scispace - formally typeset
Journal ArticleDOI

Functional integration and the Onsager-Machlup Lagrangian for continuous Markov processes in Riemannian geometries

H. Dekker
- 01 May 1979 - 
- Vol. 19, Iss: 5, pp 2102-2111
TLDR
In this paper, the Onsager-Machlup Lagrangian defined by the functional-integral representation of general continuous Markov processes is derived explicitly and concisely based on continuous and differentiable paths connecting fixed end points in the convariant propagator, and the application of a recently developed Fourier-series analysis of these trajectories in locally flat spaces.
Abstract
The Onsager-Machlup Lagrangian defined by the functional-integral representation of general continuous Markov processes is derived explicitly and concisely. Attention is given both to the mathematics and its physical interpretation. The method is based on (i) the consideration of continuous and differentiable paths connecting fixed end points in the convariant propagator, (ii) the application of a recently developed Fourier-series analysis of these trajectories in locally flat spaces, and (iii) the use of the proper transformations between locally Euclidean and globally Riemannian geometries. The spectral analysis allows for arbitrary paths rather than an a priori straight line even in the short-time propagator and avoids any ad hoc discretization rule. Specialized to globally flat spaces the result agrees with formulas given by Stratonovich, Horsthemke and Bach, Graham, and Dekker. It is demonstrated that a unique covariant path integral is equivalent to a whole class of stochastically equivalent lattice expressions.

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Riemannian geometry in thermodynamic fluctuation theory

TL;DR: The covariant thermodynamic fluctuation theory as mentioned in this paper is an extension of the basic structure of the classical one of a subsystem in contact with an infinite uniform reservoir, where a hierarchy of concentric subsystems, each of which samples only the thermodynamic state of the subsystem immediately larger than it, is used.
Journal ArticleDOI

Discrete singular convolution for the solution of the Fokker–Planck equation

TL;DR: In this paper, a discrete singular convolution algorithm for solving the Fokker-Planck equation is presented, where singular kernels of the Hilbert-type and the delta type are presented for numerical computations.
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Statistical mechanics of neocortical interactions. I. Basic formulation

TL;DR: In this article, an approach to collective aspects of the neocortical system is formulated by methods of modern nonlinear nonequilibrium statistical mechanics, which are first spatially averaged over columnar domains.
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Multiple scales of statistical physics of the neocortex: Application to electroencephalography

TL;DR: A statistical physics methodology to bridge several of these scales which are of current experimental interest is described to calculate neuronal processes underlying electroencephalographic and evoked potential data.
Journal ArticleDOI

A unified approach for the solution of the Fokker-Planck equation

TL;DR: In this article, the authors explored the use of a discrete singular convolution algorithm as a unified approach for numerical integration of the Fokker-Planck equation and demonstrated that different implementations of the present algorithm, such as global, local, Galerkin, collocation and finite difference, can be deduced from a single starting point.
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