2001
DOI: 10.1016/s0730-725x(01)00387-3
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Simulation and analysis of magnetic resonance elastography wave images using coupled harmonic oscillators and Gaussian local frequency estimation

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Cited by 49 publications
(39 citation statements)
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“…Equation [8] provides an analytical relation between the elastic moduli and phase velocity surface, showing that 12 , 13 , and the ratio E 3 /E 1 are the only elastic parameters that are relevant for group velocity inversion applied to incompressible, transversely isotropic media. Interestingly, it is not possible to deduce all three elastic parameters from a single component of u.…”
Section: Resultsmentioning
confidence: 99%
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“…Equation [8] provides an analytical relation between the elastic moduli and phase velocity surface, showing that 12 , 13 , and the ratio E 3 /E 1 are the only elastic parameters that are relevant for group velocity inversion applied to incompressible, transversely isotropic media. Interestingly, it is not possible to deduce all three elastic parameters from a single component of u.…”
Section: Resultsmentioning
confidence: 99%
“…Since the ST-mode controls pure out-of-plane displacement in the case of transverse isotropy, c ST in Eq. [8] also applies to compressible media. Its shape is described by an ellipsoid whose axes are determined by 12 and 13 (14).…”
Section: Shear Waves In Transverse Isotropic Elastic and Incompressibmentioning
confidence: 99%
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“…Stiff regions indicate an abnormality. Experiments that are devised to create displacement that will yield tissue mechanical properties include: ͑1͒ tissue is compressed; stiff tissue compresses less; the displacement is measured using ultrasound or MR; the Lamé parameter, , is imaged, ͑Oberai et al., 2004;Barbone and Bamber, 2002;Konofagou et al, 2000;Thitaikumar and Ophir, 2007͒; ͑2͒ a time harmonic excitation is applied; the maximum displacement at each point in the image plane is measured using ultrasound and the displacement is imaged ͑Gao et al, 1995;Taylor et al, 2000;Wu et al, 2002͒; or the displacement, using MR, is measured at 4 to 8 equally spaced times in a period cycle, the shear wave speed or the Lamé parameter, , is imaged ͑Greenleaf et al., 1996;Kruse et al, 2000;Braun et al, 2001;Manduca et al, 2001Manduca et al, , 2002Manduca et al, , 2003Ehman et al, 2006;Sinkus et al, 2007͒; ͑3͒ a traveling wave is created using: ͑a͒ a line source created by a sequence of interior radiation force pushes ͑Ber-coff et al., 2002, 2004͒, and a primarily shear wave, with a front, travels outward from the source; the speed of the wave front is imaged ͑McLaughlin and Renzi, 2006aRenzi, , 2006bTanter et al, 2008͒; a point source is created by an interior radiation force push and the local shear wave speed is determined by measuring the time to peak at a nearby location ͑Nightingale et al, 2001a͑Nightingale et al, , 2001bFahey et al, 2005;Palmeri et al, 2006͒; or ͑b͒ two harmonic sources that oscillate at different but nearly the same frequency; the traveling wave speed is imaged ͑Castaneda et al, 2009;Hoyt et al, 2006Hoyt et al, , 2007aHoyt et al, , 2007bHoyt et al, , 2007cHoyt et al, , 2008aHoyt et al, , 2008b…”
Section: Introductionmentioning
confidence: 99%