Magnetic resonance fingerprinting (MRF) is a novel technique which provides rapid proton density, T1 and T2 mapping. However, susceptibility related parameters such as T2* were not acquired simultaneously. In this study, FISP and multi-echo SPGR acquisition were combined within MRF scheme to allow proton density, T1, T2, T2* and field mapping.
Figure 1 shows the proposed pulse sequence diagram. FISP and multi-echo SPGR acquisitions were applied alternatively for each 200 measurements. For the FISP acquisitions, only one FISP echo was acquired for each RF excitation. However, for the multi-echo SPGR acquisitions, 30 gradient echoes were collected for each RF excitation with 50 degree of RF spoiler. For both FISP and multi-echo SPGR acquisitions, spoiler gradients (8π along the slice direction) were applied at the end of echoes. Random rotating golden angle radial acquisition5 were also applied to grant incoherency of under sampling artifacts for each measurements. A total 1000 highly under sampled (8 spokes for each images, reduction factor 32) 2D images with 3 slices were acquired in 3T Siemens scanner (Tim Trio) with 1x1mm2 resolution 256x256 mm2 FOV, 5 mm slice thickness and 391 Hz/Px bandwidth. In the FISP acquisition, echo time was set to be the half of each TR. For the multi-echo SPGR acquisitions, 1st echo time was 4.6 ms and echo spacing was 2.84 ms with collecting 30 echoes for each RF excitation. Scan time was 1 min 24 sec/slice. Each under sampled images were reconstructed using NUFFT6 with gradient delay compensation7. All experiments were performed with a healthy volunteer (IRB-approved).
Bloch simulation was used to generate dictionary. Total 501 isochromats were calculated with different spoiling gradient along the slice direction to generate FISP signal evolution. To generate multi-echo SPGR signal evolution, T2* decay was applied during multi-echo scheme and perfect transverse magnetization spoiling was assumed after the last SPGR echo. Figure 2 shows an example of signal evolutions simulated using the proposed pulse sequence. T2* decay effect and phase variation due to the field inhomogeneity were clearly shown in Figure 2. The dictionary has T1 : [300:30:1500] ms, T2 : [21:3:150] ms, T2* : [10:2:120] ms, off resonance : [-30:5:30] Hz.
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Pulse sequence diagram of the proposed method.