Tomoelastography by multifrequency wave number recovery from time-harmonic propagating shear waves☆
Graphical abstract
Introduction
Since the advent of elastography in the early 1990s, stiffness measurements of biological tissues have become routine diagnostic applications of sonography (Ophir et al., 1991, Parker et al., 1990) and magnetic resonance imaging (MRI) (Muthupillai et al., 1995, Plewes et al., 1995). Today, many, if not all, commercial ultrasound scanners have one or more elastography options (Cosgrove et al., 2013). Major MRI vendors also offer elastography as a tool for the noninvasive staging of liver fibrosis based on a standardized procedure approved by the US Food and Drug Administration (Venkatesh and Ehman, 2015). Many factors have contributed to the success of elastography, including quantitative measurements, non-invasive acquisitions, no need for contrast medium, and high sensitivity to multiscale tissue structures.
The standard output of elastography is an image of stiffness, elasticity or wave speed, which is known as an elastogram and mapped as a colored overlay onto a high-resolution anatomical image (Cosgrove et al., 2013, Venkatesh et al., 2013). In general, the resolution of the elastogram is lower than that of the underlying gray-scale sonographic or MR image due to noise and unknown boundary conditions in the elasticity reconstruction procedures (Doyley, 2012, Manduca et al., 2001). For example, stress accumulation at tissue interfaces, or wave nulls due to interfering propagating waves, or acoustic shading, often cause artifacts in the elastograms, necessitating masking in order to blank out areas of unreliable stiffness values. For this reason, the main clinical use of quantitative elastography is measuring the elasticity of entire organs or large Regions of Interest (ROIs).
Different approaches have been proposed to overcome limits in the resolution of anatomical details in elastography (Baghani et al., 2011, Honarvar et al., 2013, Manduca et al., 2003, McGarry et al., 2012). One promising method is multifrequency magnetic resonance elastography (MMRE), based on multifrequency dual elasto-visco (MDEV) inversion, in which several harmonic wave fields are acquired and averaged prior to inversion of the wave equation (Hirsch et al., 2014, Papazoglou et al., 2012). With use of this strategy, regions of low elastic strain and therefore low signal-to-noise-ratio (SNR) in one frequency are compensated for by higher strain-SNR in another frequency in order to reduce the influence of amplitude nulls on the elastogram. Although this method was found to be sensitive enough to resolve distinct mechanical properties of thin tissue layers, such as renal cortex (Streitberger et al., 2014b), cortical gray matter (Braun et al., 2014), nucleus pulposus (Streitberger et al., 2015) and uterine myometrium (Jiang et al., 2014), the overall quality of the resulting elastograms suffered from noise, especially in regions of low wave amplitudes. In general, noise is enhanced by higher-order spatial derivatives of the wave field required for the inversion of the wave equation (Manduca et al., 2001).
We here capitalize on the strength of MDEV inversion in compensating for wave amplitude nulls and address the key issue of noisy wave inversion by first-order derivative-based reconstruction of in-plane wave numbers (k-MDEV). Restriction to in-plane wave propagation accounts for the fact that in abdominal MRE, the acquired field's number of slices is much less than its in-plane length or width (e.g., 5 points in Huwart et al., 2008, 2–4 points in Venkatesh et al., 2013, 10 points in Guo et al., 2014), rendering it essentially 2-D. We thus aim at a slice-wise graphic representation of wave speed without masked regions, in an approach named here tomoelastography (from ancient Greek τόμος `slice').
Feasibility of k-MDEV based MMRE is first demonstrated in a phantom which was previously used for the validation of MMRE and is accordingly well characterized (Papazoglou et al., 2012). k-MDEV is then applied to cohorts of abdominal and pelvic acquisitions, with measurements including liver, spleen and uterus. Finally, to illustrate the clinical value of the method, results from patients with fibrotic and tumorous livers are presented.
Section snippets
Subjects
MMRE data were acquired of two cohorts of healthy volunteers as described in previous studies: Guo et al. (2014) (liver and spleen, N = 10) and Jiang et al. (2014) (uterus and cervix, N = 16). Additionally, to investigate diagnostic potential, k-MDEV was applied to abdominal acquisitions of two patients with biopsy-proven fibrosis of grades F2 and F4, respectively, according to the METAVIR score, and one patient with hepatocellular carcinoma (HCC). These latter data were newly acquired for this
Validation
Fig. 3 illustrates the noise robustness of wave number (k) recovery as compared to direct Helmholtz inversion (DI). The graphs represent spatially averaged inversion results of simulated 1D-complex-valued waves of 30 and 60 Hz vibration frequency at different noise levels. Gaussian noise was added to a complex harmonic function with 2 mm pixel spacing before it was treated by the same filters (in 1D) as elsewhere in the study. The resulting waves were subsequently analyzed by k
Discussion
We have presented a simple, noise-robust method of reconstructing high-resolution elastograms from multi-frequency, multi-component shear wave data acquired by MRE. As shown by the data presented in Table 2, the shear speed values obtained in all tissues so far analyzed with the new method fall into the ranges of values reported in the literature. As illustrated by the in vivo figures, our results outperform previous elastograms in terms of detail resolution, noise robustness, and intra-tissue
Acknowledgment
Financial support from the German Research Foundation (Sa901/10) is gratefully acknowledged.
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This paper was recommended for publication by Nicholas Ayache.