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Information geometry of non-equilibrium processes in a bistable system with a cubic damping

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Figure → −process is initially driven by the movement of the two peaks towardsby a factor of 100 shifting the curves by a factor of 10; that is, time scales ascrucial in forming a single peak atanboth exhibited the samethe off-quenching in [by a factor of
Figure 2. The PDFs for FP, for (a) D = 10−3; (b) D = 10−5; (c) D = 10−7. The initial condition isindicated by the red central peak
Figure 3.according tot. See also the three dots on each curve in Figure D± 10is 2�when the ratio The PDFs for BP, for (a) D =−3; (b) D = 10−5; (c) D = 10−7
Figure 4. Hc) −H = ⟨x4⟩ as a function of time for BP; (d) ∆ = =time for FP; (⟨x4� (a) = 0.7⟨x2⟩ − ⟨x4⟩ as a function of time for FP; (b) ∆�⟨x4⟩ − ⟨x2⟩ as a function of⟩ − ⟨x2⟩ as a function of timefor BP.
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