Fig. 4
From: Quantum control of excitons for reversible heat transfer

Heat engine efficiency. Efficiency as a fraction of the Carnot efficiency for an exciton heat engine. Results are shown as functions of the spectral chirp (a, horizontal axes) and the pulse area (Θ0, vertical axes) of the driving pulse used for the heat absorption stroke. The panels correspond to different values of the detuning, δ, and unchirped pulse duration, τ0. a δ = 0 ps−1, τ0 = 2 ps−1. b δ = 2.5 ps−1, τ0 = 2 ps−1. c δ = 0 ps−1, τ0 = 0.5 ps−1. d δ = 2.5 ps−1, τ0 = 0.5 ps−1