DLMF:12.10.E25 (Q4189)

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DLMF:12.10.E25
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    U ( 1 2 μ 2 , μ t 2 ) g ¯ ( μ ) e - μ 2 ξ ¯ ( t 2 + 1 ) 1 4 s = 0 u ¯ s ( t ) ( t 2 + 1 ) 3 2 s 1 μ 2 s , asymptotic-expansion parabolic-U 1 2 superscript 𝜇 2 𝜇 𝑡 2 ¯ 𝑔 𝜇 superscript 𝑒 superscript 𝜇 2 ¯ 𝜉 superscript superscript 𝑡 2 1 1 4 superscript subscript 𝑠 0 subscript ¯ 𝑢 𝑠 𝑡 superscript superscript 𝑡 2 1 3 2 𝑠 1 superscript 𝜇 2 𝑠 {\displaystyle{\displaystyle U\left(\tfrac{1}{2}\mu^{2},\mu t\sqrt{2}\right)% \sim\frac{\overline{g}(\mu)e^{-\mu^{2}{\overline{\xi}}}}{(t^{2}+1)^{\frac{1}{4% }}}\sum_{s=0}^{\infty}\frac{\overline{u}_{s}(t)}{(t^{2}+1)^{\frac{3}{2}s}}% \frac{1}{\mu^{2s}},}}
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    DLMF:12.10.E25
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    asymptotic-expansion {\displaystyle{\displaystyle\sim}}
    C2.S1.SS3.p1.m11ajdec
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    e {\displaystyle{\displaystyle\mathrm{e}}}
    C4.S2.E11.m2afdec
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    U ( a , z ) parabolic-U 𝑎 𝑧 {\displaystyle{\displaystyle U\left(\NVar{a},\NVar{z}\right)}}
    C12.S2.SS1.p1.m1addec
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    s 𝑠 {\displaystyle{\displaystyle s}}
    C12.S1.XMD5.m1qdec
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    ξ ¯ ¯ 𝜉 {\displaystyle{\displaystyle\overline{\xi}}}
    C12.S10.XMD15.m1dec
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    u ¯ s ( t ) subscript ¯ 𝑢 𝑠 𝑡 {\displaystyle{\displaystyle\overline{u}_{s}(t)}}
    C12.S10.XMD16.m1dec
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