Magnetic resonance fingerprinting (MRF) provides fast and simultaneous mapping of parameters including T1 and T2. However, T2 mapping in MRF has been less robust and accurate than T1 in its current form. In this work, we propose a new sequence with spiral-out and -in double echoes (SOIDE) for MRF in each TR block which provide double echo signal with better T2 contrast. The proposed SOIDE-MRF shows improved performance over FISP-MRF, as demonstrated in Monte Carlo simulation on a numerical brain phantom (at Tacq=6s/slice, NRMSE of T2 reduced to 9.41% in SOIDE-MRF, and FISP-MRF ~11% at Tacq=12s/slice) and in vivo brain (less biased and more stable T2).
As shown in Fig1, adding upon the conventional FISP-based MRF, which has a single echo (spiral-out, short TE), the proposed SOIDE-MRF introduces a second echo (spiral-in, long TE). As such, it can generate an FID-like signal and also an echo-like signal in each TR, and provide better T2 information. In implementation, the second spiral trajectory in each TR is set to be the same as the first one with reversed order thus no dummy time is needed for the rewinder. Between the two spiral readouts, a Gz spoiler gradient is inserted as the unbalanced gradient. In the same manner as in FISP-MRF, the blocks vary in FAs and TRs to create temporal incoherence. The two echo signals from each block are reconstructed separately with a sliding window scheme3 and NUFFT reconstruction4 and then matched to the dictionary which is accurately modeled with extended phase graph (EPG) theory5. We used the same FA and TR time series for both SOIDE-MRF and FISP-MRF, and the same 36x undersampled spiral trajectory with a FOV of 22cm and 1.22mm voxel size. For SOIDE-MRF, 750 TRs were acquired with total acquisition time of 15s per slice. For comparison, 1500 TRs for FISP-MRF were acquired with the same 15s acquisition time.
To investigate the feasibility of the SOIDE-MRF, Monte Carlo simulation was conducted on a numerical brain phantom which includes the acquisition, sampling and reconstruction processes. Gaussian noise was added such that SNR=20 (for white matter). Simulations were repeated 50 times for statistical analysis which include pixel-wise and overall mean error and standard deviation calculation and also NRMSE. Experiments were also conducted on in vivo human brain with the same parameters at 3T(Siemens Prisma) using 20 channel receive coil.
Fig 2 shows simulation results for both SOIDE-MRF and conventional FISP-MRF. For each case, the mean maps, mean error maps and normalized RMSE maps are shown for both T1 and T2 at different acquisition time, and the overall NRMSE of T2 is labeled in each panel. Fig.3. shows the overall relative error and normalized RMSE result versus acquisition time for different simulation cases.
In vivo results are shown in Fig.4, which includes T1 and T2 maps for different acquisition durations, with conventional T1w and T2w images for comparison.
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