A unified geometric formalism shows that mean dissipated availability and its fluctuations in microscopic heat engines are governed by metric tensors from equilibrium correlation functions in the linear-response regime.
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In the stochastic φ⁴ model, coercivity exhibits v_H scaling, a plateau at the first-order transition field H*, then v_H^{1/2} scaling, with finite-size scalings v_P ~ σ² and (H* - H_P) ~ σ^{4/3} from renormalization-group theory.
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Unified geometric formalism for dissipation and its fluctuations in finite-time microscopic heat engines
A unified geometric formalism shows that mean dissipated availability and its fluctuations in microscopic heat engines are governed by metric tensors from equilibrium correlation functions in the linear-response regime.
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Coercivity Landscape Characterizes Dynamic Hysteresis
In the stochastic φ⁴ model, coercivity exhibits v_H scaling, a plateau at the first-order transition field H*, then v_H^{1/2} scaling, with finite-size scalings v_P ~ σ² and (H* - H_P) ~ σ^{4/3} from renormalization-group theory.