DLMF:14.18.E3 (Q4904)

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DLMF:14.18.E3
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    𝖰 ν ( cos θ 1 cos θ 2 + sin θ 1 sin θ 2 cos ϕ ) = 𝖯 ν ( cos θ 1 ) 𝖰 ν ( cos θ 2 ) + 2 m = 1 ( - 1 ) m 𝖯 ν - m ( cos θ 1 ) 𝖰 ν m ( cos θ 2 ) cos ( m ϕ ) . shorthand-Ferrers-Legendre-Q-first-kind 𝜈 subscript 𝜃 1 subscript 𝜃 2 subscript 𝜃 1 subscript 𝜃 2 italic-ϕ shorthand-Ferrers-Legendre-P-first-kind 𝜈 subscript 𝜃 1 shorthand-Ferrers-Legendre-Q-first-kind 𝜈 subscript 𝜃 2 2 superscript subscript 𝑚 1 superscript 1 𝑚 Ferrers-Legendre-P-first-kind 𝑚 𝜈 subscript 𝜃 1 Ferrers-Legendre-Q-first-kind 𝑚 𝜈 subscript 𝜃 2 𝑚 italic-ϕ {\displaystyle{\displaystyle\mathsf{Q}_{\nu}\left(\cos\theta_{1}\cos\theta_{2}% +\sin\theta_{1}\sin\theta_{2}\cos\phi\right)=\mathsf{P}_{\nu}\left(\cos\theta_% {1}\right)\mathsf{Q}_{\nu}\left(\cos\theta_{2}\right)+2\sum_{m=1}^{\infty}(-1)% ^{m}\mathsf{P}^{-m}_{\nu}\left(\cos\theta_{1}\right)\mathsf{Q}^{m}_{\nu}\left(% \cos\theta_{2}\right)\cos\left(m\phi\right).}}
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    DLMF:14.18.E3
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    𝖯 ν μ ( x ) Ferrers-Legendre-P-first-kind 𝜇 𝜈 𝑥 {\displaystyle{\displaystyle\mathsf{P}^{\NVar{\mu}}_{\NVar{\nu}}\left(\NVar{x}% \right)}}
    C14.S3.E1.m2abdec
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    𝖰 ν μ ( x ) Ferrers-Legendre-Q-first-kind 𝜇 𝜈 𝑥 {\displaystyle{\displaystyle\mathsf{Q}^{\NVar{\mu}}_{\NVar{\nu}}\left(\NVar{x}% \right)}}
    C14.S3.E2.m2adec
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    cos z 𝑧 {\displaystyle{\displaystyle\cos\NVar{z}}}
    C4.S14.E2.m2abdec
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    𝖯 ν ( x ) = 𝖯 ν 0 ( x ) shorthand-Ferrers-Legendre-P-first-kind 𝜈 𝑥 Ferrers-Legendre-P-first-kind 0 𝜈 𝑥 {\displaystyle{\displaystyle\mathsf{P}_{\NVar{\nu}}\left(\NVar{x}\right)=% \mathsf{P}^{0}_{\nu}\left(x\right)}}
    C14.S2.SS2.p2.m2abdec
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    𝖰 ν ( x ) = 𝖰 ν 0 ( x ) shorthand-Ferrers-Legendre-Q-first-kind 𝜈 𝑥 Ferrers-Legendre-Q-first-kind 0 𝜈 𝑥 {\displaystyle{\displaystyle\mathsf{Q}_{\NVar{\nu}}\left(\NVar{x}\right)=% \mathsf{Q}^{0}_{\nu}\left(x\right)}}
    C14.S2.SS2.p2.m4adec
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    sin z 𝑧 {\displaystyle{\displaystyle\sin\NVar{z}}}
    C4.S14.E1.m2abdec
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