TY - JOUR
T1 - Shear wave speed measurement bias in a viscoelastic phantom across six ultrasound elastography systems
T2 - a comparative study with transient elastography and magnetic resonance elastography
AU - Kishimoto, Riwa
AU - Suga, Mikio
AU - Usumura, Masashi
AU - Iijima, Hiroko
AU - Yoshida, Masahiro
AU - Hachiya, Hiroyuki
AU - Shiina, Tsuyoshi
AU - Yamakawa, Makoto
AU - Konno, Kei
AU - Obata, Takayuki
AU - Yamaguchi, Tadashi
N1 - Funding Information:
We gratefully acknowledge the vendors who provided their ultrasound systems and made this study possible, including Canon Medical Systems, FUJIFILM Healthcare (formerly Hitachi), GE Healthcare Japan, Integral, Konica Minolta Japan, Philips Japan, and Siemens Healthcare KK. This work was conducted as part of the activities of the JSUM SWE Standardization Subcommittee and JRS J-QIBA. We would also like to thank Dr. Kazuki Tamura and Mr. Takeru Mizoguchi for their valuable help in measuring the acoustic characteristics, Mr. Daiki Ito for measuring the SWS using US-SWE, and Mr. Yo Taniguchi for measuring the MRE. This study was supported by MEXT and JSPS Grants-in-Aid for Scientific Research on Innovative Areas (Grant numbers JP17H02115, JP17H05279, and JP19K08242).
Funding Information:
We gratefully acknowledge the vendors who provided their ultrasound systems and made this study possible, including Canon Medical Systems, FUJIFILM Healthcare (formerly Hitachi), GE Healthcare Japan, Integral, Konica Minolta Japan, Philips Japan, and Siemens Healthcare KK. This work was conducted as part of the activities of the JSUM SWE Standardization Subcommittee and JRS J-QIBA. We would also like to thank Dr. Kazuki Tamura and Mr. Takeru Mizoguchi for their valuable help in measuring the acoustic characteristics, Mr. Daiki Ito for measuring the SWS using US-SWE, and Mr. Yo Taniguchi for measuring the MRE. This study was supported by MEXT and JSPS Grants-in-Aid for Scientific Research on Innovative Areas (Grant numbers JP17H02115, JP17H05279, and JP19K08242).
Publisher Copyright:
© 2022, The Author(s).
PY - 2022/4
Y1 - 2022/4
N2 - Purpose: To quantify the bias of shear wave speed (SWS) measurements in a viscoelastic phantom across six different ultrasound (US) systems and to compare the SWS with those from transient elastography (TE) and magnetic resonance elastography (MRE). Methods: A viscoelastic phantom of stiffness representing fibrotic liver or healthy thyroid was measured with nine (linear probe) and 10 (convex probe) modes of six different US-based shear wave elastography (SWE) systems using linear and convex probes. SWS measurements of three regions of interest were repeated thrice at two focal depths, coupling the probe to the phantom using a jig. An MRE system using three motion-encoding gradient frequencies of 60, 90, and 120 Hz and TE were also used to measure the stiffness of the phantom. Results: The SWS from different SWE systems had mean coefficients of variation of 9.0–9.2% and 5.4–5.6% with linear and convex probes, respectively, in viscoelastic phantom measurement. The focal depth was a less significant source of SWS variability than the system. The total average SWS obtained with US-SWE systems was 19.9% higher than that obtained with MRE at 60 Hz, which is commonly used in clinical practice, and 31.5% higher than that obtained with TE using the M probe. Conclusions: Despite the measurement biases associated with the SWE systems, biases were not necessarily consistent, and they changed with the probes used and depth measured. The SWS of the viscoelastic phantom obtained using different modalities increased according to the shear wave frequency used.
AB - Purpose: To quantify the bias of shear wave speed (SWS) measurements in a viscoelastic phantom across six different ultrasound (US) systems and to compare the SWS with those from transient elastography (TE) and magnetic resonance elastography (MRE). Methods: A viscoelastic phantom of stiffness representing fibrotic liver or healthy thyroid was measured with nine (linear probe) and 10 (convex probe) modes of six different US-based shear wave elastography (SWE) systems using linear and convex probes. SWS measurements of three regions of interest were repeated thrice at two focal depths, coupling the probe to the phantom using a jig. An MRE system using three motion-encoding gradient frequencies of 60, 90, and 120 Hz and TE were also used to measure the stiffness of the phantom. Results: The SWS from different SWE systems had mean coefficients of variation of 9.0–9.2% and 5.4–5.6% with linear and convex probes, respectively, in viscoelastic phantom measurement. The focal depth was a less significant source of SWS variability than the system. The total average SWS obtained with US-SWE systems was 19.9% higher than that obtained with MRE at 60 Hz, which is commonly used in clinical practice, and 31.5% higher than that obtained with TE using the M probe. Conclusions: Despite the measurement biases associated with the SWE systems, biases were not necessarily consistent, and they changed with the probes used and depth measured. The SWS of the viscoelastic phantom obtained using different modalities increased according to the shear wave frequency used.
KW - Magnetic resonance elastography
KW - Phantom
KW - Quantitative imaging biomarker alliance
KW - Ultrasound elastography
KW - Viscoelasticity
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U2 - 10.1007/s10396-022-01190-x
DO - 10.1007/s10396-022-01190-x
M3 - Article
C2 - 35061118
AN - SCOPUS:85123246249
SN - 1346-4523
VL - 49
SP - 143
EP - 152
JO - Japanese Journal of Medical Ultrasonics
JF - Japanese Journal of Medical Ultrasonics
IS - 2
ER -