DLMF:14.20.E10 (Q4931)

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DLMF:14.20.E10
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    𝖯 - 1 2 + i τ ( cos θ ) = 1 + 4 τ 2 + 1 2 2 2 sin 2 ( 1 2 θ ) + ( 4 τ 2 + 1 2 ) ( 4 τ 2 + 3 2 ) 2 2 4 2 sin 4 ( 1 2 θ ) + , shorthand-Ferrers-Legendre-P-first-kind 1 2 𝑖 𝜏 𝜃 1 4 superscript 𝜏 2 superscript 1 2 superscript 2 2 2 1 2 𝜃 4 superscript 𝜏 2 superscript 1 2 4 superscript 𝜏 2 superscript 3 2 superscript 2 2 superscript 4 2 4 1 2 𝜃 {\displaystyle{\displaystyle\mathsf{P}_{-\frac{1}{2}+i\tau}\left(\cos\theta% \right)=1+\frac{4\tau^{2}+1^{2}}{2^{2}}{\sin^{2}}\left(\tfrac{1}{2}\theta% \right)+\frac{\left(4\tau^{2}+1^{2}\right)\left(4\tau^{2}+3^{2}\right)}{2^{2}% \cdot 4^{2}}{\sin^{4}}\left(\tfrac{1}{2}\theta\right)+\cdots,}}
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    DLMF:14.20.E10
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    0 θ π 0 𝜃 𝜋 {\displaystyle{\displaystyle 0\leq\theta\leq\pi}}
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2afdec
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    cos z 𝑧 {\displaystyle{\displaystyle\cos\NVar{z}}}
    C4.S14.E2.m2addec
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    i imaginary-unit {\displaystyle{\displaystyle\mathrm{i}}}
    C1.S9.E1.m2apdec
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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.m2aadec
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    sin z 𝑧 {\displaystyle{\displaystyle\sin\NVar{z}}}
    C4.S14.E1.m2addec
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    τ 𝜏 {\displaystyle{\displaystyle\tau}}
    C14.S1.XMD3.m1qdec
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