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Accelerated Rosette Spectroscopic Imaging with semi-LASER Localization
Ajin Joy1, Uzay Emir2,3, Paul M. Macey4, and M. Albert Thomas1
1Radiological Sciences, University of California, Los Angeles, Los Angeles, CA, United States, 2School of Health Sciences, Purdue University, West Lafayette, IN, United States, 3Weldon School of Biomedical Engineering, Purdue University, West Lafayette, IN, United States, 4School of Nursing and Brain Research Institute, University of California, Los Angeles, Los Angeles, CA, United States

Synopsis

Keywords: Data Processing, Brain

Limiting the total data acquisition time to a clinically feasible runtime has been a major challenge in MR spectroscopic imaging. Recently rosette based non-cartesian encoding of k-space has been used for spectroscopic imaging due to their fast encoding speed and lower gradient/slew rate requirements. While rosette spectroscopic imaging has been attempted for 2D and 3D spectroscopic imaging, feasibility of undersampling the petals in rosette is not shown. In this study, we implemented a rosette 2D and 3D spectroscopic imaging sequence and shown the feasibility of acceleration factors up to 8x using compressed sensing reconstruction.

Introduction

MR spectroscopy (MRS) is an efficient biochemical tool for non-invasively analyzing metabolite and lipid concentrations in human tissues (1-4). Limiting the total data acquisition time to a clinically feasible runtime has been a major challenge in MRS imaging (MRSI). Even though k-space-weighted and average-weighted schemes have been used to shorten the total duration of MRSI, echo-planar spectroscopic imaging (EPSI) showed further acceleration of the total acquisition duration (5,6). Recently rosette based non-cartesian encoding of k-space has been used for spectroscopic imaging due to their fast encoding speed and lower gradient/slew rate requirements (7-10). It has been further reported in MRI studies that the sampling pattern of the rosette trajectory has higher incoherence than that of the other non-Cartesian trajectories like spiral and radial, and can thus achieve higher compressed sensing (CS) reconstruction performance (11). Compressed sensing (CS) based reconstruction techniques are known to be capable of recovering the signal depending on the signal sparsity and incoherent sampling patterns (12). While rosette spectroscopic imaging has been attempted for two dimensional (2D) (2 spatial+1 spectral) and three dimensional (3D) (3 spatial+1 spectral) spectroscopic imaging (7-9), feasibility of undersampling the petals in rosette is not shown. In this study, we implemented a rosette spectroscopic imaging (ROS-SI) sequence and studied the feasibility of multiple acceleration factors.

Materials and Methods

The 2D- and 3D-ROS-SI sequence was designed based on the rosette trajectory for two spatial dimensions (kx and ky) as described in (13) and was implemented on a Siemens 3T clinical scanner. Third spatial dimension (kz) in 3D-ROS-SI was phase encoded. Data from a brain phantom containing metabolites at physiological concentrations was acquired. A 68-year-old healthy volunteer was recruited with IRB approval for the acquisition of in vivo brain data. 2D-ROS-SI phantom scans were acquired with a 32 × 32 matrix size, a 24 × 24 × 2 cm3 slab using volumetric semi-LASER localization, TE = 28.6 ms, TR = 1.5 s, and a spectral width of 1250 Hz, spatially interleaved 32 petals, with 512 t2 points and 8 averages. 8 phase-encoded kz points were additionally acquired for 3D-ROS-SI. Even though (π*Nx)/2 ≈ 51 number of excitations are reported to be needed for full acquisition in (7) (where Nx is number of pixels in one dimension of reconstructed image), it has also been reported that number of petals = Nx is sufficient for adequate reconstruction in (14). Therefore, 32 petals instead of 51 is considered fully sampled for the purpose of this study. The phantom data were retrospectively undersampled at 2x (16 petals), 4x (8 petals) and 8x (4 petals) to study the effect of high undersampling and CS reconstruction. The 2D-ROS-SI volunteer scan was acquired with 8 petals and 8 averages, for 4x acceleration. All other parameters were kept the same as mentioned earlier. Time for one average was 18 seconds including 4 dummy preparation scans and 1 minutes, 42 seconds for 8 averages. CS reconstruction using Perona-Malik (14-17) and non-uniform FFT (nuFFT) (18) was used to estimate the missing samples of k-space. LCModel based quantitation was used to quantify the resulting spectra (19).

