We present a free-breathing multi-contrast 3-D cardiac CINE acquisition and reconstruction technique based on Compressed Sensing. Inversion pulses were repeatedly applied during a continuous acquisition to sample contrast- and cardiac-resolved 3-D data, while a self-navigation method was applied for respiratory gating. Validation was performed in a phantom, showing recovery curves and T1* maps in good correlation to known T1 values for the phantom as well as a MOLLI reference measurement. Feasibility for in-vivo application was demonstrated in a healthy volunteer.
Sequence
We acquired data during free-breathing using a 3-D volume-selective, ECG-gated, prototype balanced Steady-State-Free-Precession (bSSFP) sequence. Adiabatic inversion (IR) pulses were applied every $$$3s$$$ to sample multi-contrast CINE (MC-CINE) data. Waiting periods of variable length $$$x$$$ were placed after each $$$3s$$$ while maintaining the steady state to avoid coherence between the IR pulse and the R wave (Fig.1A). Incoherent subsampling of the Cartesian phase-encoding plane was achieved with a spiral spokes sampling pattern4. The first sample of each spiral arm in the k-space center was utilized to derive the respiration signal for respiratory gating.
Retrospective binning and reconstruction
Acquired readouts were sorted into a multi-dimensional space according to their positions after the R wave and the IR pulse (Fig.1B). Afterwards, data was binned into $$$m$$$ cardiac and $$$n$$$ contrast phases. Prototype image reconstruction was performed separately for every contrast phase, but jointly for all readouts using a previously published Compressed Sensing approach4,5, resulting in one 3-D volume for every cardiac and contrast phase.
Experiments
All experiments were performed on a 1.5T scanner (MAGNETOM Aera, Siemens Healthcare, Erlangen, Germany). For validation of our method, we acquired undersampled MC-CINE data of the $$$T_1$$$ array of the NIST/ISMRM phantom6 with a simulated heart rate of 60 beats per minute. Afterwards, data was binned ($$$m$$$=10 cardiac, $$$n$$$=20 contrast phases) resulting in 200 3-D datasets. To show the resulting range of reconstructed contrasts, we fit apparent $$$T_1^*$$$ values using the three-parameter fit7,8 For comparison, we acquired slices of the phantom from the same position as for the MC-CINE acquisition with a state-of-the-art MOLLI8 protocol provided by the scanner manufacturer. $$$T_1^*$$$ values from our method were obtained from the mean of 5 reconstructed slices, corresponding to one 8 mm thick MOLLI slice at this position. Regions-of-interest (ROIs) within 10 spheres (range: 90 to 2050 ms, representing physically relevant $$$T_1$$$ values within the heart) were segmented manually, and the mean and standard deviations within the ROIs were computed, respectively. Feasibility in a healthy volunteer (m, 20 years) was studied by performing a scan in short-axis (SA) orientation. Data was binned ($$$m$$$=10 cardiac, $$$n$$$=20 contrast phases) and reconstructed. Detailed acquisition and reconstruction parameters are provided in Table 1.
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[3] Ferreira, Vanessa M., et al. "Non-contrast T1-mapping detects acute myocardial edema with high diagnostic accuracy: a comparison to T2-weighted cardiovascular magnetic resonance." Journal of cardiovascular magnetic resonance 14.1 (2012): 42.
[4]Wetzl, Jens, et al. "Free-breathing, self-navigated isotropic 3-D CINE imaging of the whole heart using Cartesian sampling." Proceedings of the 24th Annual Meeting of ISMRM. Vol. 411. 2016.
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[7]Jara, Hernán. Theory of quantitative magnetic resonance imaging. Hackensack, NJ: World Scientific, 2013. ISBN: 978-981-4295-23-9.
[8] Messroghli, Daniel R., et al. "Modified Look‐Locker inversion recovery (MOLLI) for high‐resolution T1 mapping of the heart." Magnetic Resonance in Medicine: An Official Journal of the International Society for Magnetic Resonance in Medicine 52.1 (2004): 141-146.
Figure 1: Acquisition scheme. After one IR pulse, continuous readouts are acquired for 3 s over multiple heartbeats. Afterwards, a waiting period is included to vary the position of the IR pulse within the heart cycle.
A: Sampling scheme. Every spiral spoke arm is identified using its position after one R wave and IR pulse (one example is shown in red color, from 4).
B: Retrospective binning process. One example is shown in purple color: One spiral spokes arm is sorted into the multi-dimensional space according to two dimensions: its position after one R wave (cardiac) and its TI (contrast).
Figure 2: Phantom results.
A: One slice at different TIs (first row) and two recovery curves (each with 10 cardiac phases) of one position within two example spheres (second row) and examples of fitted maps (third row).
B: Comparison of mean values ± standard deviations for ROIs within phantom spheres between MC-CINE (mean values of the 10 cardiac phases for one ROI), MOLLI and ground truth. Note the decreased standard deviations from MC-CINE within the fitted values (table below). From the slight underestimation, the MC-CINE mean error is larger than MOLLI mean error for some cases.
Std.dev.: Standard deviation
Figure 3: Respiration.
A: Excerpt of central k-space readouts of the volunteer (one coil) used to derive his respiration. Left: Raw signal. Signal gaps resulting from the different contrasts after IR pulses hamper the derivation of the respiration curve. Right: Processed and interpolated signal, from which the respiration curve (blue) is fitted based on SVD. The yellow marked positions on the curve belong to the respiration phase selected for the reconstruction of the data.
B: One example slice reconstructed from all acquired data (left) differ from the same slice reconstructed using our respiration gating method and the same parameters (right).