Transducer modeling for accurate acoustic simulations of transcranial focused ultrasound stimulation

Research output: Contribution to journalJournal articleResearchpeer-review

Standard

Transducer modeling for accurate acoustic simulations of transcranial focused ultrasound stimulation. / Pasquinelli, Cristina; Montanaro, Hazael; Lee, Hyunjoo J.; Hanson, Lars G.; Kim, Hyungkook; Kuster, Niels; Siebner, Hartwig R.; Neufeld, Esra; Thielscher, Axel.

In: Journal of Neural Engineering, Vol. 17, No. 4, 046010, 2020.

Research output: Contribution to journalJournal articleResearchpeer-review

Harvard

Pasquinelli, C, Montanaro, H, Lee, HJ, Hanson, LG, Kim, H, Kuster, N, Siebner, HR, Neufeld, E & Thielscher, A 2020, 'Transducer modeling for accurate acoustic simulations of transcranial focused ultrasound stimulation', Journal of Neural Engineering, vol. 17, no. 4, 046010. https://doi.org/10.1088/1741-2552/ab98dc

APA

Pasquinelli, C., Montanaro, H., Lee, H. J., Hanson, L. G., Kim, H., Kuster, N., Siebner, H. R., Neufeld, E., & Thielscher, A. (2020). Transducer modeling for accurate acoustic simulations of transcranial focused ultrasound stimulation. Journal of Neural Engineering, 17(4), [046010]. https://doi.org/10.1088/1741-2552/ab98dc

Vancouver

Pasquinelli C, Montanaro H, Lee HJ, Hanson LG, Kim H, Kuster N et al. Transducer modeling for accurate acoustic simulations of transcranial focused ultrasound stimulation. Journal of Neural Engineering. 2020;17(4). 046010. https://doi.org/10.1088/1741-2552/ab98dc

Author

Pasquinelli, Cristina ; Montanaro, Hazael ; Lee, Hyunjoo J. ; Hanson, Lars G. ; Kim, Hyungkook ; Kuster, Niels ; Siebner, Hartwig R. ; Neufeld, Esra ; Thielscher, Axel. / Transducer modeling for accurate acoustic simulations of transcranial focused ultrasound stimulation. In: Journal of Neural Engineering. 2020 ; Vol. 17, No. 4.

Bibtex

@article{93b57dadc3674625a140b7bbc5638726,
title = "Transducer modeling for accurate acoustic simulations of transcranial focused ultrasound stimulation",
abstract = "Objective. Low-intensity transcranial ultrasound stimulation (TUS) is emerging as a non-invasive brain stimulation technique with superior spatial resolution and the ability to reach deep brain areas. Medical image-based computational modeling could be an important tool for individualized TUS dose control and targeting optimization, but requires further validation. This study aims to assess the impact of the transducer model on the accuracy of the simulations. Approach. Using hydrophone measurements, the acoustic beam of a single-element focused transducer (SEFT) with a flat piezoelectric disc and an acoustic lens was characterized. The acoustic beam was assessed in a homogeneous water bath and after transmission through obstacles (3D-printed shapes and skull samples). The acoustic simulations employed the finite-difference time-domain method and were informed by computed tomography (CT) images of the obstacles. Transducer models of varying complexity were tested representing the SEFT either as a surface boundary condition with variable curvature or also accounting for its internal geometry. In addition, a back-propagated pressure distribution from the first measurement plane was used as source model. The simulations and measurements were quantitatively compared using key metrics for peak location, focus size, intensity and spatial distribution. Main results. While a surface boundary with an adapted, 'effective' curvature radius based on the specifications given by the manufacturer could reproduce the measured focus location and size in a homogeneous water bath, it regularly failed to accurately predict the beam after obstacle transmission. In contrast, models that were based on a one-time calibration to the homogeneous water bath measurements performed substantially better in all cases with obstacles. For one of the 3D-printed obstacles, the simulated intensities deviated substantially from the measured ones, irrespective of the transducer model. We attribute this finding to a standing wave effect, and further studies should clarify its relevance for accurate simulations of skull transmission. Significance. Validated transducer models are important to ensure accurate simulations of the acoustic beam of SEFTs, in particular in the presence of obstacles such as the skull. ",
keywords = "computational dosimetry, finite difference time domain, gamma method, single element focused transducer, transcranial focused ultrasound stimulation",
author = "Cristina Pasquinelli and Hazael Montanaro and Lee, {Hyunjoo J.} and Hanson, {Lars G.} and Hyungkook Kim and Niels Kuster and Siebner, {Hartwig R.} and Esra Neufeld and Axel Thielscher",
year = "2020",
doi = "10.1088/1741-2552/ab98dc",
language = "English",
volume = "17",
journal = "Journal of Neural Engineering",
issn = "1741-2560",
publisher = "Institute of Physics Publishing Ltd",
number = "4",

}

RIS

TY - JOUR

T1 - Transducer modeling for accurate acoustic simulations of transcranial focused ultrasound stimulation

AU - Pasquinelli, Cristina

AU - Montanaro, Hazael

AU - Lee, Hyunjoo J.

