2014
DOI: 10.1121/1.4892768
|View full text |Cite
|
Sign up to set email alerts
|

Stochastic ray tracing for simulation of high intensity focal ultrasound therapy

Abstract: An algorithm is presented for rapid simulation of high-intensity focused ultrasound (HIFU) fields. Essentially, the method combines ray tracing with Monte Carlo integration to evaluate the Rayleigh-Sommerfeld integral. A large number of computational particles, phonons, are distributed among the elements of a phase-array transducer. The phonons are emitted into random directions and are propagated along trajectories computed with the ray tracing method. As the simulation progresses, an improving stochastic est… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
8
0

Year Published

2015
2015
2024
2024

Publication Types

Select...
8

Relationship

1
7

Authors

Journals

citations
Cited by 13 publications
(8 citation statements)
references
References 23 publications
0
8
0
Order By: Relevance
“…In this case, the computation time should be less than one minute. Three main categories of numerical acoustic propagation methods have been reported and can be listed in increasing complexity: ray tracing [27], angular spectrum methods [24] and full wave propagation [21,28]. The first two methods provide almost instantaneous results.…”
Section: Introductionmentioning
confidence: 99%
“…In this case, the computation time should be less than one minute. Three main categories of numerical acoustic propagation methods have been reported and can be listed in increasing complexity: ray tracing [27], angular spectrum methods [24] and full wave propagation [21,28]. The first two methods provide almost instantaneous results.…”
Section: Introductionmentioning
confidence: 99%
“…Within every plane of the modeled tissue stack, the steady‐state pressure field p ( r) was assumed to satisfy the linear wave equation:normal∇2pfalse(boldrfalse)+k2pfalse(boldrfalse)=0 where 2 is the Laplace operator, and k = ω / c − iα is the complex wave number determined by the angular frequency ω , the celerity c , and the attenuation coefficient α in the respective medium. Therefore, nonlinear wave propagation was not taken into account.…”
Section: Methodsmentioning
confidence: 99%
“…The steady‐state pressure field was calculated at 1.0 MHz in a reference plane positioned in the oil tank containing the transducer, perpendicular to the beam axis (Lx×Ly=120×120 mm2, Nx×Ny = 513 × 513 pixels). For the clinical phased arrays, this pressure field was obtained through the far‐field approximation:pij=Dfalse(ri,rjfalse)eikfalse|boldriboldrjfalse|2italicπfalse|boldriboldrjfalse| where pij is the pressure induced by element i at the position of pixel j , D(ri,rj) is the directivity function, ri is the position vector of the center of element i , and rj is the position vector of pixel j . The pressure in each pixel j in the reference plane was thus obtained by summation of the pressure contributions from every transducer element i .…”
Section: Methodsmentioning
confidence: 99%
“…In future work on the method, in order to obtain a higher accuracy method with a short calculation time, the ray-tracing method can replace SR as the method of determining the phase of each element. 33) We will achieve an accurate and rapid method of determining the phase distribution by considering refraction at the interface between water and the skull, as well as the difference in the time of flight between all elements.…”
Section: Focal Controllability With Phase Controlmentioning
confidence: 99%