DLMF:20.10.E4 (Q6840)

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DLMF:20.10.E4
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    0 e - s t θ 1 ( β π 2 | i π t 2 ) d t = 0 e - s t θ 2 ( ( 1 + β ) π 2 | i π t 2 ) d t = - s sinh ( β s ) sech ( s ) , superscript subscript 0 superscript 𝑒 𝑠 𝑡 Jacobi-theta-tau 1 𝛽 𝜋 2 𝑖 𝜋 𝑡 superscript 2 𝑡 superscript subscript 0 superscript 𝑒 𝑠 𝑡 Jacobi-theta-tau 2 1 𝛽 𝜋 2 𝑖 𝜋 𝑡 superscript 2 𝑡 𝑠 𝛽 𝑠 𝑠 {\displaystyle{\displaystyle\int_{0}^{\infty}e^{-st}\theta_{1}\left(\frac{% \beta\pi}{2\ell}\middle|\frac{i\pi t}{\ell^{2}}\right)\mathrm{d}t=\int_{0}^{% \infty}e^{-st}\theta_{2}\left(\frac{(1+\beta)\pi}{2\ell}\middle|\frac{i\pi t}{% \ell^{2}}\right)\mathrm{d}t=-\frac{\ell}{\sqrt{s}}\sinh\left(\beta\sqrt{s}% \right)\operatorname{sech}\left(\ell\sqrt{s}\right),}}
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    DLMF:20.10.E4
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    θ j ( z | τ ) Jacobi-theta-tau 𝑗 𝑧 𝜏 {\displaystyle{\displaystyle\theta_{\NVar{j}}\left(\NVar{z}\middle|\NVar{\tau}% \right)}}
    C20.S2.SS1.m1acdec
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    π {\displaystyle{\displaystyle\pi}}
    C3.S12.E1.m2acdec
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    d x 𝑥 {\displaystyle{\displaystyle\mathrm{d}\NVar{x}}}
    C1.S4.SS4.m1acdec
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    e {\displaystyle{\displaystyle\mathrm{e}}}
    C4.S2.E11.m2adec
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    sech z 𝑧 {\displaystyle{\displaystyle\operatorname{sech}\NVar{z}}}
    C4.S28.E6.m2adec
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    sinh z 𝑧 {\displaystyle{\displaystyle\sinh\NVar{z}}}
    C4.S28.E1.m2adec
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    i imaginary-unit {\displaystyle{\displaystyle\mathrm{i}}}
    C1.S9.E1.m2acdec
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    {\displaystyle{\displaystyle\int}}
    C1.S4.SS4.m3acdec
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    s 𝑠 {\displaystyle{\displaystyle s}}
    C20.S10.XMD1.m1dec
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    β 𝛽 {\displaystyle{\displaystyle\beta}}
    C20.S10.XMD2.m1dec
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