Fig. 10.

Hard-scatter jet efficiency as a function of a number of reconstructed primary vertices $N_{\mathrm{PV}}$ and b pseudorapidity $|\mathit{\eta }|$, as well as stochastic pile-up jet efficiency as a function of c number of reconstructed primary vertices $N_{\mathrm{PV}}$ and d pseudorapidity $|\mathit{\eta }|$ at 90% efficiency of selecting hard-scatter jets in simulated $t\overline{t}$ events