Abstract
This study evaluates the performance of an acoustic radiation force impulse (ARFI)-based outcome parameter, the decadic logarithm of the variance of acceleration, or log(VoA), for measuring carotid fibrous cap thickness. Carotid plaque fibrous cap thickness measurement by log(VoA) was compared to that by ARFI peak displacement (PD) in patients undergoing clinically indicated carotid endarterectomy using a spatially-matched histological validation standard. Fibrous caps in parametric log(VoA) and PD images were automatically segmented using a custom clustering algorithm, and a pathologist with expertise in atherosclerosis hand-delineated fibrous caps in histology. Over 10 fibrous caps, log(VoA)-derived thickness was more strongly correlated to histological thickness than PD-derived thickness, with Pearson correlation values of 0.98 for log(VoA) compared to 0.89 for PD. The log(VoA)-derived cap thickness also had better agreement with histology-measured thickness, as assessed by the concordance correlation coefficient (0.95 versus 0.62), and, by Bland-Altman analysis, was more consistent than PD-derived fibrous cap thickness. These results suggest that ARFI log(VoA) enables improved discrimination of fibrous cap thickness relative to ARFI PD and further contributes to the growing body of evidence demonstrating ARFI’s overall relevance to delineating the structure and composition of carotid atherosclerotic plaque for stroke risk prediction.
Index Terms—: Atherosclerosis, carotid endarterectomy (CEA), carotid plaque, acoustic radiation force impulse (ARFI) imaging
I. Introduction
STROKE, a leading cause of morbidity and mortality in the United States and around the world, is predominantly ischemic secondary to a thromboembolic event [1]. Ischemic stroke often occurs subsequent to carotid atherosclerotic plaque rupture, so properly identifying rupture-prone carotid plaque is vitally important to stratifying stroke risk [2]. The features of rupture-prone, or ‘vulnerable’, plaques are well described and include thin fibrous cap, large lipid-rich necrotic core, increased vasa-vasorum neovascularization, inflammation, and intra-plaque hemorrhage [3–6]. Among these features, thin fibrous cap conveys the highest hazard ratio (HR) for stroke (intraplaque hemorrhage HR = 4.59 versus necrotic core HR = 3.00) [4]. Therefore, technologies that support accurate measurement of fibrous cap thickness could substantially improve stroke risk assessment and facilitate optimal disease management.
While the relevance of fibrous cap thickness to stroke risk prediction is well known, it is absent from current clinical diagnostic algorithms. The conventional method for evaluating carotid plaque is duplex ultrasound, which estimates stroke risk by Doppler-derived blood flow velocity and degree of stenosis [7]. Because its assessment of stroke risk is based on degree of stenosis, duplex underestimates risk in the case of positive vascular remodeling. Moreover, it is incapable of determining plaque composition and structure, including fibrous cap thickness [8].
Alternatives to duplex are emerging, including MRI [9–11], optical techniques based on optical coherence tomography [12, 13] and optical spectroscopy [14, 15], virtual histology [16, 17], and elastographic methods, all of which aim to evaluate the composition and structure of carotid atherosclerotic plaque. Elastographic approaches evaluate plaque composition and structure by interrogating mechanical properties deduced from tissue displacement in response to intrinsic or extrinsic mechanical excitations. For example, in response to intrinsic arterial pulsation, Roy-Cardinal et al developed a plaque component classification scheme that uses homodyned-K parametric maps and elastograms to identify ruptured fibrous cap with an AUC of 0.97 [18, 19]. Further, Hansen et al demonstrated compound ultrasound strain imaging methods for identifying fibrous plaques [20] and Schaar et al and de Korte et al demonstrated intravascular elastography for characterizing plaque components [21, 22]. In addition, Nayek et al have developed methods for estimating carotid artery strain using synthetic aperture imaging [23, 24].