AU - Hanson, Lars G.

AU - Kim, Hyungkook

AU - Kuster, Niels

AU - Siebner, Hartwig R.

AU - Neufeld, Esra

AU - Thielscher, Axel

PY - 2020

Y1 - 2020

N2 - Objective. Low-intensity transcranial ultrasound stimulation (TUS) is emerging as a non-invasive brain stimulation technique with superior spatial resolution and the ability to reach deep brain areas. Medical image-based computational modeling could be an important tool for individualized TUS dose control and targeting optimization, but requires further validation. This study aims to assess the impact of the transducer model on the accuracy of the simulations. Approach. Using hydrophone measurements, the acoustic beam of a single-element focused transducer (SEFT) with a flat piezoelectric disc and an acoustic lens was characterized. The acoustic beam was assessed in a homogeneous water bath and after transmission through obstacles (3D-printed shapes and skull samples). The acoustic simulations employed the finite-difference time-domain method and were informed by computed tomography (CT) images of the obstacles. Transducer models of varying complexity were tested representing the SEFT either as a surface boundary condition with variable curvature or also accounting for its internal geometry. In addition, a back-propagated pressure distribution from the first measurement plane was used as source model. The simulations and measurements were quantitatively compared using key metrics for peak location, focus size, intensity and spatial distribution. Main results. While a surface boundary with an adapted, 'effective' curvature radius based on the specifications given by the manufacturer could reproduce the measured focus location and size in a homogeneous water bath, it regularly failed to accurately predict the beam after obstacle transmission. In contrast, models that were based on a one-time calibration to the homogeneous water bath measurements performed substantially better in all cases with obstacles. For one of the 3D-printed obstacles, the simulated intensities deviated substantially from the measured ones, irrespective of the transducer model. We attribute this finding to a standing wave effect, and further studies should clarify its relevance for accurate simulations of skull transmission. Significance. Validated transducer models are important to ensure accurate simulations of the acoustic beam of SEFTs, in particular in the presence of obstacles such as the skull.

AB - Objective. Low-intensity transcranial ultrasound stimulation (TUS) is emerging as a non-invasive brain stimulation technique with superior spatial resolution and the ability to reach deep brain areas. Medical image-based computational modeling could be an important tool for individualized TUS dose control and targeting optimization, but requires further validation. This study aims to assess the impact of the transducer model on the accuracy of the simulations. Approach. Using hydrophone measurements, the acoustic beam of a single-element focused transducer (SEFT) with a flat piezoelectric disc and an acoustic lens was characterized. The acoustic beam was assessed in a homogeneous water bath and after transmission through obstacles (3D-printed shapes and skull samples). The acoustic simulations employed the finite-difference time-domain method and were informed by computed tomography (CT) images of the obstacles. Transducer models of varying complexity were tested representing the SEFT either as a surface boundary condition with variable curvature or also accounting for its internal geometry. In addition, a back-propagated pressure distribution from the first measurement plane was used as source model. The simulations and measurements were quantitatively compared using key metrics for peak location, focus size, intensity and spatial distribution. Main results. While a surface boundary with an adapted, 'effective' curvature radius based on the specifications given by the manufacturer could reproduce the measured focus location and size in a homogeneous water bath, it regularly failed to accurately predict the beam after obstacle transmission. In contrast, models that were based on a one-time calibration to the homogeneous water bath measurements performed substantially better in all cases with obstacles. For one of the 3D-printed obstacles, the simulated intensities deviated substantially from the measured ones, irrespective of the transducer model. We attribute this finding to a standing wave effect, and further studies should clarify its relevance for accurate simulations of skull transmission. Significance. Validated transducer models are important to ensure accurate simulations of the acoustic beam of SEFTs, in particular in the presence of obstacles such as the skull.

KW - computational dosimetry

KW - finite difference time domain

KW - gamma method

KW - single element focused transducer

KW - transcranial focused ultrasound stimulation

U2 - 10.1088/1741-2552/ab98dc

DO - 10.1088/1741-2552/ab98dc

M3 - Journal article

C2 - 32485690

AN - SCOPUS:85088485856

VL - 17

JO - Journal of Neural Engineering

JF - Journal of Neural Engineering

SN - 1741-2560

IS - 4

M1 - 046010

ER -

ID: 250972997