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Malakhov A.N.

Exact relaxation times and metastable state decay times for
Brownian diffusion in arbitrary potential profiles

A.N. Malakhov
Radiophysical Dept., Nizhny Novgorod State University,
Nizhny Novgorod, Russia

One-dimensional chaotic motion of the Brownian particles in the overdumped regime (Brownian diffusion) in potential profiles is considered. Exact relaxation times and metastable state decay times are obtained. The potential profiles tex2html_wrap_inline3812 may be arbitrary except its behaviour at tex2html_wrap_inline3814 . The initial probability distribution of the particles density is tex2html_wrap_inline3816 .

Three types of potential profiles are investigated. The first: tex2html_wrap_inline3818 at tex2html_wrap_inline3814 ; the second: tex2html_wrap_inline3822 at tex2html_wrap_inline3814 ; the third: tex2html_wrap_inline3818 at tex2html_wrap_inline3828 and tex2html_wrap_inline3822 at tex2html_wrap_inline3832 (or tex2html_wrap_inline3822 at tex2html_wrap_inline3828 and tex2html_wrap_inline3818 at tex2html_wrap_inline3832 ).

For the first type of a potential profile there is the equilibrium probability distribution tex2html_wrap_inline3842 where tex2html_wrap_inline3844 is a dimensionless potential profile, A;SPMgt;0 is the normalization factor. The relaxation time is a characteristic time of a variation probability distribution from the initial probability distribution to a final one tex2html_wrap_inline3848 .

For the second and third types of potential profiles the final probability distribution is zero: tex2html_wrap_inline3850 .

Let in potential profiles exist local minima (metastable states) where the initial probability distribution is placed. The total probability near a local minimum is varied from unity to final. A characteristic time of this variation is the metastable state decay time. Besides that it may be very interesting to know the life time of an unstable state, when the potential profile at the initial point tex2html_wrap_inline3852 does not have a local minimum.

By the new method of attack it has been demonstrated that all exact characteristic times in question are represented in terms of quadrature of the dimensionless potential profile, as well as it was found by L.A.Pontryagin et. al. for the mean first passage time.

The results following from common obtained formulae are shown to coinside with the time characteristics derived for different particular cases of the potential profiles, which is known from the literature (see e.g. M.Mörsch, H.Risken, V.Vollmer, Z. Phys. B32, 245 (1979), H.Frisch, V.Privman, C.Nicolis, G.Nicolis, J.Phys. A23, L1147 (1990), V.Privman, H.Frisch, J.Chem.Phys. 94, 8216 (1991), N.V. Agudov, A.N.Malakhov, Radiophys. and Quant. Electr. 36, 97 (1993), etc.).


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Next: Malakhov A.N.Agudov N.V. Up: Book of Abstracts Previous: Makishima M. and Shimizu T.

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