Respiratory motion is a major limiting factor for the application of cardiac proton MR spectroscopy (MRS) in clinical settings. Prospective navigator gating is frequently applied to minimize respiratory motion effects. However, scan durations are subject-dependent and hence difficult to predict. The present work describes cardiac proton MRS with fixed scan time employing retrospective phase-based gating. It is demonstrated that, relative to prospective navigator gating, the phase-based gating approach provides comparable triglyceride-to-water ratios with predictable scan time.
Cardiac proton MRS was performed on a 1.5T system (Achieva, Philips, Best, the Netherlands) using a 5-channel coil in 13 healthy subjects (6 male, mean age: 28.9±6.2 years). Cine steady-state free precession images in short-axis and 4-chamber view were obtained for planning purposes. After iterative volume shimming, voxels of 8 mL (4x2x1cm3) were placed in the interventricular septum. A PRESS (point-resolved spectroscopy) sequence (TE: 21 ms, TR: 2000 ms) was applied to acquire spectra in systole using (a) prospective navigator gating on the diaphragm (navigator window 4 mm) and (b) using free-breathing data collection without navigator gating and accepting all averages. In 5 subjects, the free-breathing scan was repeated to assess reproducibility. Data acquisitionwas ECG-triggered for all scans. A total of 96 averages with CHESS-based water suppression (WS) and 16 averages without WS were acquired for prospective gating whereas 304 averages with and 48 without WS were acquired for the phase-based gating approach. Data was post-processed in MATLAB using a customized reconstruction pipeline implemented in ReconFrame (GyroTools LLC, Zurich, Switzerland) (Fig.1). For phase-based gating, signal phases of the water and the main TG peak at 1.3ppm were extracted. These phases were preprocessed and normalized according to$$\phi^{*}_{i} = \frac{1}{N}\sum_{j=1}^{N}{\left\lvert\phi_{i}-\phi_{j}\right\rvert},\;\phi^{'}_{i}=\frac{\phi^{*}_{i}-min\left(\phi^{*}\right)}{max\left(\phi^{*}\right)}\;(1)$$with φi being the phase of a single water or TG average, i being a single average and N being the number of all averages. Afterwards, signals with normalized phases φ'i were selected according to different thresholds (phase thresholding, thresholds between 0.4-0.1) with higher thresholds indicating higher residual phase fluctuations. Subsets of averages for different thresholds as well as the best 16 averages without WS and 96 averages with WS were considered as separate data sets and entered into the post-processing pipeline (Fig.1).Signal intensities of all scans were obtained by fitting the spectra in the time-domain in jMRUI/AMARES3. TG resonances were fitted at 0.9 and 1.3 ppm, the unsuppressed water at 4.7 ppm (Fig.1). Data were corrected for T1- and T2-relaxation effects and the triglyceride-to-water ratio (TG/W) was calculated.
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Figure 3: Standard deviation (SD) of water amplitude fluctuations for prospective navigator gating and retrospective phase-based gating accepting all averages, the best 16/96 averages or using the lowest threshold for each subject.