Abstract

A recent calculation, in the weak-noise limit, of the rate of escape of a particle over a one-dimensional potential barrier is extended by including an inertial term in the Langevin equation. Specifically, we consider a system described by the Langevin equation\(m\ddot x + \dot x + V\prime (x) = \xi \), whereξ is a Gaussian colored noise with mean zero and correlator 〈ξ(t)ξ(t')〉=(D/τ)exp(−|t−t'|/τ). A pathintegral formulation is augmented by a steepest descent calculation valid in the weak-noise (D→0) limit. This yields an escape rateΓ∼exp(−S/D), where the “action”S is the minimum, over paths characterizing escape over the barrier, of a generalized Onsager-Machlup functional, the extremal path being an “instanton” of the theory. The extremal actionS is calculated analytically for smallm andτ for general potentials, and numerical results forS are displayed for various ranges ofm andτ for the typical case of the quartic potentialV(x)=−x2/2+x4/4.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.