DLMF:12.5.E3 (Q4117)

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DLMF:12.5.E3
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    U ( a , z ) = e - 1 4 z 2 Γ ( 3 4 + 1 2 a ) 0 t 1 2 a - 1 4 e - t ( z 2 + 2 t ) - 1 2 a - 1 4 d t , parabolic-U 𝑎 𝑧 superscript 𝑒 1 4 superscript 𝑧 2 Euler-Gamma 3 4 1 2 𝑎 superscript subscript 0 superscript 𝑡 1 2 𝑎 1 4 superscript 𝑒 𝑡 superscript superscript 𝑧 2 2 𝑡 1 2 𝑎 1 4 𝑡 {\displaystyle{\displaystyle U\left(a,z\right)=\frac{e^{-\frac{1}{4}z^{2}}}{% \Gamma\left(\frac{3}{4}+\frac{1}{2}a\right)}\*\int_{0}^{\infty}t^{\frac{1}{2}a% -\frac{1}{4}}e^{-t}\left(z^{2}+2t\right)^{-\frac{1}{2}a-\frac{1}{4}}\mathrm{d}% t,}}
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    DLMF:12.5.E3
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    | ph z | < 1 2 π phase 𝑧 1 2 𝜋 {\displaystyle{\displaystyle|\operatorname{ph}z|<\tfrac{1}{2}\pi}}
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    a > - 3 2 𝑎 3 2 {\displaystyle{\displaystyle\Re a>-\tfrac{3}{2}}}
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    Γ ( z ) Euler-Gamma 𝑧 {\displaystyle{\displaystyle\Gamma\left(\NVar{z}\right)}}
    C5.S2.E1.m2abdec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2aadec
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    d x 𝑥 {\displaystyle{\displaystyle\mathrm{d}\NVar{x}}}
    C1.S4.SS4.m1abdec
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    e {\displaystyle{\displaystyle\mathrm{e}}}
    C4.S2.E11.m2abdec
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    {\displaystyle{\displaystyle\int}}
    C1.S4.SS4.m3abdec
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    U ( a , z ) parabolic-U 𝑎 𝑧 {\displaystyle{\displaystyle U\left(\NVar{a},\NVar{z}\right)}}
    C12.S2.SS1.p1.m1abdec
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    ph phase {\displaystyle{\displaystyle\operatorname{ph}}}
    C1.S9.E7.m1aadec
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    absent {\displaystyle{\displaystyle\Re}}
    C1.S9.E2.m1abdec
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    z 𝑧 {\displaystyle{\displaystyle z}}
    C12.S1.XMD3.m1bdec
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