\( \int _ { 0 } ^ { \infty } 1 / ( e ^ { x } - 1 ) d x \)
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The integral \( \int_{0}^{\infty} \frac{1}{e^{x} - 1} \, dx \) is closely related to the calculation of the Riemann zeta function, particularly at even integers. This integral can be evaluated using the series expansion of the integrand or through residues in complex analysis. In short, this integral evaluates to \( \frac{\pi^2}{6} \). Moreover, this integral shows up frequently in physics, particularly in the study of thermodynamics and quantum mechanics. It's associated with the calculation of the Stefan-Boltzmann law, which describes how the energy radiated by a black body scales with temperature. So not only is this integral mathematically fascinating, it has real-world implications in understanding how objects emit radiation!