Using Acoustic Radiation Force Impulse (ARFI) imaging, Czernuszewicz et al demonstrated ARFI-induced peak displacement (PD) for measuring fibrous cap thickness [25]. In 25 patients undergoing clinically indicated carotid endarterectomy, carotid plaques were imaged in vivo immediately prior to surgery. Imaging results were interpreted by three trained, blinded readers, and the assessments were compared to an expert pathologist’s interpretation of the spatially matched histology of the extracted plaque specimens. The best reader outcomes for average fibrous cap thickness were in close correlation with the histologically measured thickness (R = 0.89), but Bland Altman analysis revealed a statistically significant positive bias of 0.12 ± 0.30 mm. Further, in silico studies by Czernuszewicz et al indicated that for the employed system parameters, the minimum measurable fibrous cap thickness was 0.2 mm, suggesting in vivo overestimation of fibrous cap thicknesses smaller than this level [26].
A likely cause of fibrous cap thickness overestimation by ARFI PD assessment is improper delineation of the boundaries between the lumen and the fibrous cap and between the fibrous cap and the underlying lipid-rich necrotic core (LRNC) or intraplaque hemorrhage (IPH). Therefore, a method for improving differentiation of fibrous cap boundaries could improve cap thickness measurement to support more accurate carotid plaque risk assessment. Rather than ARFI PD, a potential strategy is to employ an alternative ARFI-derived parameter, Variance of Acceleration (VoA), which has been demonstrated for differentiating subcutaneous hemorrhage from surrounding soft tissue [27] and for identifying carotid plaque composition and structure [28].
As its name implies, VoA is calculated as the variance of the second time-derivative of ARFI induced tissue displacement. The second time-derivative is a high-pass filtering operation that amplifies variance, or “jitter”, in the displacement estimate. Therefore, VoA is directly related to jitter magnitude (σ), which is derived from the Cramer-Rao lower bound [29] as,
(1) |
where f is the center frequency, T is the tracking kernel size, B is the bandwidth, ρ is the correlation coefficient, and SNR is the signal to noise ratio. When the first three parameters, f, T, and B, are maintained constant, jitter magnitude varies specifically due to SNR and signal decorrelation in the region of analysis. Considering that signals will be more decorrelated and have lower SNR when they originate from luminal blood than from plaque fibrous cap, VoA is relevant to differentiating lumen-cap boundaries. Similarly, considering that signals will be more decorrelated and have lower SNR when they originate from soft, hypoechoic LRNC and IPH, VoA is relevant to discriminating cap-underlying plaque boundaries. In this study, we present the novel application of ARFI VoA to supporting more accurate and precise fibrous cap thickness measurement in human carotid plaque, in vivo, relative to ARFI PD. This hypothesis is herein tested using ARFI data previously acquired from patients undergoing clinically indicated carotid endarterectomy (CEA), with histological validation [25].
II. Methods
A. Patient Recruitment
Patient recruitment and imaging protocol are described in detail on our prior work [25]. A total of 25 patients undergoing clinically indicated CEA were recruited from UNC Hospitals. Inclusion criteria included either asymptomatic carotid artery disease with >60% Doppler-indicated stenosis and unresponsive to medical management or symptomatic carotid artery disease with a stenosis suspected to be the source of emboli. All procedures were approved by the institutional review board (IRB), and informed written consent was given from each study participant.
B. ARFI Imaging
A Siemens Acuson Antares research imaging system (Siemens Healthcare, Ultrasound Division) was used for in vivo imaging with a VF7–3 linear array transducer. ARFI excitation pulses were 300-cycles at 4.21 MHz, tracking pulses were 2-cycles at 6.15 MHz, and acquisitions were timed to diastole using electrocardiogram gating. From the acquired radio frequency data, ARFI-induced displacements were measured using normalized cross correlation (NCC) with a 1.5λ (376-μm) kernel, two-stage interpolation, and linear motion filtering [30].
A registered sonographer (M.C.C.) acquired all imaging data before patient sedation, on the same day of surgery. The time interval between imaging and specimen extraction was approximately four hours. The plaque to be removed by CEA was identified from prior ultrasound imaging sessions archived in the patient’s medical record and was typically the plaque with the greatest stenosis. Before completing the imaging session, the transducer was rotated 90°, and transverse B-modes and CINE loops of the carotid bifurcation were obtained to aid in sample alignment (see Section II-D below).
