Milica Medved1, Marco Vicari2, and Gregory S Karczmar1
1Radiology, University of Chicago, Chicago, IL, United States, 2Fraunhofer MEVIS, Bremen, Germany
Synopsis
Strong T2* weighting has allowed high sensitivity of HiSS breast MRI to
cancer, but in whole-breast imaging, contrast is compromised due to necessarily
shorter echo trains. k-space
under-sampling techniques such as compressed sensing (CS) yield time savings
that can be traded for longer echo trains and stronger T2* weighting,
potentially increasing breast HiSS MRI performance in screening and diagnostic
applications. Our CS simulation resulted
in minimal reduction in spatial resolution for acceleration factor R = 2,
showing CS to be a promising acceleration strategy for HiSS MRI, allowing
longer echo trains and stronger T2* weighting.
INTRODUCTION
Because of the risks of
gadolinium contrast use, large MRI breast cancer screening programs are not
viable without effective non-contrast enhanced MR sequences. EPSI-based High Spectral and Spatial
resolution (HiSS) breast MRI has high diagnostic utility for lesion
characterization, and could also potentially serve as a powerful tool for
non-contrast enhanced breast cancer screening. [1, 2] However, whole breast HiSS MRI is currently
implemented with short echo trains to reduce run time; this potentially reduces
sensitivity. Compressed sensing (CS) acceleration
reduces the number of phase encoding steps per slice, producing significant
time savings which in HiSS MRI could be traded for longer echo trains. This would restore T2* weighting and higher
spectral resolution that could facilitate effective breast cancer screening and
diagnostic applications. Here, we demonstrate
the application of CS to in vivo
breast HiSS imaging, and evaluate its effect on image
quality.METHODS
Whole-breast HiSS MRI was acquired on 1 patient on a Philips Achieva
3T-TX scanner, (2D multislice, 384 mm FOV, 0.8x0.8x3 mm3 voxels in 60
slices, TR/TE 2350/23 ms, 23 echoes, 23.9 Hz spectral resolution, scan time 7.5
min, SENSE factor 3 (L/R)). Because of
SENSE reconstruction, k-space data was not directly available; instead, k-space
data were calculated from reconstructed complex gradient echo images. CS acceleration was simulated by under-sampling
the full k-space dataset, with three acceleration factors R. For R = 1, full k-space information was retained. For R = 2: variable-density random under-sampling,
by a factor of 2 (pattern did not vary from echo to echo) was applied, and for R
= 3 the same algorithm was applied, but using a factor of 3 under-sampling. After retrospective under-sampling, full
k-space information was reconstructed for R = 2 and R = 3 using CS with
sparsifying operators in spatial total variation and wavelet domains. [1] Complex gradient echo images, preserving
phase information along the echo train, were reconstructed for R = 2 and 3. The complex gradient echo images were Fourier
transformed along the temporal direction in order to obtain proton spectra in
each individual voxel. The spectra
resolved water and fat peaks, which were fit to Lorentzian functions in order
to extract the pure water signal above the baseline and any lipid peak tails. [2] The water peak information thus obtained was
used to generate water peak height images, with excellent fat suppression. [3] In order to quantify loss of image resolution
with application of CS algorithm, signal profiles across the lateral or frontal
edge of the chest wall muscle were extracted, to approximate a sharp edge. The profiles were positioned to be parallel
to the readout and phase encoding directions and perpendicular to the chest
wall. The profiles’ derivatives were fit
to a Gaussian function which, after a Fourier transform, provided the
modulation transfer function (MTF) for datasets with R = 1, 2, and 3. The loss of image resolution in both the
readout and phase encoding direction was evaluated by comparing k values for an
equal MTF level, with R = 1 dataset and k = 0.625 1/mm (equivalent to 0.8 mm
resolution) used as a baseline.RESULTS
R = 2 and R = 3 datasets resulted in an effective spatial resolution in
the phase-encoding direction of 0.88 and 1.33 mm, respectively, which compares
to 0.8 mm for R = 1. The effective spatial
resolution in the readout direction was 0.87 and 0.90, for R = 2, and 3, respectively.DISCUSSION
Our results indicate that minimal blurring due to CS implementation can
be expected with two-fold acceleration.
This would allow significant acceleration without correspondingly increased
image quality loss. The sensitivity of
HiSS MRI to breast lesions could be increased to allow non-contrast enhanced
screening and diagnostic applications.CONCLUSION
CS acceleration simulation in in vivo breast HiSS MRI resulted in minimal
reduction in spatial resolution for an acceleration factor of R = 2. Therefore, CS is a promising acceleration
strategy for HiSS MRI. Faster HiSS
acquisitions with longer echo trains and increased T2* weighting could improve sensitivity
of HiSS breast imaging to breast lesions, and facilitate screening and
diagnostic applications without the need to inject contrast media.Acknowledgements
No acknowledgement found.References
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