DLMF:13.4.E15 (Q4378)

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DLMF:13.4.E15
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    U ( a , b , z ) Γ ( c ) Γ ( c - b + 1 ) = z 1 - c 2 π i - ( 0 + ) e z t t - c 𝐅 1 2 ( a , c ; a + c - b + 1 ; 1 - 1 t ) d t , Kummer-confluent-hypergeometric-U 𝑎 𝑏 𝑧 Euler-Gamma 𝑐 Euler-Gamma 𝑐 𝑏 1 superscript 𝑧 1 𝑐 2 𝜋 imaginary-unit superscript subscript limit-from 0 superscript 𝑒 𝑧 𝑡 superscript 𝑡 𝑐 hypergeometric-bold-pFq 2 1 𝑎 𝑐 𝑎 𝑐 𝑏 1 1 1 𝑡 𝑡 {\displaystyle{\displaystyle\frac{U\left(a,b,z\right)}{\Gamma\left(c\right)% \Gamma\left(c-b+1\right)}=\frac{z^{1-c}}{2\pi\mathrm{i}}\int_{-\infty}^{(0+)}e% ^{zt}t^{-c}{{}_{2}{\mathbf{F}}_{1}}\left(a,c;a+c-b+1;1-\frac{1}{t}\right)% \mathrm{d}t,}}
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    DLMF:13.4.E15
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    | ph z | < 1 2 π phase 𝑧 1 2 𝜋 {\displaystyle{\displaystyle\left|\operatorname{ph}z\right|<\frac{1}{2}\pi}}
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    Γ ( z ) Euler-Gamma 𝑧 {\displaystyle{\displaystyle\Gamma\left(\NVar{z}\right)}}
    C5.S2.E1.m2aldec
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    U ( a , b , z ) Kummer-confluent-hypergeometric-U 𝑎 𝑏 𝑧 {\displaystyle{\displaystyle U\left(\NVar{a},\NVar{b},\NVar{z}\right)}}
    C13.S2.E6.m2afdec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2ajdec
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    d x 𝑥 {\displaystyle{\displaystyle\mathrm{d}\NVar{x}}}
    C1.S4.SS4.m1andec
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    e {\displaystyle{\displaystyle\mathrm{e}}}
    C4.S2.E11.m2amdec
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    𝐅 q p ( 𝐚 ; 𝐛 ; ) hypergeometric-bold-pFq 𝑝 𝑞 𝐚 𝐛 {\displaystyle{\displaystyle{{}_{\NVar{p}}{\mathbf{F}}_{\NVar{q}}}\left(\NVar{% \mathbf{a}};\NVar{\mathbf{b}};\right)\)\@add@PDF@RDFa@triples\end{document}}}
    C16.S2.E5.m2abdec
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    i imaginary-unit {\displaystyle{\displaystyle\mathrm{i}}}
    C1.S9.E1.m2afdec
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    {\displaystyle{\displaystyle\int}}
    C1.S4.SS4.m3andec
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    ph phase {\displaystyle{\displaystyle\operatorname{ph}}}
    C1.S9.E7.m1agdec
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    z 𝑧 {\displaystyle{\displaystyle z}}
    C13.S1.XMD6.m1ndec
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