Error Bound Analysis of Physics-Informed Neural Networks-Driven T2 Quantification in Cardiac Magnetic Resonance Imaging
Mengxue Zhang, Qingrui Cai, Yinyin Chen, Hang Jin, Jianjun Zhou, Qiu Guo, Peijun Zhao, Zhiping Mao, Xingxing Zhang, Yuyu Xia, Xianwang Jiang, Qin Xu, Chunyan Xiong, Yirong Zhou, Chengyan Wang, Xiaobo Qu

TL;DR
This paper introduces a physics-informed neural network approach for T2 mapping in cardiac MRI, embedding the Bloch equation to improve accuracy without extensive training data, supported by theoretical error bounds validated on models, phantoms, and clinical data.
Contribution
The study develops a PINN-based T2 estimation method incorporating MRI physics and derives error bounds, providing a theoretical foundation absent in prior deep learning approaches.
Findings
Accurate T2 estimation demonstrated on numerical models and phantoms.
Low-error T2 mapping achieved in clinical myocardial infarction patients.
Theoretical error bounds effectively predict estimation accuracy.
Abstract
Physics-Informed Neural Networks (PINN) are emerging as a promising approach for quantitative parameter estimation of Magnetic Resonance Imaging (MRI). While existing deep learning methods can provide an accurate quantitative estimation of the T2 parameter, they still require large amounts of training data and lack theoretical support and a recognized gold standard. Thus, given the absence of PINN-based approaches for T2 estimation, we propose embedding the fundamental physics of MRI, the Bloch equation, in the loss of PINN, which is solely based on target scan data and does not require a pre-defined training database. Furthermore, by deriving rigorous upper bounds for both the T2 estimation error and the generalization error of the Bloch equation solution, we establish a theoretical foundation for evaluating the PINN's quantitative accuracy. Even without access to the ground truth or a…
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Taxonomy
TopicsCardiac Imaging and Diagnostics · Advanced MRI Techniques and Applications · Functional Brain Connectivity Studies