C. ARFI-Derived Parameter Estimation
ARFI PD and VoA parameters were calculated from ARFI-induced displacement versus time profiles. From the displacement profiles, which were obtained using one-dimensional (axial) normalized cross correlation [30], PD was calculated as the maximum displacement per pixel, as described in [31]. VoA was calculated as the unbiased variance of the second time derivative through the total ensemble time per pixel:
(2) |
where x and y are axial and lateral pixel coordinates, respectively, t is ensemble time, k is the total number of ensemble time samples, Acc is acceleration, and μAcc is the mean of Acc.
D. Histology
CEA specimens were harvested, μCT imaged (Scanco 40, Scanco Medical AG, Bassersdorf, Switzerland), and processed for spatially-matched histological validation. Spatial alignment was performed by matching the histological cutting plane with the imaging frame using the μCT image as reference for orientation before paraffin embedding. The orientation and alignment process were performed by a separate reviewer, before and independent of the quantitative analysis described below. A more detailed description of the process for aligning ARFI and histology data is contained in Czernuszewicz et al [25].
The aligned microscopy images were divided into four laterally adjacent, equally sized subsections spatially corresponding to four laterally adjacent, equally sized quarters in the ARFI images. The histology subsections were read by a pathologist with expertise in atherosclerosis (J.W.H.), who hand-delineated fibrous caps using a custom graphical user interface (GUI) developed in Matlab (Mathworks Inc., Natick, MA, USA) for the previous blinded-reader study [25]. In the parametric ARFI image subsections, fibrous caps were segmented using a semiautomatic k-means clustering method [28, 32]. Centroids from each fibrous cap were calculated from the parametric images aligned with histology, and these centroids were input to the k-means algorithm for segmenting k regions, where k is the number of fibrous cap areas identified by the pathologist on each histology slide. A more detailed description of this clustering method is contained in Torres et al [28].
E. Data Analysis
Exclusion criteria were applied to the data collected from the 25 patients to ensure high-quality and well-matched histology and ARFI data. First, plaque specimens that were damaged or fractured during surgery were excluded. Second, plaques imaged with the lumen-plaque boundary outside the axial range of ARFI imaging (spanning ± 5 mm from the focal depth) were excluded. Third, carotid plaques without the presence of a fibrous cap in histology were excluded. After data exclusions, 14 fibrous caps were retained for comparison of fibrous cap thickness measurement by ARFI PD and VoA parameters.
ARFI PD and VoA outcomes were rendered into two-dimensional parametric images, with VoA depicted as its decadic logarithm, denoted log(VoA), to increase dynamic range. For display purposes, both PD and log(VoA) images were normalized to the mean value within the plaque ± two median absolute deviations (MAD). The linear relationship between histology-derived fibrous cap thickness measurements and imaging-derived thickness from PD and log(VoA) images were visually assessed in scatterplots and tested by Pearson correlation. Bland-Altman analysis was performed to evaluate the agreement between fibrous cap thicknesses derived from ARFI and histology. Finally, the concordance correlation coefficient (CCC), a measure of both the precision and accuracy of imaging-derived thickness compared to histology-derived thickness, was calculated for both ARFI PD and ARFI log(VoA), with the CCC closest to 1 considered to be the most accurate and precise measurement [33]. All statistical analyses were performed using Matlab (Mathworks Inc., Natick, MA, USA).
III. Results
For a representative plaque from a 53 year-old symptomatic female, B-Mode, ARFI PD, and ARFI log(VoA) images are shown in Figure 1, without (left column) and with (right column) the automatically segmented fibrous cap regions shown in white. The fibrous cap thicknesses derived from the segmented regions in PD and log(VoA) images were 0.93 and 0.90 mm, respectively, while the thickness of the fibrous cap hand-delineated by the pathologist was 0.84 mm. For reference, the plaque boundary hand-delineated from ARFI PD images by the best-performing radiologist reader in [25] is shown in black.
Figure 2 shows another carotid plaque example from a symptomatic 45-year-old female. Again, the automatically segmented fibrous caps are shown in white in the right column. These segmentations yielded fibrous cap thickness measures of 0.99 and 0.90 mm for ARFI PD and log(VoA), respectively, while the histology-derived thickness was 0.91 mm.
Figure 3 shows a third plaque example from a symptomatic 59-year-old male. In this case, the fibrous cap thicknesses derived from automatic segmentation of PD and log(VoA) images were 1.40 and 1.35 mm, respectively, while the fibrous cap thickness measured from the spatially matched histology was 1.26 mm.
