Subashini Srinivasan1, Brian A Hargreaves1, and Bruce L Daniel1
1Radiology, Stanford University, Stanford, CA, United States
Synopsis
Three-dimensional breast dynamic
contrast-enhanced imaging is susceptible to deformable motion and affects both
semi-quantitative and pharmacokinetic parameters. B-Spline motion registration
with a mutual information metric is often used to register DCE images but is
sometimes susceptible to introduction of new motion. Here we have introduced a
fat-based motion registration, using a mean-squared-difference signal metric,
to register the water images without introducing new motion. The acquired
images and both registration methods were qualitatively assessed in 16 breasts.
Voxel-by-voxel pharmacokinetic mapping was also performed in 21 tumors. Our
results show that fat-based registration can be used to register the water
images with improved image quality and reduced errors in quantification.Introduction
Breast dynamic contrast-enhanced (DCE) imaging often
acquires many three-dimensional datasets for over 7.5 minutes and is
susceptible to deformable motion. This motion affects both semi-quantitative
measures such as washout slope as well as voxel-by-voxel pharmacokinetic parameters,
and therefore needs to be corrected before quantification. B-Spline based motion registration [1] is
commonly used to register deformed 3D images along with a normalized mutual
information metric to account for temporally varying water signal due to
contrast dynamics. Although this method reduces motion in several cases, additional
jittery motion is also sometimes introduced with the mutual information metric.
Here we introduce a fat-based registration method, using mean-squared-difference
signal metric, to register the water images without introducing new
jitteriness.
Methods
The water signal in the breast changes with the
contrast concentration; however, the fat signal does not exhibit temporal
dynamics (Fig.1) and hence the smoothed temporal fat signal changes can be used
to estimate the motion when Dixon-based methods are used. 3D fat-based motion
registration was performed with mean-squared-difference signal as the metric and
b-spline transformation with a grid dimension of five along each direction. Water
images were then warped using the corresponding fat-based b-spline transform. The
steps of this registration method are detailed in Fig.2.
The original image series and images from both
fat- and water-based registration methods were evaluated in 14 patients (2
bilateral) with known masses. 3D RF-spoiled gradient echo fat-water separated
DCE images were acquired using DISCO [2], a pseudorandom ky-kz
sampling scheme enabling a favorable tradeoff between temporal and spatial
resolution, on a 3T scanner (GE Healthcare, Waukesha, WI). The imaging parameters were: FOV= 270×324 mm,
TR/TE1/TE2= 6.3/2.2/3.3 ms. One pre-contrast and four
post-contrast images were acquired with high spatial resolution of 0.5×0.6×1.0
mm and low temporal resolution of 2 min. Fourteen images were acquired during
the wash-in period with high temporal resolution of 13s and lower spatial
resolution of 0.5×1.2×2.0 mm. All the images were reconstructed to lower
spatial resolution before performing fat and water-based registration.
The image quality of the original
and the registration methods were presented in random order to 2 experienced readers
and scored in a scale of zero to two. A score of 0 was given to images with
minimal motion of < 2 voxels in each direction in both tumor and surrounding
tissue. Similarly a score of 1 was given to residual motion of 2 to 4 voxels
and score of 2 for > 4 voxels. The readers also ranked the images from best
(rank 1) to worst (rank 3).
Voxel-by-voxel
pharmacokinetic mapping was also performed using a standard Tofts model [3] with
modified Fritz-Hansen AIF as well as modified local density
random walk (mLDRW) Dispersion model [4] in 21 tumors. The average error
between the data and the fitted model was evaluated over the tumor ROI for both
the models using the original images as well as fat-based registered images.
Results
Fig.3 shows an example dense breast movie
(viewable in browser) with minimal motion (white arrows). The water-based
registration method introduces jittery motion (cyan arrows), and the fat-based
registration reduces motion without introducing new motion, even in this case of
minimal fat. The average image quality score of the original images, water-based
and fat-based registration methods are tabulated in Fig.4a. Friedman test showed
significant (P<0.01) differences
between the three datasets. All the fat-based registered images were scored better
than the original images. All the four images of fat-based registration that
were ranked 2 had identical image quality score compared to water-based
registration. Three to four water-based registered datasets received a score of
2 that was equal to or higher than the original images due to insufficient
motion compensation or new motion.
Fig.5 compares example wash-out slope maps (top
row), kep map of the Tofts model (middle row) and kappa map of the mLDRW model
between the original and fat-based registration methods. These maps show the
erroneous enhancement in the edges (arrows) that are corrected after motion
correction. The average error between the data and the fitted model is also
reduced after motion correction (Fig. 4b).
Discussion
Our results indicate that the fat-based
registration of breast DCE images reduced the motion compared to both original
and water-based registration method and improved image quality. Both
registration methods, however, also introduced minimal blurring in patients
with motion >4 voxels. The image quality including blurriness will be
further evaluated in more patients with significant motion.
Conclusion
Fat-based breast DCE registration can be used to
register the water images with improved image quality and reduced errors in
quantification.
Acknowledgements
Research support from NIH R01 EB009055 and
GE HealthcareReferences
[1] Rueckert D, et al., IEEE Transactions on
medical imaging, 1999:18
[2] Saranathan M, et al., JMRI 2014;40 (6):1392-1399
[3] Tofts P, et al., JMRI 1999;10:223-232
[4] Mischi M, et al., IEEE EMBS, 2013