We present a theoretical study of quantum coherent dynamics in a three-level Λ system driven by a thermal environment. By solving the nonsecular Bloch-Redfield master equations, we obtain analytical results for the ground-state population and coherence dynamics and classify the dynamical regimes of the incoherently driven Λ-system as underdamped and overdamped depending on whether the ratio ∆/[rf (p)] is greater or less than one, where ∆ is the ground-state energy splitting, r is the incoherent pumping rate, and f (p) is a dimensionless function of the transition dipole alignment parameter p. In the underdamped regime, we observe long-lived coherent dynamics that lasts for τc 1/r, even though the initial state of the Λ-system contains no coherences in the energy basis. In the overdampled regime for p = 1, we observe the emergence of coherent quasi-steady states with the lifetime τc = 1.34(r/∆ 2 ), which have low von Neumann entropy compared to the conventional thermal states. Our results suggest that thermal excitations can enhance the lifetimes of initially created coherent superpositions, making thermal driving a potentially useful coherence-enhancing tool for quantum information science.