Brian Bozymski1, Xin Shen2, Ali Caglar Ozen3, Serhat Ilbey3, Albert Thomas4, Mark Chiew5, William Clarke5, Ulrike Dydak1,6, and Uzay Emir1,7
1School of Health Sciences, Purdue University, West Lafayette, IN, United States, 2Department of Radiology and Biomedical Imaging, University of California San Francisco, San Francisco, CA, United States, 3Department of Radiology and Radiotherapy, Medical Center - University of Freiburg, Freiburg, Germany, 4Department of Radiology, University of California, Los Angeles, CA, United States, 5Wellcome Centre for Integrative Neuroimaging, University of Oxford, Oxford, United Kingdom, 6Department of Radiology and Imaging Sciences, Indiana University School of Medicine, Indianapolis, IN, United States, 7Weldon School of Biomedical Engineering, Purdue University, West Lafayette, IN, United States
Synopsis
Keywords: Data Acquisition, Muscle
Quantitative
comparison of novel, rosette trajectory UTE (70 μs) and conventional weighted
Cartesian 3D 31P MRSI sequences is performed at 3T in quadriceps
muscle. After previous validation, five
healthy volunteers were scanned by both sequences without interruption. Fitted metabolite maps and SNR calculations of
PCr and ATP signals across selected slices and voxels displayed competitive performance
between each acquisition.
Retrospective
compressed sensing (CS) acceleration results suggest this UTE MRSI may enable faster,
higher resolution 31P metabolite mapping in leg muscle and other
organs of interest.
Introduction
Plentiful literature has highlighted the value of phosphorus-31 (31P) MRS metabolites in providing non-invasive measurements of tissue pH, muscular energy metabolism, and disease prognosis1. Unfortunately, relatively short T2 relaxation times and low in vivo abundance introduce significant restrictions on SNR and resolution within a “clinically feasible” length scan, especially when working below 7T2. Following previous validation3, a rosette UTE 3D sequence was adapted to 31P MRSI and observed to produce comparable results to gold-standard conventional 3D CSI given the same amount of scanning time. Due to the rosette k-space trajectory’s relatively incoherent sampling pattern, it is possible that high under-sampling and compressed sensing (CS) reconstruction techniques could greatly accelerate this acquisition4. A comparative analysis was performed in five healthy volunteers to assess relative performance between the full conventional scan, full UTE scan, and CS accelerated UTE reconstruction.Methods
All data acquisition occurred on a 3T Siemens Prisma scanner at the Purdue MRI facility. The same 8-channel, dual-tuned 1H/31P phased array coil (2 parallel plates with 4 31P channels each)5 was used in all sessions. Five healthy volunteer subjects (BMI = 26 ± 2 kg/m2; age = 29 ± 5 years; 2 f / 3 m) were positioned feet-first and supine, with the upper thighs tightly surrounded by the coil plates. Figure 1 summarizes the two sets of sequence parameters while Figure 2 illustrates coil setup. The adjustment volume was manually positioned (covering both upper legs) and linewidth manually minimized using a 3D GRE abdomen field map and interactive SIEMENS shimming (VE11c). The total scanning process required approximately 90 minutes for each subject
Raw (TWIX) data files were exported for reconstruction and pre-processing in MATLAB (Mathworks, Natick, USA). Gridding and FFT were completed using the nonuniform FFT (NUFFT) method. Data were Hanning filtered and coil-combined using singular value decomposition. Spectra from both acquisitions were zero-order phased by maximizing the real integral of the PCr peak (~0 ppm), and first-order phased by adding 2.3 ms and 70 μs delays respectively. Spectra were fitted within OXSA using AMARES methods6,7. SNR was calculated by dividing PCr peak amplitude by the standard deviation of a noisy spectral region (+10 to +14 ppm, left of the PCr peak). Metabolite maps were generated using ratios of fit amplitudes, with voxels disqualified whenever CRLB estimates were exceedingly high.Results
Figure 3 lists SNR calculations from the full acquisitions for each subject, along with point-spread-function (PSF) simulations. Acquired SNR appears extremely comparable between the methods across all five subjects.
Figure 4 contains example PCr SNR maps calculated from a single slice in one individual. Reported ratio values in healthy quadriceps/hamstrings range from 3.81-5.802, reasonably close to the OXSA AMARES fitting results across all subjects. Although the full metabolite map is closest to the full conventional CSI, the original structure remains clearly visible in the accelerated map. A greater degrees of CS acceleration under-sampling slightly changes the image scaling, however this can be corrected retrospectively. CS acceleration reconstruction also alters the original UTE rosette’s PSF, requiring accurate simulations to calculate the new effective voxel size and compensate SNR calculations.Discussion and Conclusion
These initial results demonstrated the
potential of our novel rosette UTE 31P 3D MRSI sequence for CS
acceleration. Although the version shown
here had a relatively large FOV with a coarse resolution, acquisition is
possible with much smaller FOVs and finer resolution. This acceleration also does not impede the
UTE sequence’s intrinsic avoidance of first-order phasing issues nor
measurement of extremely fast T2 metabolites.
Future work is focused on application to non-alcoholic fatty liver
disease (NAFLD) and high resolution 31P brain metabolite mapping. In hepatology clinics, accelerated 3D MRSI
with a large FOV might aid in quickly assessing NAFLD prognosis in
overweight-to-obese patients. Similarly,
a 2x acceleration factor could generate whole-brain, high-resolution metabolite
maps in under 15 minutes of scan time.Acknowledgements
Data
acquisition was supported in part by the Indiana CTSI. The authors would also like to thank Dr.
Anshuman Panda for his initial work with the 8-channel phased array coil.References
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