2003
DOI: 10.1016/s0378-4754(02)00224-0
|View full text |Cite
|
Sign up to set email alerts
|

A Feynman–Kac path-integral implementation for Poisson’s equation using an h-conditioned Green’s function

Abstract: This study presents a Feynman-Kac path-integral implementation for solving the Dirichlet problem for Poisson's equation. The algorithm is a modified "walk on spheres" (WOS) that includes the Feynman-Kac path-integral contribution for the source term. In our approach, we use an h-conditioned Green's function instead of simulating Brownian trajectories in detail to implement this path-integral computation. The h-conditioned Green's function allows us to represent the integral of the right-hand-side function from… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
19
0

Year Published

2005
2005
2023
2023

Publication Types

Select...
6
3

Relationship

0
9

Authors

Journals

citations
Cited by 28 publications
(19 citation statements)
references
References 13 publications
0
19
0
Order By: Relevance
“…In the case of a non-constant source term, the modified walk on spheres could be used to compute this contribution [23]. If the walk hits ∂D it stops.…”
Section: 33mentioning
confidence: 99%
“…In the case of a non-constant source term, the modified walk on spheres could be used to compute this contribution [23]. If the walk hits ∂D it stops.…”
Section: 33mentioning
confidence: 99%
“…We propose to check it when we use the so-called discrete Euler scheme [Gob00], which is the simplest procedure that can be used for general stopped diffusions. An alternative is the WOS scheme, which is especially efficient when we are dealing with the Brownian motion (see [HMG03] and the references therein). Some refinements to the discrete Euler scheme are also possible, using Brownian bridge simulations [Bal95,Gob00,Gob01].…”
Section: Proof Of Theorem 32mentioning
confidence: 99%
“…We use an interpolation at the bidimensional Tchebychef grid, two types of discretization schemes, and Monte Carlo simulations. The first one is the modified WOS method [HMG03,GM04] which can take into account the source term f . This walk goes from one sphere to another until the motion reaches the ε-absorption layer.…”
Section: The Bidimensional Casementioning
confidence: 99%
“…Under exponential timestepping, the corresponding improvement is from an error proportional to δt 1/2 , i.e., to the square root of the mean duration of a timestep, to an error proportional to δt [2]. Alternatively, under the walk-on-spheres method, a path is constructed as a sequence of jumps from ball centers to ball surfaces and an absorption layer is defined close to the boundary [16,17]. Realizations are brought to an end when they enter the layer.…”
Section: P[δt > T] = Exp(−λt) (11)mentioning
confidence: 99%