DLMF:13.21.E2 (Q4610)

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DLMF:13.21.E2
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    W κ , μ ( x ) = x Γ ( κ + 1 2 ) ( sin ( κ π - μ π ) J 2 μ ( 2 x κ ) - cos ( κ π - μ π ) Y 2 μ ( 2 x κ ) + env Y 2 μ ( 2 x κ ) O ( κ - 1 2 ) ) , Whittaker-confluent-hypergeometric-W 𝜅 𝜇 𝑥 𝑥 Euler-Gamma 𝜅 1 2 𝜅 𝜋 𝜇 𝜋 Bessel-J 2 𝜇 2 𝑥 𝜅 𝜅 𝜋 𝜇 𝜋 Bessel-Y-Weber 2 𝜇 2 𝑥 𝜅 envelope-Bessel-Y 2 𝜇 2 𝑥 𝜅 Big-O superscript 𝜅 1 2 {\displaystyle{\displaystyle W_{\kappa,\mu}\left(x\right)=\sqrt{x}\Gamma\left(% \kappa+\tfrac{1}{2}\right)\*\left(\sin\left(\kappa\pi-\mu\pi\right)J_{2\mu}% \left(2\sqrt{x\kappa}\right)-\cos\left(\kappa\pi-\mu\pi\right)Y_{2\mu}\left(2% \sqrt{x\kappa}\right)+\mathrm{env}\mskip-2.0mu Y_{2\mu}\left(2\sqrt{x\kappa}% \right)O\left(\kappa^{-\frac{1}{2}}\right)\right),}}
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    DLMF:13.21.E2
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    J ν ( z ) Bessel-J 𝜈 𝑧 {\displaystyle{\displaystyle J_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C10.S2.E2.m2aadec
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    Y ν ( z ) Bessel-Y-Weber 𝜈 𝑧 {\displaystyle{\displaystyle Y_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C10.S2.E3.m2adec
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    O ( x ) Big-O 𝑥 {\displaystyle{\displaystyle O\left(\NVar{x}\right)}}
    C2.S1.E3.m2aadec
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    Γ ( z ) Euler-Gamma 𝑧 {\displaystyle{\displaystyle\Gamma\left(\NVar{z}\right)}}
    C5.S2.E1.m2aadec
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    W κ , μ ( z ) Whittaker-confluent-hypergeometric-W 𝜅 𝜇 𝑧 {\displaystyle{\displaystyle W_{\NVar{\kappa},\NVar{\mu}}\left(\NVar{z}\right)}}
    C13.S14.E3.m2adec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2adec
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    cos z 𝑧 {\displaystyle{\displaystyle\cos\NVar{z}}}
    C4.S14.E2.m2adec
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    env Y ν ( x ) envelope-Bessel-Y 𝜈 𝑥 {\displaystyle{\displaystyle\mathrm{env}\mskip-2.0mu Y_{\NVar{\nu}}\left(\NVar% {x}\right)}}
    C2.S8.SS4.p5.m4adec
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    sin z 𝑧 {\displaystyle{\displaystyle\sin\NVar{z}}}
    C4.S14.E1.m2adec
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    x 𝑥 {\displaystyle{\displaystyle x}}
    C13.S1.XMD4.m1adec
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