Results

Figure 1 shows the localization images, extracted voxel from reconstructed data at 1x, 2x, 4x and 8x acceleration factors along with a bar chart showing comparison of metabolite ratios with respect to Creatine (Cre) across multiple voxels from different acceleration factors quantified using LCModel. Different sampling patterns used for this study are shown in Fig. 2. Figure 3 shows metabolite maps of Creatine 3.0 (Cre 3.0), myo-Inositol (mI), N-acetylaspartate (NAA) and choline (Cho) at multiple acceleration factors for both gridding and PM based CS reconstruction. In-vivo data was reconstructed using nuFFT based PM. Sagittal and axial localization images, as well as the reconstructed metabolite maps of Cre 3.0, Creatine 3.9 (Cre 3.9), mI, NAA, Cho and Glx (Glutamine + Glutamate) overlaid on the localization image are shown in Figure 4. Multi-voxel spectra covering multiple voxels within the VOI (white box in the localization image) and the LCModel fit of an extracted spectrum is shown in Figure 5.

Discussion

Accelerated rosette based spectroscopic imaging was implemented and tested using phantom and in-vivo datasets. The metabolite maps in Fig 1 shows reconstructed maps devoid without visible undersampling artifacts for CS reconstruction until 4x acceleration (8 petals), while gridding shows visible aliasing artifacts even at 2x acceleration. Increasing acceleration to 8x tend to retain aliasing artifacts in the reconstructed data even with CS reconstruction. However most of the metabolite ratios stayed within relatively same range across different acceleration factors. While mI was marginally overestimated at 8x, Glx ratio was slightly reduced at 4x and slightly increased at 8x compared to ratios from fully sampled. Ratios of alanine (Ala), aspartate (Asp), GABA, lactate (Lac) and total choline (tCho) were stable across all acceleration factors considered in this study.

Conclusion

Due to the higher incoherence level of sampling pattern, rosette trajectory based spectroscopic imaging sequence has the potential for highly accelerated acquisitions (11). A rosette based Spectroscopic Imaging sequence was implemented and the feasibly of acceleration upto Nx/8 petals is demonstrated in this work.

Acknowledgements

Authors acknowledge grants support from National Institute of Health (5R21MH125349-02 and 5R01HL135562-04).

References

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Figures

Fig 1: (a) Axial and sagittal localization images for 2D ROS-SI (b) Axial and sagittal localization image for 3D ROS-SI (c) voxels extracted from accelerated and reconstructed phantom data. (d) bar chart showing comparison of metabolite ratios with respect to creatine across multiple voxels while different acceleration factors were used for the spatial dimensions.

Fig 2: (a) Sampling patterns used for 3D-ROS-SI (b) 2D rosette sampling pattern along Kx and Ky for fully sampled (32 petals), 2x(16 petals), 4x(8 petals) and 8x(4 petals) acceleration factors for a matrix size of 32x32.

Fig 3: Metabolite maps from accelerated and reconstructed phantom data. Panels in first and third rows show the results of CS reconstruction. Panels in second and fourth rows shows the results of gridding. Column-wise panels corresponds to different acceleration factors.

Fig 4: Sagittal and axial localization images from 68-year-old healthy volunteer are shown in first and second panels from left to right in top row. Remaining panels show the reconstructed metabolite maps of Cre 3.0, Cre 3.9, mI, NAA, Cho and Glx overlaid on the localization image.

Fig 5: Multi-voxel spectra covering the voxels within the red box in the axial localization image is shown in the top row. Bottom row shows the LCModel fit of an extracted in-vivo spectrum from an voxel of 1.125ml volume.

Proc. Intl. Soc. Mag. Reson. Med. 31 (2023)
3953
DOI: https://doi.org/10.58530/2023/3953