Tianyu Han1, Teresa Nolte1,2, Nicolas Gross-Weege1, and Volkmar Schulz1
1Physics of Molecular Imaging Systems, RWTH Aachen University, Aachen, Germany, 2Multiphysics and Optics, Philips Research Europe, Eindhoven, Netherlands
Synopsis
To make the MRF technique most suitable for clinical needs, efforts are still to be made to accelerate MRF acquisitions while maintaining the accuracy in parameter determination. However, the dictionary calculation is a heavy computational burden for each trial MRF measurement within the optimization process. In this work, we present a numerical study on the optimization of MRF-FISP sequences by using a parallel tempering algorithm. Specifically, an optimization framework tailored for MRF with severe k-space undersampling was developed based on the previously proposed dictionary-free reconstruction (DFR). In vivo measurements were carried out to evaluate the performance of the optimized sequence.
Introduction
MR fingerprinting (MRF) offers a rapid way to simultaneously quantify multiple tissue parameters. By varying acquisition parameters over a time-series of images, e.g., flip angles (FA) and repetition times (TR), tissue-specific signals, i.e., fingerprints, are obtained 1. To make the MRF technique most suitable for clinical needs, efforts are still to be made to accelerate MRF acquisitions while maintaining the accuracy in parameter determination.Methods
In our optimization framework, FA patterns were generated by the trigonometric interpolation method 3. TRs were kept in a constant fashion throughout each of simulated MRF acquisitions. As can be seen in Figure 1, the tissue which modeled by Tj1 and Tj2 was inserted together with a candidate MRF pattern into the EPG simulator 5. Gaussian noise, i.e., SNR = 4.0, was added to both the real and the imaginary part of the signal to mimic the signal gathered from an undersampling acquisition 8. The amplitude of Gaussian noise was modulated by the signal magnitude throughout the fingerprinting train 8. A DFR was performed on the noisy fingerprint to retrieve the best matching Tj1,es and Tj2,es. The corresponding estimation biases δTj1/2 was computed according to |Tj1/2−Tj1/2,es|Tj1/2. In addition, the similarity of the best matching fingerprint (DPjmax) to its adjacent T1 and T2 entires (DPji) was minimized in order to alleviate the matching ambiguity. We quantified the similarity by a calculating gradients kj in the T1−T2 space 2 (Figure 1): kj=4∑i=1ΔDPjiΔTj1,i+w4∑i=1ΔDPjiΔTj2,i,ΔDPji=DPjmax−DPji,ΔTj1/2,i=Tj1/2,es−Tj1/2,i. We set the weighting factor w=103 for increasing the T2 accuracy in our optimization. In Figure 1, eight entries (Tstep1=5ms, Tstep2=2.5ms) around the best matching entry, e.g. DPjmax, were involved in the gradient calculation. We defined the total objective function p as: p=∑jδTj1+δTj2kj. It sums over contributions from all tissue components in the anatomical region of interest. The parallel tempering algorithm 6 was used to minimize the proposed objective function p. In-vivo data was acquired on a 3T MRI scanner (Achieva3T, Philips, The Netherlands). 36 constant density spiral interleaves were combined to fully sample the k-space. A non-uniform dictionary with T1 resolutions of 40ms (T1∈[100ms,2000ms]), 200ms (T1∈[2010ms,6000ms]) and T2 resolutions of 20ms (T2∈[10ms,500ms]), 200ms (T2∈[510ms,2500ms]) were used for reconstruction.Results and discussion
We compare the encoding performance of Jiang's pattern PJiang 7, our algorithm pattern PFully (Fully: fully converged), and an algorithm pattern PEarly (Early: early stopping). The proposed algorithm is able to generate MRF patterns such as (A) in Figure 2, by including a priori knowledge, i.e., the relaxation times of tissues found in the brain (Figure 2 (B)). By comparing T1/2 maps under fully sampled (R=1) and undersampled (R=36) measurements (Figure 3), PFully shows an equivalent undersampling tolerance to PJiang 7. Previous MRF measurements 1,7 showed large inaccuracies in the CSF T2 prediction. We visualize inconsistencies in CSF estimation in Figure 4 by thresholding the quantitative maps. The distribution of CSF can be retrieved from the T1 maps due to the higher precision in CSF T1 estimations 1. Notably, in the measurement obtained with PJiang, the common circulation area of CSF such as lateral ventricles and brain sinuses are invisible due to their low reconstructed T2 values (marked by white arrows in Figure 4). However, CSF T2 maps from the PFully acquisition (second row in Figure 4) better represent the CSF distribution. As predicted by the optimization cost function, the corresponding quantitative maps reconstructed from the PFully measurements show consistent CSF distribution between T1, T2 maps, even for high undersampling of R=36. On the other hand, weaker robustness to undersampling, i.e., inconsistencies in T1 and T2 maps (last row in Figure 4), are observed in the measurements with PEarly. When thresholding for GM and WM, PJiang and PFully measurements show similar results. However, reconstructed maps from PEarly measurements (last row of Figure 5) show T1 overestimation (underestimation) in the left (right) part of the WM region (indicated by arrows in Figure 5). In addition, a more noisy T2 map is observed in the PEarly reconstructed T2 maps. Conclusion
The proposed optimization framework enables optimized MRF pattern generation based on tissues of interest for accurate quantitative MR mappings.Acknowledgements
This project has received funding from the European Union’s Horizon 2020 research and innovation program under grant agreement No. 667211.
References
1. Dan. M, et al. Magnetic Resonance Fingerprinting. Nature. 2013; 495: 187-193.
2. Tianyu. H, et al. Fast Dictionary-free Reconstruction in MR Fingerprinting. Proc. Intl. Soc. Mag. Reson. Med. 2018; 26: 2893.
3. Kendall A, An Introduction to Numerical Analysis (2nd edition), Section 3.8. John Wiley & Sons. New York,1988.
4. Ouri. C, et al. Algorithm comparison for schedule optimization in MR fingerprinting Magnetic Resonance Imaging. 2017; 41:15-21.
5. Matthias W, Extended phase graphs: Dephasing, RF pulses, and echoes ‐ pure and simple. Journal of Magnetic Resonance Imaging. 2015; 41: 266-295.
6. David. J. E, et al. Parallel tempering: Theory, applications, and new perspectives. Phys . Chem. Chem. Phys. 2005; 7: 3910-3916.
7. Yun. J, et al. MR fingerprinting using fast imaging with steady state precession (FISP) with spiral readout. Magn Reson Med. 2015; 74:1621-1631.
8. Karsten S, et al. Towards predicting the encoding capability of MR fingerprinting sequences. Magnetic Resonance Imaging. 2017; 41: 7-14.