Figure 4 illustrates median ARFI PD (a) and log(VoA) (b) fibrous cap thickness measurements plotted versus the histological validation standard for the evaluated plaques. It can be observed that median PD-derived fibrous cap thickness measurements correlated more weakly with the validation standard than corresponding log(VoA) measures. The R2, sum squared error (SSE) values were (0.79, 0.19) for PD and (0.97, 0.03) for log(VoA). The concordance correlation coefficient (CCC) was 0.62 for PD and 0.95 for log(VoA), which indicates more precision and agreement between log(VoA) and histology than PD and histology. Additionally, the correlation between histology with PD was 0.88 (95% CI: 0.38 to 0.90; P = 0.001), while the correlation with log(VoA) was stronger, at 0.98 (95% CI: 0.94 to 0.99, P<0.0001). In figure 5, Bland-Altman results indicate that the coefficient of variation was 16% for PD-derived median fibrous cap thickness versus 6.3% for log(VoA)-derived median fibrous cap thickness. The bias in PD-derived median fibrous cap thickness, 0.10 mm, was statistically significant, while the 0.05 mm bias in log(VoA)-derived median fibrous cap thickness was not statistically significant (p<0.05).
Figure 6 illustrates minimum (a) PD and (b) log(VoA) fibrous cap thickness measurements plotted versus the histological validation standard. The (R2, SSE) values were (0.74, 0.22) for PD and (0.95, 0.05) for log(VoA). The concordance correlation coefficient (CCC) was 0.61 for PD and 0.87 for log(VoA). Figure 7 shows Bland-Altman results for the minimum fibrous cap thickness measurements. The coefficient of variation for minimum fibrous cap thickness measurement was 20% for PD versus 8.6% for log(VoA).
Figure 8 illustrates maximum (a) PD (a) and (b) log(VoA) fibrous cap thickness measurements plotted versus the histological validation standard. For the maximum fibrous cap thickness measurements, the (R2, SSE) values were (0.67, 0.35) for PD and (0.84, 0.23) for log(VoA). The concordance correlation coefficient (CCC) was 0.55 for PD and 0.89 for log(VoA). Figures 9 shows Bland-Altman results for maximum fibrous cap thickness measurements. The coefficient of variation for maximum fibrous cap thickness measurement was 21% for PD versus 16% for log(VoA).
The axial locations of PD- and log(VoA)-derived lumen-cap and cap-LRNC boundaries were compared. The median difference in {PD – log(VoA)} lumen-cap boundary position was −0.33 ± 0.21 mm. The median difference in {PD −log(VoA)} cap-LRNC boundary position was +0.21 ± 0.10 mm.
IV. Discussion
In Figure 1, the boundary using the ARFI PD image yields a median fibrous cap thickness measurement that is 10.71% larger than the histological validation standard, while the thickness derived using log(VoA) is 7.14% larger. These data, suggesting that median fibrous cap thickness measurement by log(VoA) is in better agreement with the histological validation standard than that by PD, are consistent with the results observed in Figure 2 (relative to histology, 8.79% larger median fibrous cap thickness by PD versus 1.10% larger by logVoA) and Figure 3 (relative to histology, 11.11% larger median fibrous cap thickness by PD versus 7.14% larger by logVoA). Over these plaques, median fibrous cap thickness measured by PD had an absolute difference of 0.10 ± 0.26 mm compared to histology, whereas fibrous cap thickness measured by log(VoA) had an absolute difference of 0.05 ± 0.09 mm compared to histology.
Figure 4 illustrates that, over all 14 examined plaques, median fibrous cap thickness measured by log(VoA) is more strongly correlated (R2 = 0.97) with the histological validation standard than that measured using PD (R2 = 0.79). Further, the CCC of 0.95 for log(VoA) versus 0.62 for PD suggests that ARFI log(VoA) enables more accurate and precise measurement of median fibrous cap thickness than ARFI PD. Figure 5 further supports that median fibrous cap thickness measurement is more accurate and precise by log(VoA) than by PD. While neither parameter’s bias was statistically significant (p<0.05), log(VoA) bias was 0.05 mm versus 0.10 mm for PD. Similarly, the reproducibility coefficient (RPC) and coefficient of variation (CV) were lower for log(VoA) (0.10 and 6.3%) than for PD (0.26 and 16%) median fibrous cap thickness measurements.
