Jonathan K. Stelter1, Christof Boehm1, Stefan Ruschke1, Maximilian N. Diefenbach1,2, Mingming Wu1, Kilian Weiss3, Tabea Borde1, Stephan Metz1, Marcus R. Makowski1, and Dimitrios C. Karampinos1
1Department of Diagnostic and Interventional Radiology, School of Medicine, Technical University of Munich, Munich, Germany, 2Division of Infectious Diseases and Tropical Medicine, University Hospital, LMU Munich, Munich, Germany, 3Philips Healthcare, Hamburg, Germany
Synopsis
Patients with silicone breast implants
undergoing MR mammography are examined with a water- and fat-suppressed
sequence to verify the implant’s integrity. In parallel, chemical shift
encoding-based water–fat separation has been recently used for quantifying
breast water-fat composition to assess breast density and for extracting
magnetic susceptibility maps to detect breast calcifications. In this work, a
water–fat–silicone separation method is developed for a joint estimation of all
three components and applied with NSA-optimized echo times to simulated
single-voxel data, scanner phantom and in vivo data showing robust species separation
and fat fraction mapping.
Purpose
Silicone implants are commonly used for breast augmentation
or breast reconstruction after mastectomy. MRI is a sensitive method for
monitoring the implant’s integrity to detect possible ruptures1. T2-weighted turbo spin echo acquisitions
employing frequency-selective water suppression and short tau inversion
recovery (STIR) for fat suppression are clinically primarily used to generate
silicone-only images with bright silicone signal2,3.
In parallel, multi-echo gradient echo imaging acquisitions have been also
recently combined with chemical shift encoding-based water–fat separation for
quantifying water–fat composition to assess breast density4
and for extracting magnetic susceptibility maps to detect breast calcifications5-7. However, there is still limited knowledge on how to
simultaneously separate three chemical species in the breast in the presence of
water, fat, and silicone. The present work aims to develop a methodology
for the joint estimation of the field-map as well as water, fat, and silicone
images based on the variable projection (VARPRO) method for chemical species
seperation8,
to find optimal experiment parameters using the Cramér–Rao
analysis9,
and to demonstrate the method for Dixon acquisitions with 4 or 6 echoes in numerical
simulations, in a phantom and in vivo.Methods
Parameter estimation for three species
The
water–fat voxel signal model10
was extended for silicone and its chemical shift of -4.9 ppm11:
$$s(t_n)=(\rho_W+\rho_F(\sum_{p=1}^P\alpha_pe^{i2\pi f_{F,p}t_n})+\rho_Se^{i2\pi f_S t_n})e^{i2\pi \phi t_n}e^{-R_2^*t_n}$$ where $$$t_n$$$ is the echo time shift, $$$\phi$$$ is the field-map, $$$\alpha_i$$$ are the relative amplitudes for the spectral fat model for $$$i\in\{1,..,P\}$$$, $$$ f_{j}$$$ are the resonance frequencies in
consideration of temperature shift effects12
and $$$\rho_j$$$ are the complex signals of the water, fat and silicone components
assuming a common transverse relaxation rate $$$R_2^*$$$.
Residuals
were calculated using the VARPRO method8
and all local minima were extracted and inserted to a single-min-cut variable-layer
graph-cut algorithm13
for field-mapping:
$$\{\rho_W,\rho_F,\rho_S,\phi,R_2^*\}=\operatorname*{argmin}_{\rho_W,\rho_F,\rho_S,\phi,R_2^*}\sum_{n=1}^{N_{TE}}|s(t_n)-y_n|^2$$ where $$$y_n$$$ is the measured signal for the n-th echo and $$$N_{TE}$$$
is
the number of echoes.
Based on the global optimal field-map yielded by the graph-cut, the
water, fat and silicone images can be computed with consideration of the $$$T_2^*$$$ decay14.
Proton density fat fraction (PDFF) maps were calculated with correction for
noise bias effects using magnitude discrimination15,16.
Cramér–Rao
analysis
The
selection of echo times was optimized based on the Cramér–Rao analysis using
the Fisher Information Matrix9,17
to minimize the noise variance expressed by the number of signal averages (NSA)9.
Several
water–fat–silicone-fractions were analyzed based on its noise performance
in dependence on the number and spacing of echoes. For experiment optimization,
the mean NSA for the magnitudes of the species was computed and the minimum
value for different water–fat–silicone-fractions was compared for varying echo
spacings and first echo times.
Numerical phantom
A numerical phantom (20x20x1 voxels) consisting of
different fat and silicone fractions in the range of 0% to 100% with constant $$$R_2^*$$$=50
Hz was simulated based on the water–fat–silicone signal model. A constant echo
spacing with ΔTE$$$\in$$${1, 1.5}ms, TE1=1.7 ms for 4 and 6 echoes and ΔTE=2.75 ms, TE1=1.55
ms for 6 echoes was simulated based on the results of the Cramér–Rao analysis. A
ramp map was specified as field-map and Rician noise18 with SNR=100 was added.
MR measurements
A phantom composed of vials with different water–fat-fractions ([10.0,19.5,36.3,34.9,58.2]%, verified by single-voxel spectroscopy) and a silicone implant was scanned twice with a monopolar
time-interleaved multi-echo gradient echo sequence19
on a clinical 3T scanner (Ingenia/Elition X, Philips Healthcare, Best, The
Netherlands) with NTE=20,
ΔTE=0.45 ms, TE1=1.7 ms, FOV=179.5x179.5x140.4 mm³ and NTE=6, ΔTE=2.75 ms, TE1=1.55
ms, FOV=179.5x179.5x140.4 mm³. From the scanned images, echo times were selected
matching to the phantom simulations.
A
breast scan of a subject with a silicone implant with NTE=6, ΔTE=1.28 ms, TE1=1.58
ms, FOV=384x384x192.4 mm³ using the aforementioned sequence at 3T
was evaluated separately for the first 4 and all 6 echoes.Results
For
the noise performance of the three species, similar patterns were shown (Fig.1):
a local maximum at ΔTE=1 ms, and local minima when the phasors of
the silicone or the main fat component stay the same across TEs. In the latter case, the
separated images suffered from high noise, however, the accuracy of the
field-map estimate was high (Fig.3, NRMSEwater/silicone>10*NRMSEfield-map).
The selection of ΔTE was more robust with 6 echoes than with 4 echoes if
the echo spacing was in a similar range. In vivo results (Fig.5) demonstrated
the feasibility of the method in separating all three species in a large
field-of-view with 6 non-optimized echo times.
Phantom PDFF maps (Fig.4) showed a good agreement to MRS PDFF values, but
higher deviations from the MRS were measured for the larger echo spacing.Discussion & Conclusion
Similar
phasors for the species lead to low differentiation and therefore to more noise
due to broadened peaks in the residual. For large echo spacings (ΔTE=2.75
ms), the distance
between minima in the residual is smaller, such that field-map jumps are more
probable due to the graph-cut algorithm, although high NSA was predicted.
High
PDFF accuracy and low noise in the separated images were achieved for ΔTE=1
ms using 4 echoes and a stronger independence of the results on the echo
spacing was observed using 6 echoes. The feasibility
of the water–fat–silicone separation was also shown in vivo with non-NSA-optimized
6 echo times.Acknowledgements
The present work was supported by the European Research Council (grant
agreement No 677661, ProFatMRI). This work reflects only the authors view and
the EU is not responsible for any use that may be made of the information it
contains. The authors also acknowledge research support from Philips
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