Fig. 6: Signatures of TPL states in the stochastic simulations.

a Average speed and b diffusion coefficient of the oscillators for weak and strong driving force asymmetry. Peaks are observed as the resonances are crossed for strong asymmetry appearing as a function of the coupling strength. c The correlation between oscillators rapidly grows independently of the driving force asymmetry. d Quality factor quantifying the stochastic thermodynamics of precision (Eq. (5)). The quality factor drops as the resonances are crossed.