Woronowicz-type integral representations for the triple sine function

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Let S3(z∣ω1,ω1,ω2)S_3(z\mid\omega_1,\omega_1,\omega_2) denote the triple sine function with two coinciding periods, and let B3,3(z∣ω1,ω1,ω2)B_{3,3}(z\mid\omega_1,\omega_1,\omega_2) be the triple Bernoulli polynomial. Then the following two integral representations hold:

Woronowicz-type integral representations.

log⁡S3(z∣ω1,ω1,ω2)=−πi6B3,3(z∣ω1,ω1,ω2)+12(1−zω1)log⁡(1−e2πiz/ω1)−12πi(z−ω1ω2+12)Li⁡2(e2πiz/ω1)−ω12π2ω2Li⁡3(e2πiz/ω1)+ω22ω12∫0∞ds log⁡(1−e−2πs)[s+i(z−ω1)ω2e−2πω1(ω2s+iz)−1−s−i(z−ω1)ω2e2πω1(ω2s−iz)−1]\begin{aligned} \log S_3(z\mid\omega_1,\omega_1,\omega_2)={}&-\frac{\pi\mathrm{i}}{6}B_{3,3}(z\mid\omega_1,\omega_1,\omega_2)+\frac{1}{2}\left(1-\frac{z}{\omega_1}\right)\log\left(1-e^{2\pi\mathrm{i}z/\omega_1}\right)\\ &-\frac{1}{2\pi\mathrm{i}}\left(\frac{z-\omega_1}{\omega_2}+\frac{1}{2}\right)\operatorname{Li}_2\left(e^{2\pi\mathrm{i}z/\omega_1}\right)-\frac{\omega_1}{2\pi^2\omega_2}\operatorname{Li}_3\left(e^{2\pi\mathrm{i}z/\omega_1}\right)\\ &+\frac{\omega_2^2}{\omega_1^2}\int_0^\infty\mathrm{d}s\,\log\left(1-e^{-2\pi s}\right)\left[\frac{s+\frac{\mathrm{i}(z-\omega_1)}{\omega_2}}{e^{-\frac{2\pi}{\omega_1}(\omega_2s+\mathrm{i}z)}-1}-\frac{s-\frac{\mathrm{i}(z-\omega_1)}{\omega_2}}{e^{\frac{2\pi}{\omega_1}(\omega_2s-\mathrm{i}z)}-1}\right] \end{aligned}

and

log⁡S3(z∣ω1,ω1,ω2)=−πi6B3,3(z∣ω1,ω1,ω2)+ω224π2ω12Li⁡3(e2πiz/ω2)−112log⁡(1−e2πi(z−ω1)/ω2)−ω14πω2∫0∞ds (Li⁡2(e−2πs)−2πslog⁡(1−e−2πs))sinh⁡(2πsω1/ω2)sinh⁡(πω2(ω1(s−i)+iz))sinh⁡(πω2(ω1(s+i)−iz)).\begin{aligned} \log S_3(z\mid\omega_1,\omega_1,\omega_2)={}&-\frac{\pi\mathrm{i}}{6}B_{3,3}(z\mid\omega_1,\omega_1,\omega_2)+\frac{\omega_2^2}{4\pi^2\omega_1^2}\operatorname{Li}_3\left(e^{2\pi\mathrm{i}z/\omega_2}\right)-\frac{1}{12}\log\left(1-e^{2\pi\mathrm{i}(z-\omega_1)/\omega_2}\right)\\ &-\frac{\omega_1}{4\pi\omega_2}\int_0^\infty\mathrm{d}s\,\frac{\left(\operatorname{Li}_2\left(e^{-2\pi s}\right)-2\pi s\log\left(1-e^{-2\pi s}\right)\right)\sinh\left(2\pi s\omega_1/\omega_2\right)}{\sinh\left(\frac{\pi}{\omega_2}(\omega_1(s-\mathrm{i})+\mathrm{i}z)\right)\sinh\left(\frac{\pi}{\omega_2}(\omega_1(s+\mathrm{i})-\mathrm{i}z)\right)}. \end{aligned}

These formulas are conjectured on the basis of comparisons with Bridgeland's expressions and numerical checks for random values of the arguments; their general validity remains to be proved.

References

Primary source

Sergei Alexandrov and Boris Pioline, “Conformal TBA for resolved conifolds”, arXiv:2106.12006 (2021).

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