On computer simulation of Feynman-Kac path-integrals

Consider a path-integral E x exp {∞ t o V( X( s)) ds} f( X( t)) which is the solution to a diffusion version of the generalized Schrödinger's equation ∂u ∂t = Hu , u(0,x) = ƒ(x). Here H = A + V, where A is an infinitesimal generator of a strong continuous Markov semigroup corresponding to the d...

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Bibliographic Details
Published inJournal of computational and applied mathematics Vol. 66; no. 1; pp. 333 - 336
Main Author Korzeniowski, Andrzej
Format Journal Article Conference Proceeding
LanguageEnglish
Published Amsterdam Elsevier B.V 01.01.1996
Elsevier
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Summary:Consider a path-integral E x exp {∞ t o V( X( s)) ds} f( X( t)) which is the solution to a diffusion version of the generalized Schrödinger's equation ∂u ∂t = Hu , u(0,x) = ƒ(x). Here H = A + V, where A is an infinitesimal generator of a strong continuous Markov semigroup corresponding to the diffusion process { X( s), 0⩽ s⩽ t, X(0) = x}. To see a connection to quantum mechanics, take A = 1 2 Δ and replace V by − V. Then one obtains H ̄ = −H = − 1 2 Δ + V , which is a quantum mechanical Hamiltonian corresponding to a particle of mass 1 (in atomic units) subject to interaction with potential V. Path-integrals play a role in obtaining physical quantities such as ground state energies. This paper will be concerned with explanations of two approaches in the actual computer evaluations of path-integrals through simulations of the diffusion processes. The results will be presented by comparing, in concrete examples, the computational advantages or disadvantages depending on whether the diffusion process X( t) is ergodic or not.
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ISSN:0377-0427
1879-1778
DOI:10.1016/0377-0427(95)00170-0