The virial expansion characterizes the high-temperature approach to the quantum-classical crossover in any quantum many-body system. Here, we calculate the virial coefficients up to the fifth-order of Fermi gases in 1D, 2D, and 3D, with attractive contact interactions, as relevant for a variety of applications in atomic and nuclear physics. To that end, we discretize the imaginary-time direction and calculate the relevant canonical partition functions. In coarse discretizations, we obtain analytic results featuring relationships between the interaction-induced changes $��b_3$, $��b_4$, and $��b_5$ as functions of $��b_2$, the latter being exactly known in many cases by virtue of the Beth-Uhlenbeck formula. Using automated-algebra methods, we push our calculations to progressively finer discretizations and extrapolate to the continuous-time limit. We find excellent agreement for $��b_3$ with previous calculations in all dimensions and we formulate predictions for $��b_4$ and $��b_5$ in 1D and 2D. We also provide, for a range of couplings,the subspace contributions $��b_{31}$, $��b_{22}$, $��b_{41}$, and $��b_{32}$, which determine the equation of state and static response of polarized systems at high temperature. As a performance check, we compare the density equation of state and Tan contact with quantum Monte Carlo calculations, diagrammatic approaches, and experimental data where available. Finally, we apply Pad�� and Pad��-Borel resummation methods to extend the usefulness of the virial coefficients to approach and in some cases go beyond the unit-fugacity point.

15 pages, 14 figures; greatly expanded version including subspace contributions, extrapolations to the continuous-time limit, and applications in 1D, 2D, and 3D using resummation techniques