4D flow MRI enables comprehensive abdominal evaluation, but long acquisition times and motion corruption limit its clinical applicability. To address these limitations, we present a 4D flow sequence with a 3D golden-angle reordered cones sampling trajectory. Cones has high sampling efficiency to allow for vastly accelerated scan times, and excellent aliasing properties that diffuse respiratory and bowel motion artifacts. To further improve motion-robustness, respiratory signals are estimated from each cone readout, and then used to suppress motion during reconstruction. We show that these techniques can be combined to achieve high quality abdominal 4D flow renderings in under 5 minutes.
Trajectory design and pulse sequence: Gradient waveforms are iteratively designed on-the-fly as described by Gurney et al5. Cone interleaves are permuted by the 2D golden-means algorithm7 to enable arbitrary temporal resolution, and enhance motion-robustness (Figure 1a). The pulse sequence is based on RF-spoiled gradient recalled echo (SPGR) with a simple 4-point interleaved velocity encoding scheme (Figure 2).
Image reconstruction: All datasets are reconstructed in BART8 using l1-ESPIRiT9 with spatial wavelet and temporal total variation regularization. Due to memory limitations, data required coil compression from 32 to 16 channels using the singular value decomposition. A low pass filter (cutoff at 0.67 Hz) is applied to a DC navigator10 to estimate respiratory motion signals from each coil element (Figure 1b). The dominant signal is chosen by a coil clustering algorithm11. Motion estimates are used during reconstruction to suppress respiratory motion artifacts by assigning lower weights to motion-corrupted readouts in the data consistency term (soft-gating)12.
Experiments: With informed consent and IRB approval, subjects referred for contrast-enhanced abdominal MRI were scanned using the cones 4D flow sequences on a 3T scanner (GE MR750, Waukesha, WI) with a 32-channel cardiac coil. All data was acquired with subjects freely breathing. Cones 4D flow scan parameters include flip angle: 15o, readout bandwidth: +/- 250 kHz, readout duration: 0.9 ms, TE: 0.9-1.1 ms, TR: 3.9-4.1 ms, spatial resolution: 1.0x1.0x1.5 mm3, matrix size: 256x256x120, 8 cardiac phases, venc: 100-150 cm/s, and scan durations: 4-7 minutes. One subject was also scanned with radially view-ordered Cartesian 4D flow13 for comparison. Cartesian acquisition and reconstruction parameters were kept the same as cones except for readout bandwidth: +/- 125 kHz, TE: 2.2 ms, and TR: 6.3 ms.
We introduce the first 4D flow sequence with a cones sampling trajectory. Higher k-space sampling efficiency allows scan time acceleration rates of up to R=30 without significant loss of image quality or change in velocity quantification. Due to desirable aliasing properties and soft-gating, motion artifacts are reduced in the cones reconstructions when compared against Cartesian.
Similar to findings with PC-VIPR1, cones 4D flow underestimates peak flows relative to those estimated by Cartesian (Figure 5), although a more rigorous evaluation is necessary. Since readout begins shortly after flow encoding, short-term eddy current effects during DC acquisition induce larger phase errors in velocity maps than in Cartesian 4D flow. These effects were corrected after careful tuning of the phase correction. As with any non-Cartesian trajectory, cones is also sensitive to off-resonance artifacts, particularly from fat, and may require fat saturation in certain patients.
This initial implementation yielded a reasonable scan time and spatiotemporal resolution for venous imaging. For arterial applications, cones 4D flow acquisitions may require further acceleration by increasing the sampling efficiency via extended readouts with more twisting. However, further study is required to determine the resulting impact on both flow quantification and off-resonance blurring.
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