Qi Liu1, Hoang (Mark) Nguyen1,2, Xucheng Zhu3, Xiaohui Zhai3, Bo Li3, Jian Xu1, and Weiguo Zhang1
1UIH America, Inc., Houston, TX, United States, 2Department of Computer Science and Electrical Engineering, University of Missouri at Kansas City, Kansas City, MO, United States, 3United Imaging Healthcare, Shanghai, China
Synopsis
A versatile, practical, and effective gradient trajectory
correction technique that considers gradient system nonlinearity is proposed using
deep learning. Its performance was validated on phantoms and human subjects and demonstrated superior quality than the conventional techniques.
Introduction
Certain MRI applications, including spiral and ultrashort
echo-time (UTE) imaging, require obtaining an accurate gradient trajectory that
often deviates from the prescribed waveform. The deviation can be attributed to
factors such as gradient delay, eddy currents, and gradient amplifier imperfection
encompassing nonlinear components coming mainly from PID (proportional–integral–derivative)
feedback. Existing trajectory correction techniques include gradient field
measurement, gradient system response (GSR) calibration, and delay correction,
among others [1-5]. Gradient field measurement can obtain accurate trajectory but
is impractical in the clinical scan where gradient waveform changes with user-specified
parameters thus would require re-measurement. Other correction techniques
mostly rely on the assumption of linearity, assuming the MRI gradient system
can be modeled by an impulse response function. However, as will be shown, the
above assumption is not valid and will cause artifacts.
In this study, a versatile, practical, and effective
gradient trajectory correction technique that considers gradient system nonlinearity
is proposed and validated on phantoms and human subjects. It incorporates deep neural
network (DNN) to predict actual gradient waveforms from prescribed waveforms as
input. After system setup, additional calibration is not needed during scanning.
To our knowledge, this is the first time DNN has been employed to solve MRI
gradient system problems. Methods
Gradient waveform measurement:
Following exciting a thin slice perpendicular to the gradient
axis, the to-be-measured gradient was played with simultaneous signal
receiving. Four different slice positions were used, and polarities of the
gradients were varied to remove confounding factors, similar to previously
published [6].
GSR calibration:
A series of triangle waveforms with different amplitudes were
prescribed and measured. Sample waveforms (Figure 1) were shown at a similar
scale to emphasize nonlinearity features that are not scalable. GSR was
calculated following the previous approach [5].
DNN architecture and training:
The task could be viewed as a signal reconstruction problem where
the model attempts to a generate measured waveform, with the prescribed waveform
as the input. The most popular deep learning architecture for image or signal
reconstruction is U-Net and its variants which consist of an encoder and a decoder
[7-9]. However, gradient waveforms are predefined functions that contain more
global features (overall shape) than local features (texture), and therefore
using a convolutional operation would not be effective. Instead, a long short-term
memory (LSTM) architecture is proposed (Figure 2). The feedback connection in
LSTM allows the network to remember the entire sequence of the dataset, which
helps the model memorize the waveform shapes as well as their amplitude. After
LSTM, two convolution layers are added to reconstruct waveforms from extracted
features.
The LSTM contained one hidden layer with 100 dimensions, and
the two convolution layers had kernel sizes of 5x1 and 9x1, respectively. Mean
squared error loss function and Adam optimization were used. The initial
learning rate was 0.01 and reduced by half when the validation loss was not
improved after 20 consecutive epochs. The model was trained with 500 epochs,
and the weight that yielded the lowest validation loss was saved. Duration and
amplitude of triangle, spiral and trapezoid gradients, whose shapes are
commonly used in MRI scans, were varied to generate different waveforms. A
total of 1517 waveforms were recruited for training. Data augmentation was employed
by inverting gradient polarity and time-shifting waveforms.
Study experiment: All data were acquired on a clinical 3T
scanner (uMR790, United Imaging Healthcare, Shanghai, China). 2D spiral imaging
and 3D UTE imaging with koosh ball trajectory were performed on phantoms and
human brains (Table 1). For comparison, reconstruction was conducted using the following
waveforms: the measured actual waveforms (as gold standard), waveforms
predicted using GSR, waveforms predicted using the proposed DNN, and the prescribed
waveforms. Care was taken not to use waveforms already in the DNN’s training
dataset for imaging. Reconstruction involved regridding with Kaiser-Bessel
kernel, density compensation, and sum-of-squares coil combination.Results
Typical spiral and UTE gradient waveforms from the various
methods are illustrated in Figure 3. Compared to GSR, DNN waveforms have better
agreement with the gold standard, particularly at low-amplitude which
correspond to the region around k-space center that contributes heavily to
image contrast. Phantom and volunteer images (Figures 4 and 5) reconstructed
with DNN waveforms are free of artifacts present in those with GSR and have
similar image quality to the gold standard.Conclusion and Discussion
The feasibility of using DNN for gradient waveform
prediction was demonstrated and showed superior image quality than the
conventional GSR method by incorporating the nonlinearity response. Despite
that only predicting gradient waveform is demonstrated in this study, applying
the same approach to predicting B0 eddy current should be straightforward. In
response to the large amount of data needed for DNN training, future work will
be directed towards accelerating model training by transfer learning between 1)
scanners of the same model, 2) scanners of different models but same field
strength, and 3) scanners of different field strengths. Acknowledgements
No acknowledgement found.References
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