While the accuracy and precision of median fibrous cap thickness measurement suggest general utility, ability to measure minimum fibrous cap thickness indicates relevance to identify caps with high rupture potential. In figures 6 and 7, minimum fibrous cap thickness measures were more strongly correlated to the histological standard (R2 = 0.95 v. 0.74) and had lower error (SSE = 0.22 v. 0.05) when measured by log(VoA) versus PD. Moreover, log(VoA) measures of minimum fibrous cap thickness had lower RPC and CV (0.12 and 8.6%) than PD measures (0.27 and 20%). Interestingly, both log(VoA) and PD measures of minimum fibrous cap thickness had the same bias (0.11), but neither bias was statistically significant (p<0.05). These results show that log(VoA) enables more accurate and precise measures of minimum fibrous cap thickness than PD, suggesting that rupture potential is better determined by log(VoA).
Like median and minimum, log(VoA) outperforms PD in terms of accuracy and precision of maximum fibrous cap thickness measurement. Figure 8 shows that log(VoA) maximum fibrous cap thickness measures are more strongly correlated to the histological standard (R2 = 84 v. 0.67) and had lower error (SSE = 0.23 v. 0.35) than PD. Further, in fig. 9, log(VoA) had greater precision than PD (RPC = .29 v. .42; CV = 16% v. 21%). Finally, while both log(VoA) and PD measures of maximum fibrous cap thickness had statistically significant bias (p>0.05), the log(VoA) bias was −0.08 mm, while the PD bias was 0.08.
More accurate and precise median, minimum, and maximum fibrous cap thickness measurement by log(VoA) versus PD is consistent with results previously reported by Torres et al [28], which showed that contrast-to-noise ratio (CNR) for differentiating collagen from LRNC was 3.3 times greater by log(VoA) than by PD and that CNR for discriminating stiff from soft plaque features was 3.6 times greater. However, an unexpected outcome is that, for both log(VoA) and PD, maximum fibrous cap thickness measurement performance was worse than median and minimum cap thickness measurement performance. Specifically, maximum thickness measures were less correlated with the histological standard (PD R2 = 0.67 for maximum v. 0.79 for median and 0.74 for minimum, log(VoA) R2 = 0.84 for maximum v. 0.97 for median and 0.95 for minimum), had higher error (PD SSE = 0.35 for maximum v. 0.19 for median and 0.22 for minimum, log(VoA) SSE = 0.23 for maximum v. 0.03 for median and 0.05 for minimum), and had lower precision (PD RPC = 0.42 for maximum v. 0.26 for median and 0.27 for minimum, log(VoA) RPC = 0.29 for maximum v. 0.10 for median and 0.12 for minimum). The reasons for the observed poorer maximum fibrous cap thickness performance are yet to be determined.
It is interesting to consider that, relative to PD, log(VoA) yielded thinner fibrous cap delineations on both the lumen-cap (median difference of −0.33 ± 0.21 mm) and cap-LRNC (median difference of 0.21 ± 0.10 mm) interfaces. These data suggest that log(VoA) improves discrimination of fibrous cap from LRNC (which is consistent with results reported in [28]) and from luminal blood (which has not been previously shown). Future studies are needed to more comprehensively evaluate log(VoA)’s potential for discriminating plaque from blood under variable flow and clutter conditions.
Aspects of the study design may have influenced outcomes. First, fibrous cap thickness measurement performances by ARFI PD and log(VoA) were evaluated relative to histology-derived fibrous cap thickness, which was considered to be a validation standard. However, inconsistency between fibrous cap thickness in histology and ARFI images could arise due to plaque stretching and/or compression during in vivo imaging or due to sample shrinkage during histological processing. Plaque stretching and compression were minimized by acquiring in vivo data with gating to diastole, and specimens that were evidently warped were excluded from the study.
