Quantum coherent dynamics of a
Λ-system driven by a thermal environment: Enhancing coherence lifetimes via incoherent driving
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
Δ/[rf(p)] is greater or less than one, where
Δ 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/Δ2), 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.
We present a theoretical study of quantum coherent dynamics of a three-level Λ-system driven by a thermal environment (such as blackbody radiation), which serves as an essential building block of photosynthetic light-harvesting models and quantum heat engines. By solving 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 Δ/[rf(p)] is greater or less than one, where Δ is the ground-state energy splitting, r is the incoherent pumping rate, and f(p) is a 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 overdamped regime for p = 1, we observe the emergence of coherent quasi-steady states with the lifetime τc = 1.34(r/Δ2), which have a low von Neumann entropy compared to conventional thermal states. We propose an experimental scenario for observing noise-induced coherent dynamics in metastable He* atoms driven by x-polarized incoherent light. Our results suggest that thermal excitations can generate experimentally observable long-lived quantum coherent dynamics in the ground-state subspace of atomic and molecular Λ-systems in the absence of coherent driving.