  We propose a new strategy to probe the $Z$ boson couplings to bottom and
charm quarks at the LHC. In this work we mainly focus on the case of bottom
quarks. Here, the $Z$ boson is produced in association with two $b$-jets and
decays to electrons or muons. In this final state, tagging the charge of the
$b$-jets allows us to measure the charge asymmetry and thus to directly probe
the $Zb\bar{b}$ couplings. The leptonic final state not only allows us to
cleanly reconstruct the $Z$ boson but also to mitigate the otherwise
overwhelming backgrounds. Furthermore, while LEP could only scan a limited
range of dilepton invariant masses, there is no such limitation at the LHC.
Consequently, this allows us to make full use of the interference between the
amplitudes mediated by a $Z$ boson and a photon. Using the full high-luminosity
LHC dataset of $3~\text{ab}^{-1}$ and with the current flavor and
charge-tagging capabilities would allow us to reject the wrong-sign
right-handed coupling solution by 4$\sigma$. Further improving the
charge-tagging efficiency would disfavor it by 6$\sigma$.
