DLMF:11.6.E6 (Q3982)

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DLMF:11.6.E6
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    𝐊 ν ( λ ν ) ( 1 2 λ ν ) ν - 1 π Γ ( ν + 1 2 ) k = 0 k ! c k ( λ ) ν k , asymptotic-expansion associated-Struve-K 𝜈 𝜆 𝜈 superscript 1 2 𝜆 𝜈 𝜈 1 𝜋 Euler-Gamma 𝜈 1 2 superscript subscript 𝑘 0 𝑘 subscript 𝑐 𝑘 𝜆 superscript 𝜈 𝑘 {\displaystyle{\displaystyle\mathbf{K}_{\nu}\left(\lambda\nu\right)\sim\frac{(% \tfrac{1}{2}\lambda\nu)^{\nu-1}}{\sqrt{\pi}\Gamma\left(\nu+\tfrac{1}{2}\right)% }\sum_{k=0}^{\infty}\frac{k!c_{k}(\lambda)}{\nu^{k}},}}
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    DLMF:11.6.E6
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    | ph ν | 1 2 π - δ phase 𝜈 1 2 𝜋 𝛿 {\displaystyle{\displaystyle|\operatorname{ph}\nu|\leq\tfrac{1}{2}\pi-\delta}}
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    Γ ( z ) Euler-Gamma 𝑧 {\displaystyle{\displaystyle\Gamma\left(\NVar{z}\right)}}
    C5.S2.E1.m2abdec
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    𝐊 ν ( z ) associated-Struve-K 𝜈 𝑧 {\displaystyle{\displaystyle\mathbf{K}_{\NVar{\nu}}\left(\NVar{z}\right)}}
    C11.S2.E5.m2abdec
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    asymptotic-expansion {\displaystyle{\displaystyle\sim}}
    C2.S1.SS3.p1.m11addec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2aedec
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    ! {\displaystyle{\displaystyle!}}
    introduction.Sx4.p1.t1.r15.m5abdec
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    ph phase {\displaystyle{\displaystyle\operatorname{ph}}}
    C1.S9.E7.m1aedec
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    ν 𝜈 {\displaystyle{\displaystyle\nu}}
    C11.S1.XMD3.m1cdec
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    k 𝑘 {\displaystyle{\displaystyle k}}
    C11.S1.XMD5.m1ddec
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