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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Published in | Journal of computational and applied mathematics Vol. 66; no. 1; pp. 333 - 336 |
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Main Author | |
Format | Journal Article Conference Proceeding |
Language | English |
Published |
Amsterdam
Elsevier B.V
01.01.1996
Elsevier |
Subjects | |
Online Access | Get full text |
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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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Bibliography: | SourceType-Scholarly Journals-2 ObjectType-Feature-2 ObjectType-Conference Paper-1 content type line 23 SourceType-Conference Papers & Proceedings-1 ObjectType-Article-3 |
ISSN: | 0377-0427 1879-1778 |
DOI: | 10.1016/0377-0427(95)00170-0 |