}&b_{2}&c_{2}&\end{Bmatrix}}}}
    C15.S11.E3.m2abdec
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    cos ⁑ z 𝑧 {\displaystyle{\displaystyle\cos\NVar{z}}}
    C4.S14.E2.m2acdec
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