This talk presents the results of the first coupled-channel meson-baryon $\pi\Sigma-\bar{K}N$ calculation from lattice QCD in the $\Lambda(1405)$ region. The relevant methods to compute correlation functions and extract finite-volume energy spectra are presented, as well as the method to study scattering amplitudes. This study was carried out using a single ensemble with pion mass $m_{\pi}=200$ MeV and kaon mass $m_K = 487$ MeV, and included additional sets of multi-hadron operators. Once the stationary-state energy levels were reliably extracted, the Lüscher formalism was employed to study scattering amplitudes. The final results are consistent with the two-pole picture, where every parametrization of the two-channel $\textit{K}$-matrix exhibits two poles in the complex energy plane. The location of these poles corresponds to a virtual bound state below the $\pi\Sigma$ threshold and a resonance pole below the $\bar{K}N$.