A linear third-order 'jerk' equation driven by active Ornstein-Uhlenbeck noise yields mean-square displacement scaling with time exponents 6, 5, 4, or 3, and can destabilize harmonic confinement.
Heterogeneous diffusion in an harmonic potential: the role of the interpretation
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abstract
Diffusion in heterogeneous energy and diffusivity landscapes is widespread in biological systems. However, solving the Langevin equation in such environments introduces ambiguity due to the interpretation parameter $\alpha$, which depends on the underlying physics and can take values in the range $0<\alpha<1$. The typical interpretations are It\^o ($\alpha=0$), Stratonovich ($\alpha=1/2$), and H\"anggi-Klimontovich ($\alpha=1$). Here, we analyse the motion of a particle in an harmonic potential -- modelled as an Ornstein-Uhlenbeck process -- with diffusivity that varies in space. Our focus is on two-phase systems with a discontinuity in environmental properties at $x=0$. We derive the probability density of the particle position for the process, and consider two paradigmatic situations. In the first one, the damping coefficient remains constant, and fluctuation-dissipation relations are not satisfied. In the second one, these relations are enforced, leading to a position-dependent damping coefficient. In both cases, we provide solutions as a function of the interpretation parameter $\alpha$, with particular attention to the It\^o, Stratonovich, and H\"anggi-Klimontovich interpretations, revealing fundamentally different behaviours, in particular with respect to an interface located at the potential minimum.
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Gigantic dynamical spreading and anomalous diffusion of jerky active particles
A linear third-order 'jerk' equation driven by active Ornstein-Uhlenbeck noise yields mean-square displacement scaling with time exponents 6, 5, 4, or 3, and can destabilize harmonic confinement.