Jiye Kim1, Dongmyung Shin1, Juhyung Park1, Hwihun Jeong1, and Jongho Lee1
1Department of Electrical and Computer Engineering, Seoul National University, Seoul, Korea, Republic of
Synopsis
A deep reinforcement learning method
referred to as DeepRF-Grad, is newly developed to design an RF pulse and a
slice selective gradient waveform. The method is demonstrated for
slice-selective inversion and compared with SLR and VERSE-designed pulses. The DeepRF-Grad
designed pulse showed lower SAR (SLR: 13.2mG2s, VERSE: 6.37mG2s,
DeepRF-Grad: 5.00mG2s). When designed for off-resonance robustness, the
DeepRF-Grad generated enhanced off-resonance characteristics compared to that
of VERSE-designed pulse, while showing similar SAR.
Introduction
In MR imaging, a high specific
absorption rate (SAR) of a radiofrequency (RF) pulse is a significant problem
in clinical use, particularly for high field systems. To reduce SAR, a variable-rate
selective excitation (VERSE) method, which remaps uniform slice-selective gradient into the time-varying
gradient, was introduced1. As reported, however, VERSE pulses are vulnerable
to off-resonance frequency, limiting the applicability of the method. Recently,
deep reinforcement learning (DRL)-powered RF pulse design has been proposed,
demonstrating improved performance in SAR2,3. In this work, we extended the dimension of the design space in DeepRF3 to include both RF pulse and slice-selective gradient waveform (Gz).
This new method is named DeepRF-Grad
(Fig 1) and is tested to generate i) SAR-reduced design and ii) SAR-reduced
and off-resonance robust design, while satisfying hardware constraints (i.e., gradient
slew rate and max gradient limits).Methods
For a conventional RF pulse, a slice-selective linear-phase
inversion pulse is designed using Shinnar-Le-Roux (SLR)4,5. The parameters are
as follows: pulse duration = 3.873 ms, time-bandwidth product = 2.711, stopband
ripple = 1%, and passband ripple = 1%. This pulse is redesigned using the VERSE
algorithm to reduce SAR6.
In DeepRF-Grad, the pulse duration is the same and the
ripple conditions are designed to match the conventional RF pulse. The design
process of DeepRF-Grad is as follows: first, magnitude and phase parts of the RF
pulse and slice selective gradient waveform (Gz) are simultaneously
designed using DRL (3x256 points). Secondly, these designs are jointly updated
using gradient descent until they converged to an optimal point (Fig 2).
To design a slice-selective
inversion pulse while regularizing SAR, the reward of DRL is devised as follows:
$$reward=-\frac{1}{N}\sum_{z_p\in{Z_{pass}}}M_z(RF,G_z,z_p)+\frac{1}{M}\sum_{z_s\in{Z_{stop}}}M_z(RF,G_z,z_s)-c_{SAR}SAR$$
where N (= 24) is the number of
z-positions in the passband (Zpass), and M (= 86) is the number of
z-positions in the stopband (Zstop), Mz is the longitudinal magnetization, and cSAR
(= 0.3) is a coefficient for the SAR regularizer term. Each training of the DRL
agent consists of 1000 epochs. After training, RF pulses and Gz generated with the
top 1000 highest rewards are selected as seeds for the second part of DeepRF-Grad,
gradient descent.
The objective of the gradient descent step is to match the slice
profile to that of the SLR-designed result while minimizing SAR and keeping the
slew rate under the limit. Two types of designs are developed: i) SAR minimized
design with off-resonance sensitivity comparable to that of VERSE, and ii) off-resonance
robust design with reduced SAR. The loss function, which is minimized via
gradient descent, is designed as follows:
$$loss=\sum_{w_o\in{W}}\parallel{M_z(RF,G)-M_z(SLR)}\parallel+c_1SAR+c_2\sum_{i=1}^{256}u(slew_i-slew_{max})$$
where wo means off-resonance frequencies, c1
and c2 are coefficients, u is a unit step function, slewi
is a gradient slew rate for each time step, slewmax is the slew rate
limit (= 170 mT/(m*ms)). The off-resonance frequencies are included only for the
off-resonance robust design. The derivatives of the loss function with respect
to each of the RF pulse and Gz are computed via automatic
differentiation.
The gradient descent is repeated until the RF pulse and Gz
converge.
The SLR,
VERSE, DeepRF, and DeepRF-Grad designs are evaluated
in terms of their slice profile and SAR. Additionally, the slice profiles of
the VERSE and DeepRF-Grad designs are compared at two additional off-resonance frequencies
(200 Hz, and 400 Hz). For a fair comparison, a VERSE designed pulse that has a similar
SAR to the DeepRF-Grad pulse is produced. Lastly, an additional DeepRF-Grad
design is produced for a low slew rate condition (135 mT/(m*ms); 20% lower slew
rate), comparing for the SAR and slice profile.Results
[SAR minimized design]
The
SARs of the four designs are 13.2mG2s for SLR, 6.37 mG2s
for VERSE, 11.3mG2s for DeepRF, and 5.00 mG2s for DeepRF-Grad,
demonstrating a reduction of 62% in SAR when comparing the DeepRF-Grad result
with that of SLR (Fig. 3). The slice profiles (last column in Fig. 3) reveal
comparable results in all designs. In DeepRF-Grad, the mean Mz in the passband is
-0.97 (SLR: -0.99), and the stopband ripple is 1.19% (SLR: 0.21%). No hardware
constraint is violated. When the off-resonance profiles are compared, both VERSE
and DeepRF-Grad results show similar profiles (Fig. 3e).
[Off-resonance robust design]
The SARs are 8.81mG2s for
DeepRF-Grad, and 8.40 mG2s for VERSE. Figure 4 illustrates the VERSE
and off-resonance robust DeepRF-Grad designs with similar SAR. DeepRF-Grad reveals
an improved off-resonance profile, particularly at a high off-resonance frequency
(400Hz).Conclusion and Discussion
In this study, we propose a deep learning method that
simultaneously designs RF pulse and slice-selective gradient waveform. The
results show that DeepRF-Grad can reduce SAR by 62% when compared to the SLR
pulse. Additionally, DeepRF-Grad can be utilized to design an off-resonance
robust RF/Gz design that has 35% lower SAR than the SLR pulse. Since DeepRF-Grad
designed gradient shows a high slew rate at the edges, an eddy-current-induced
artifact could exist. This may be mitigated by setting a lower limit to the
slew rate, which resulted in a similar pulse while maintaining SAR reduction performance
(60% reduction) (Fig. 5). Acknowledgements
This work was supported by the National Research Foundation of
Korea (NRF) grant funded by the Korea government (MSIT) (NRF- 2018R1A2B3008445), and Brain Research Program through the
National Research Foundation of Korea(NRF) funded by the Ministry of Science,
ICT & Future Planning (NRF-2019M3C7A1031994).References
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