We present a benchmark study of gas phase geometry optimizations in the excited states of carbon monoxide, acetone, acrolein, and methylenecyclopropene using many-body Green's functions theory within the <i>GW</i> approximation and the Bethe-Salpeter Equation (BSE). We scrutinize the influence of several typical approximations in the <i>GW</i>-BSE framework: using of one-shot <i>G<sub>0</sub>W<sub>0</sub></i> or eigenvalue self-consistent ev<i>GW</i>, employing a fully-analytic approach or plasmon-pole model for the frequency dependence of the electron self-energy, or performing the BSE step within the Tamm--Dancoff approximation. The obtained geometries are compared to reference results from multireference perturbation theory (CASPT2), variational Monte Carlo (VMC), second-order approximate coupled cluster (CC2), and time-dependent density-functional theory (TDDFT). We find overall a good agreement of the structural parameters optimized with the <i>GW</i>-BSE calculations with CASPT2, with an average relative error of around 1% for the <i>G<sub>0</sub>W<sub>0</sub></i> and 1.5% for the ev<i>GW</i> variants, respectively, while the other approximations have negligible influence. The relative errors are also smaller than those for CC2 and TDDFT with different functionals and only larger than VMC, indicating that the <i>GW</i>-BSE method does not only yield reliable excitation energies but also geometries.