Chao Li1,2, Jinwei Zhang1,3, Jiahao Li1,3, Anne K. Koehne de González4, Martin R. Prince1, Gary M. Brittenham5, Pascal Spincemaille1, Thanh D. Nguyen1, and Yi Wang1
1Radiology, Weill Cornell Medicine, New York, NY, United States, 2Applied and Engineering Physics, Cornell Univeristy, Ithaca, NY, United States, 3Meinig School of Biomedical Engineering, Cornell Univeristy, Ithaca, NY, United States, 4Department of Pathology, Columbia University Medical Center, New York, NY, United States, 5Department of Pediatrics, Columbia University, New York, NY, United States
Synopsis
Keywords: Liver, Liver
Motivation: Liver biopsy, traditionally regarded as the benchmark for liver fibrosis staging, is an invasive procedure that may cause infection and bleeding.
Goal(s): To develop a non-invasive method to evaluate liver fibrosis using MRI.
Approach: Diamagnetic sources are separated from paramagnetic sources using a biophysical model and multi echo gradient echo data. The value of the diamagnetic sources can be used to quantify the amount of accumulation of collagen due to liver fibrosis.
Results: Significant differences in liver negative susceptibility were observed between lower stage, medium stage and higher stage of fibrosis.
Impact: Multi-echo
gradient echo data may provide a way to non-invasively stage liver fibrosis.
Introduction
Liver fibrosis is a pathological condition characterized by
the excessive accumulation of extracellular matrix proteins, particularly
collagen, as a response to chronic liver injury (1).
The extracellular matrix proteins and collagens are diamagnetic. Therefore, the
amount of diamagnetic susceptibility sources may be used to evaluate the stage
of liver fibrosis. However, the coexistence of paramagnetic contents such as iron
in some patients with liver fibrosis makes measuring the diamagnetic content
difficult. Recently, a biophysical model was proposed that separates the paramagnetic
and diamagnetic sources in MRI by utilizing QSM and additional ’ information (2-3). In
this work, we demonstrate that the diamagnetic susceptibility can be useful to
quantify the fibrotic tissues in the liver. In this work, we compare different MRI
parameters including R2*, R2, R2’, QSM, PDFF and (negative susceptibility sources) in their
ability to differentiate non-fibrotic/mild-stage fibrosis (F0, F1), medium
stage fibrosis (F2, F3), and cirrhosis (F4).
Theory
The relaxation of the collage fibers and iron granules,
which manifest as micro-cylinders and micro-spheres respectively, can be
modeled with the static dephasing model (3). R2’(r) is given by:$$R_2'(r)=R_2^*(r)-R_2(r)=D_r^+|\chi^+(r)|+D_r^-|\chi^-(r)|,$$ where $$$\chi^+(r)$$$ and $$$\chi^-(r)$$$ are the positive and negative susceptibility
sources respectively, ,and $$$D_r^+$$$ and $$$D_r^-$$$ are the relaxometric constants of the positive
and negative susceptibility sources respectively.
The QSM, $$$\chi(r)$$$ can be written as
$$\chi(r)=|\chi^+(r)|-|\chi^-(r)|.$$
The
reconstruction of $$$\chi^+(r)$$$ and $$$\chi^-(r)$$$ are detailed in (2).Method
Liver explant samples from 18 patients were collected, scanned,
and analyzed (Figure 1). The liver samples also underwent histopathological
analysis using hematoxylin and eosin (H&E), Masson's trichrome and Prussian
Blue stains for histology, fibrosis, and iron evaluation, respectively.
MRI imaging parameters were (1) 3D mGRE at 3T (GE
Healthcare, Waukesha, WI, USA), 8 echoes, flip angle = 15, TE1 = 2.6 ms, ΔTE = 2.7
ms, TR = 24.43 ms, reconstructed voxel size = 0.88 × 0.88 × 1 mm3, bandwidth =
390 Hz/pixel, reconstructed matrix = 256 × 256 x 74-128. (2) 2D multi-echo spin-echo data (for R2), FOV
= 240 ×240 mm2 , voxel size = 0.9375 ×0.9375 mm2 , slice thickness = 1 mm,
number of slices = 18-22, TR = 1500 ms, TE = 6.6, 13.2, 19.8 26.4, 33.1, 39.7, 46.3,
and 52.9 ms, band-width = 244 Hz/pixel.
From mGRE, water-fat separation (4-5) was performed, and QSM
(6-9) and R2* (10) were calculated. Masks
are drawn on the scanned liver samples, and average R2*, R2, R2’, $$$\chi$$$, PDFF and | were calculated within the masks.Results
Figure 2 shows a representative example of QSM, $$$|\chi^+(r)|$$$ and $$$|\chi^-(r)|$$$ as well as hematoxylin and eosin (H&E),
Prussian Blue and Masson's trichrome stains in the same liver sample.
Figure 3 compares R2*, R2, R2’, $$$\chi$$$, PDFF and $$$|\chi^-(r)|$$$ for the samples without fibrosis or with mild
fibrosis (F0-1), samples with medium stage fibrosis (F2-3) and samples with
cirrhosis (F4). R2* and R2’ showed a significant difference between F2-3 and
F4 samples (P = 0.0426 and 0.0293 respectively). R2 showed a significant
difference between non-fibrotic/mild-fibrotic samples F0-1 and mediated stage fibrotic
(F2-3) samples (P = 0.0381). There is
also a significant difference between the PDFF of the F2-3 and F4 samples, since
7 out of the 8 samples in the F4 group have steatosis, but 5 out of 6 of F2-3
do not exhibit steatosis. The average absolute negative susceptibility is
significantly different between F0-1 and F2-3 (P = 0.019) and between F2-3 and
F4 (P=0.0027). The higher stage corresponds to higher absolute diamagnetic susceptibility values,
which is consistent with the assumption. This trend can also be shown in the
finer fibrosis groups, as in Figure 4 (right). The mean negative susceptibility values of F0, F2, F2 and F3 are 0.03, 0.04,
0.07 and 0.08 ppm respectively. However, R2*does not exhibit this trend, likely
due to the coexistence of iron, as shown in Figure 4 (left).
ROC curves for distinguishing between fibrosis stages F0-2
and fibrosis stages F3-4 are shown in Figure 5. The negative susceptibility
source yields the best AUC= 0.95.Discussion
This study shows that the susceptibility values of
diamagnetic can be used to quantify the fibrotic tissues in liver, which may allow
a non-invasive evaluation of fibrosis stage in patients. Acknowledgements
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