Chris R Bradley1,2, Deirdre McGrath1,2, Eleanor F Cox1,2, and Susan T Francis1,2
1Sir Peter Mansfield Imaging Centre, University of Nottingham, Nottingham, United Kingdom, 2NIHR Nottingham Biomedical Research Centre, Nottingham University Hospitals NHS Trust and University of Nottingham, Nottingham, United Kingdom
Synopsis
Iron-mediated T2* effects are more prominent in
MRE data acquired at 3T compared to 1.5 T, and have been suggested to lead to
failure rates of up to 15% for MRE at 3T. MRE based liver stiffness was
measured using the QIBA recommendation with a 2D gradient‐recalled‐echo MRE
sequence using a 1.5x4.5x10 mm3 acqusition. For comparison, MRE data
was also collected at 4.5mm isotropic spatial resolution. A larger voxel volume
in the MRE acquisition provided higher SNR which in turn resulted in a higher
proportion of voxels being fit for stiffness with confidence >0.95.
Introduction
Magnetic Resonance Elastography (MRE) is becoming an
accepted biomarker of liver injury and is being widely adopted for clinical trials
using the Quantitative Imaging Biomarker Alliance (QIBA) recommendations.
However, higher failure rates of the gradient‐recalled‐echo (GRE) MRE sequences
are observed, particularly in patients with fatty liver disease and/or iron
overload. The iron-mediated T2* effects are more prominent at 3 T
than 1.5 T, and have been suggested to lead to failure rates of up to 15 % for
MRE at 3 T [1]. Here we assess the effect of liver T2* and acquired
spatial resolution on GRE MRE stiffness maps. Methods
5 healthy volunteers
(3M/2F, BMI 23.1 ± 1 kg/m2, age range 24-27 years) and 2 patients
with liver disease (both Non-Alcoholic SteatoHepatitis, NASH) (1M/1F, BMI 29.9 ± 4
kg/m2, age range 31 - 51 years) were recruited. Participants attended
an MRI scan after an overnight fast. Data was collected on a 3 T Philips Ingenia
DDAS scanner (DS Anterior coil + posterior bed coil) to assess liver stiffness as
assessed by MRE, liver tissue T2*.
Data acquisition:
MRE based
liver stiffness was measured using the QIBA recommendation with a 2D GRE
MRE sequence (FOV 360x375 mm, voxel 1.5x4.5x10 mm3, TE = 20 ms, TR =
50 ms, 4 axial slices through the liver, slice gap 1 mm, 1 slice acquired per 18
second breath hold) [2]. For comparison, data was also collected at 4.5 mm
isotropic spatial resolution with matched FOV, TE/TR and slice positioning. For
both acquisitions, the passive acoustic driver (Resoundant, Rochester, MN) was
placed against the lower right chest at the level of the xiphoid in the
midclavicular line, and continuous vibrations of 60 Hz were applied. Liver T2*
maps were collected using multi-echo fast-field echo (mFFE) data acquired
at 12 echo times (TE1 = 2.5 ms, ΔTE
= 2.5 ms, 9 axial slices, 3x3x8 mm3 voxel).
Data Analysis:
T2*: Manual ROIs were drawn on the scanner
computed T2* map images, avoiding large blood vessels, bile ducts,
and edges of the liver parenchyma. Histogram
analysis was then performed to assess the distribution of T2* within
the liver, the mode of the distribution was used to represent tissue T2*
and FWHM to assess heterogeneity.
MRE: From the acquired magnitude and phase
images, the scanner computed elastograms depicting the spatial distribution of
the shear stiffness (ie, magnitude of the complex modulus, |G*|) in kPa, and
confidence masks computed from voxels with confidence values >0.95. Data
were then reshaped to match the resolution of the T2* maps. Liver
stiffness measurements were calculated based on mode values from the elastograms
within the intersection of manually drawn ROIs and confidence masks. The
percentage of the liver in which a confidence mask was formed was computed. In
addition liver stiffness values were computed within each confidence mask for
each spatial resolution of MRE data.Results
Figure 1 shows example liver stiffness maps computed for the
non-isotropic and isotropic resolutions in two participants, one participant with
a short T2* (12 ms mode) and one with a longer T2* (22 ms
mode). For shorter liver T2* values, the percentage of the liver fit
as defined by the confidence map is reduced when using the non-isotropic GRE-MRE
protocol compared with the isotropic protocol, Fig. 2. Mean liver stiffness for
the non-isotropic GRE-MRE protocol was 2.4 ± 2 kPa and 1.9 ±
1.4 kPa for the isotropic protocol.Discussion
Participants who have shorter liver T2*
associated with higher iron content within the liver tissue, have a smaller percentage
of the liver which fits with confidence (confidence >0.95), Fig. 2. The GRE acquisition
is limited to a TE of 20 ms as the MRE motion encoding gradient frequency is
set to match the mechanical driving frequency of 60 Hz. As a result, signal-to-noise ratio is
limited in participants with a shorter liver T2* as rapid dephasing
of the signal occurs during the echo time. We show that by choosing an
isotropic resolution with larger voxel volume (91.1 ml isotropic compared to
67.5 ml for the non-isotropic QIBA recommendation), the goodness of fit in the
stiffness maps is improved, and not dependent on the T2* of the
liver, allowing successful spatial mapping of stiffness over a larger area of
the liver (Fig. 2). Conclusion
Using a isotropic voxel size with larger volume as compared to
the QIBA recommendation for the GRE MRE acquisition provides a higher SNR which
in turn results in a higher proportion of voxels being fit for stiffness with
confidence >0.95 within the liver tissue.Acknowledgements
We would like
to thank the NIHR Nottingham BRC research nurses who conducted patient
enrolmentReferences
1. Dong Wook Kim, So
Yeon Kim, Hee Mang Yoon, Kyung Won Kim and Jae Ho Byun. Comparison of
technical failure of MR elastography for measuring liver stiffness between
gradient‐recalled echo and spin‐echo echo‐planar imaging: A systematic review
and meta‐analysis. J Magn Reson Imaging. 2019 Aug 27.
2. QIBA MR Elastography of the Liver Biomarker Committee.
Magnetic Resonance Elastography of the Liver. Profile Stage: Consensus. QIBA,
May 2, 2018. Available from: http://qibawiki.rsna.org/index.php/Profiles