In addition, it is important to consider that the ARFI imaging focal depth could have impacted fibrous cap thickness measurement. In this study, the imaging focal depth was determined by the position of the carotid plaque and ranged from 1.8 to 2.3 cm across the examined plaques. Generally speaking, deeper focal depths experience lower radiation force magnitude [34, 35], and therefore smaller displacements, which could reduce fibrous cap contrast in PD and log(VoA) images. Further, tracking ARFI-induced displacements at deeper focal depths results in lower SNR and higher jitter, to the potential detriment of fibrous cap contrast by both PD and log(VoA). The impact of ARFI focal depth on fibrous cap thickness measurement is a topic of ongoing investigation.
Along with focal depth, the implemented tracking center frequency (6.15 MHz) and normalized axial cross-correlation displacement tracking kernel size (1.5λ) could have impacted fibrous cap thickness measurement. Czernuszewicz et al showed that for these values, the expected minimum fibrous cap thickness measurement resolution is 0.2 mm [26], which is comparable to the thickness of the thinnest fibrous cap included in this study. Notably, no caps thinner than 0.2 mm were contained in the available data set and, therefore, could not be evaluated. Using higher tracking center frequencies and/or smaller displacement tracking kernel sizes could improve thickness resolution, but at the potential cost of SNR and increases in jitter that impact fibrous cap contrast in PD and log(VoA) images. Comparing in vivo ARFI fibrous cap thickness measurement across tracking center frequencies and kernel sizes is work in progress.
Another factor impacting ARFI-based fibrous cap thickness measurement is reverberation clutter, which can be accentuated when calcium deposits are present in the plaque [25]. Clutter artifact corrupts displacement estimation as well as signal correlation and SNR and therefore diminishes fibrous cap contrast in PD and log(VoA) images. Advanced clutter filters and harmonic imaging could suppress clutter artifact and improve fibrous cap thickness measurement [36, 37].
Finally, while the results reported herein suggest that in vivo, human carotid fibrous cap thickness measurement is better supported by log(VoA) than by PD imaging, and while Bland Altman analyses and the CCC showed that performance improved when using log(VoA) in comparison to PD, the work is pilot in nature. After exclusions, only fourteen examples of fibrous caps with spatially matched histological validation were evaluated. Larger studies are needed in the future to more comprehensively compare ARFI PD and log(VoA) for fibrous cap thickness measurement.
V. Conclusions
This study demonstrates the potential of ARFI log(VoA) for improving fibrous cap thickness measurement in comparison to ARFI PD. In fourteen human carotid plaques, imaged in vivo, log(VoA)-derived fibrous cap thickness is more strongly correlated to true thickness, has a higher CCC, and is less variable than PD-derived fibrous cap thickness. Overall, these results add to the growing body of evidence that suggests that ARFI-based imaging, evaluating log(VoA) in particular, is relevant to delineating carotid plaque structure and composition for vulnerable carotid plaque detection.
Acknowledgment
The authors would like to thank Siemens Healthcare, Ultrasound Division, Issaquah, WA, USA, for technical support.
This work was supported in part by NIH grants R01HL092944, R01DK107740, R01NS074057, and T32HL069768.
Contributor Information
Gabriela Torres, Joint Department of Biomedical Engineering, University of North Carolina at Chapel Hill, Chapel Hill, NC 27514 USA, and North Carolina State University, Raleigh, NC 27695 USA..
Tomasz J. Czernuszewicz, Joint Department of Biomedical Engineering, University of North Carolina at Chapel Hill, Chapel Hill, NC 27514 USA, and North Carolina State University, Raleigh, NC 27695 USA. He is now with SonoVol, Inc., Durham, NC 27713 USA..
Jonathon W. Homeister, Department of Pathology and Laboratory Medicine, University of North Carolina at Chapel Hill, Chapel Hill, NC 27514 USA.
Mark A. Farber, Department of Surgery, University of North Carolina at Chapel Hill, Chapel Hill, NC 27514 USA.
Melissa C. Caughey, Joint Department of Biomedical Engineering, University of North Carolina at Chapel Hill, Chapel Hill, NC 27514 USA, and North Carolina State University, Raleigh, NC 27695 USA
Caterina M. Gallippi, Joint Department of Biomedical Engineering, University of North Carolina at Chapel Hill, Chapel Hill, NC 27514 USA, and North Carolina State University, Raleigh, NC 27695 USA..
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