A spiral projection acquisition scheme was implemented for 3D MR fingerprinting to achieve isotropic resolution of 1x1x1 mm3 in whole brain T1 and T2 mapping within 2.5 minutes by using efficient L1SPIRiT reconstruction (ESPIRiT) and back-projection reconstruction.
Methods
The acquisition and reconstruction process were shown in Figure 1.
a. A spiral trajectory was rotated about x-axis along time points (TP) dimension and simultaneously about z-axis along acquisition group (AG) dimension.
b. By combining the spiral interleaves acquired from the same time point but different acquisition groups, spiral interleaves formed an undersampled disk-like k-space coverage in a same plane.
c. Undersample the “disk” with acceleration factor R=2, which means it could reduce the number of acquisition groups by half, resulting in a two-fold reduction of acquisition time.
d. ESPIRit 5 reconstruction method was applied on the undersampled disk-like k-space data. Since the “disk” was rotated along time points dimension, the reconstructed image of each time point was actually a parallel-beam projected image from a specific angle.
e. By using a sliding-window method 6 to select adjacent projected images and applying a back-projection reconstruction method 7 on these images, a series of 3D images with varying mixed contrast were obtained along the time point dimension.
f. Reconstructed images were template matched with a pre-calculated dictionary voxel-by-voxel to generate T1 and T2 maps by using the extended phase graph (EPG) 8 method. The dictionary entries were also implemented with sliding-window method in the same way as we did it in step e.
Figure 2 shows a typical pulse sequence design of a 3D MRF fingerprinting with fast imaging with steady state precession (FISP) readout 9 and SPI trajectory. A slab-selective gradient was used to achieve a 240-mm slab thickness and a dephase gradient was used to achieve a 4- dephase. Each acquisition group includes 500 time points in which the flip angles vary in a preset way as Figure 2b shows and the TRs were set at 16 msec constantly. Between two adjacent acquisition groups, a waiting time of 2sec was inserted for the recovery of longitudinal magnetization. A total of 30 acquisition groups were acquired for fully-sampled data as reference and 15 of them were used for the validation of the proposed method. The spiral rotates about x-axis at tiny golden angle (23.63°) along time points dimension. The isotropic spatial resolution of 1x1x1 mm3 was achieved for the identified parametric maps in a field of view (FOV) of 240x240x240 mm3. The measurements of a phantom and in vivo brains were performed on a Siemens 3T Prisma scanner with a 64-channel head coil.
Discussion and Conclusion
We proposed a reconstruction scheme by combining the ESPIRiT and back-projection reconstruction on 3D MRF with SPI trajectory. Compared to original 3D SPI MRF using 3D INUFFT method [4], the reconstruction was split into two part, 2D INUFFT which transforms k-space data to projected images and back-projection which transforms projected images to 3D images. With a simple 2D INUFFT replaced by ESPIRiT, acquisition acceleration could be achieved by undersampling the “disk” data with less spiral interleaves. Therefore, the T1 and T2 maps of 1-mm isotropic resolution and FOV = 240x240x240mm3 could be obtained within half the acquisition time of original 3D SPI MRF, namely 2.5 minutes. A drawback of the proposed method is that the images seem to be smoothed which may be caused by the rudimental algorithm of back-projection method we are using currently. In the future work, we will utilize a better back-projection reconstruction scheme to fix this problem.1. Ma D, Gulani V, Seiberlich N, Liu K, Sunshine JL, Duerk JL, Griswold MA. Magnetic resonance fingerprinting. Nature 2013;495(7440):187-192.
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Figure.1
Process of acquisition and reconstruction for the proposed method.
Figure.2
(a) Pulse sequence of 3D MRF with spiral projection acquisition.
(b) Flip angles pattern. TR was kept at 16 ms constantly for whole scan.
(c) Acquisition groups distribution.
Figure.3
The projected images reconstructed from full-sampled (a) and under-sampled using a simple 2D INUFFT (b) and ESPIRiT algorithm (d) as well as corresponding difference map compared with the full-sampled data (c,e).
Figure.4
T1 (a) and T2 (b) maps using different reconstruction schemes with full-sampled and under-sampled (acceleration factor R=2) data.