2016
DOI: 10.1088/1361-6560/62/1/91
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A diffraction correction for storage and loss moduli imaging using radiation force based elastography

Abstract: Noninvasive evaluation of the rheological behavior of soft tissues may provide an important diagnosis tool. Nowadays, available commercial ultrasound systems only provide shear elasticity estimation by shear wave speed assessment under the hypothesis of a purely elastic model. However, to fully characterize the rheological behavior of tissues, given by its storage (G') and loss (G″) moduli, it is necessary to estimate both: shear wave speed and shear wave attenuation. Most elastography techniques use the acous… Show more

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Cited by 49 publications
(36 citation statements)
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“…Two procedures are commonly used to estimate the phase velocity and attenuation from the Fourier transform signal trueufalse(r,ωfalse). First, as described by Chen, et al [4] and Deffieux, et al [13], the phase of the asymptotic Hankel function (9) varies linearly with the coordinate r , so a linear fit of phase vs. position can be used to measure the wavenumber k and phase velocity c ( ω ) = ω / k. Similarly, the attenuation α ( ω ) can be measured using the exponential decay with position in (9) [14, 15], or by using the Hankel function dependence in (8) [9]. A second method to measure the phase velocity and attenuation is by constructing the two-dimensional Fourier transform (2DFT) of the spatial-temporal shear wave signal and to measure the phase velocity and attenuation from the peak location and width of the 2DFT signal at each specific temporal frequency [8, 16, 17].…”
Section: Introductionmentioning
confidence: 99%
“…Two procedures are commonly used to estimate the phase velocity and attenuation from the Fourier transform signal trueufalse(r,ωfalse). First, as described by Chen, et al [4] and Deffieux, et al [13], the phase of the asymptotic Hankel function (9) varies linearly with the coordinate r , so a linear fit of phase vs. position can be used to measure the wavenumber k and phase velocity c ( ω ) = ω / k. Similarly, the attenuation α ( ω ) can be measured using the exponential decay with position in (9) [14, 15], or by using the Hankel function dependence in (8) [9]. A second method to measure the phase velocity and attenuation is by constructing the two-dimensional Fourier transform (2DFT) of the spatial-temporal shear wave signal and to measure the phase velocity and attenuation from the peak location and width of the 2DFT signal at each specific temporal frequency [8, 16, 17].…”
Section: Introductionmentioning
confidence: 99%
“…2 can also be compared to shear wave spectroscopy measurements of the phase velocity as described by Deffieux, et al(2009) and attenuation from the decay of the shear wave signal as described by Budelli, et al(2017). Using the asymptotic form of the Bessel function in (5) and including a x weighting factor, the temporal Fourier transform shear wave signal has the form xtruevfalse(x,ωfalse)~eikfalse(ωfalse)xeαfalse(ωfalse)x…”
Section: Resultsmentioning
confidence: 99%
“…Measurements of c ( ω ) and/or α ( ω ) in viscoelastic materials have been reported by many authors including Deffieux, et al(2009), Nenadic, et al(2017), Nightingale, et al(2015) and Budelli, et al(2017). In addition, direct measurements of μ ( ω ) have been reported by several authors including Henni, et al(2010) and Manduca, et al(2001).…”
Section: Introductionmentioning
confidence: 99%
“…This situation is further exacerbated in viscoelastic estimators where researchers often attempt to estimate phase speed of individual shear wave spectral components [49]. Since the energy of a frequency component is much lower than that of the broadband signal, large variances are reported in the literature while estimating viscous attenuation (>50 Np/m in [50]). A common technique to tackle this issue is to use a larger shear wave propagation ROI [49], [51].…”
Section: Discussionmentioning
confidence: 99%