0759

A Fast T2-weighted Approach for Prostate Imaging using non-Cartesian GRAPPA and Spiral TSE readout
James Ahad1, Yun Jiang2, Vikas Gulani2, and Nicole Seiberlich2
1Biomedical Engineering, Case Western Reserve University, CLEVELAND, OH, United States, 2Radiology, University of Michigan, Ann Arbor, MI, United States

Synopsis

In-gantry prostate biopsy relies on repeated time-consuming T2-weighted TSE imaging for needle guidance. Reducing the acquisition time for this scan has been challenging due to the spatial resolution and field-of-view requirements of these images, in addition to susceptibility and off resonance artifacts sources common to pelvic imaging. This work proposes a non-Cartesian GRAPPA approach with a short spiral in-out TSE readout to reduce acquisition time for needle guidance images. Comparisons of in vivo Cartesian and spiral TSE images with 300mm FOV, 1.17x1.17mm2 resolution, and 3mm slice thickness acquired in 61s and 8s respectively, are shown.

Introduction

MR-guided in-gantry prostate biopsy has been shown to be more sensitive and specific than other biopsy techniques1, but often entails long procedure time2. After initial high resolution planning images, repeated intermediate resolution T2-weighted turbo spin echo (TSE) images are obtained for introducer probe targeting the lesion of interest2. Acceleration of these guidance images would enable faster probe targeting during biopsy and improve clinical workflow. Parallel imaging is used to accelerate guidance images but is limited due to the intrusive appearance of ghost-like aliasing artifacts in Cartesian sampling. Spiral trajectories have been shown to reduce acquisition time3,4 and improve scan efficiency5 of TSE acquisitions due to their greater sampling efficiency within a single readout6, and have undersampling artifacts that manifest as blur rather than ghosts6. This work explores spiral TSE with non-Cartesian GRAPPA as a potential fast substitute for Cartesian TSE in prostate imaging.

Methods

Uniform density spiral in-out trajectories were designed by concatenating a fully sampled spiral-out gradient waveform with its time-reversed spiral-in waveform. A 216-interleaf spiral with short readout (TADC = 3.71ms) was designed to minimize off-resonance artifacts, and was integrated into a spiral TSE acquisition with ETL=36, TEeff=153ms, TR=4000s

Phantom and in vivo data were obtained in this IRB-approved study on a 3T Siemens Vida scanner. Both fully-sampled and undersampled (R=3) spiral TSE data were collected. Additionally, a second spiral image was collected to correct spiral TSE artifacts3 and any additional off resonance artifacts7 with the same imaging parameters, but reversed interleaf sampling order and time-reversed interleaf gradient waveforms. Undersampled data were reconstructed with spiral GRAPPA8 using a single calibration frame collected with ETL=36, TEeff=160ms, and TR=500ms. A 32x8 (read x proj) calibration segment was used to obtain enough kernel repetitions to determine the GRAPPA weights. For comparison, a Cartesian TSE image was acquired with 300mm2 FOV, 1.17x1.17mm2 resolution, 201Hz/px bandwidth, ETL=20, TEeff = 102ms, TR=4000s, and GRAPPA R=2 with integrated ACS lines.

Phantom data were acquired using a 16-channnel head array to compare the apparent resolution and contrast of spiral TSE, accelerated spiral TSE, and clinically-used Cartesian TSE. A fat fraction phantom9 with vials containing 0%, 10%, 20%, 30%, 40%, 50% and 100% fat fraction was used to assess apparent resolution to observe impact of fat off resonance at different fat fraction regimes. Apparent resolution is defined by the % increase in vial diameter with the termination of the vial edge defined as a drop to 10% of mean vial signal. Contrast was assessed by computing the average signal of each vial normalized by the highest signal vial in the T2-array of the ISMRM/NIST MRI system phantom10. In vivo data were collected from four healthy volunteers using a 30-channel body array.

Results

Figure 2 shows that spiral TSE variants had a maximum apparent vial size increase of 9.1% compared to 7.2% in the Cartesian readout direction and 14.4% in the Cartesian phase encoding direction, respectively, in high fat fraction vials. At low fat fraction (≤20%), the maximum increase in apparent vial size was 8.7%, 7.2%, and 6.8% respectively and was comparable between all sequences. The contrast for vials with different T2 values was similar between the spiral acquisitions and Cartesian TSE except in vials with T2 values of less than 45ms, where spiral TSE signal was hypointense compared with Cartesian TSE images.

Figures 3 and 4 show in vivo images of the prostate collected using standard Cartesian TSE, Spiral TSE, and Spiral TSE with R=3 reconstructed with spiral GRAPPA. Spiral acquisition reduces chemical shift artifacts near the rectum and seminal vesicles (Figure 4). The acquisition of an additional spiral image for correction doubles acquisition time but also reduces artifacts around the phantom vials for all spiral TSE approaches (Figure 2), intensity artifacts near the bladder (Figure 3), and distortion artifact near the rectum (Figure 4), and recovers anatomic detail in the prostate (Figure 4).

Discussion

Fully sampled spiral TSE images can be acquired in 24s with increased noise compared to Cartesian TSE (Tacq=61s). Spiral TSE images with an acceleration factor of R=3 and non-Cartesian GRAPPA reconstruction can be collected in but suffer from increased blurring and noise enhancement. This issue could potentially be improved by using a lower TEeff, but necessitating a longer acquisition time or a long spiral readout with fewer interleaves that could enhance blur. The acquisition of additional spiral correction images reduces the appearance of artifacts in the ISMRM/NIST phantom and in vivo prostate images and reduces noise in both spiral TSE variants at the cost of acquisition speed. Further experiments in patients with pathology are necessary to assess lesion conspicuity using these approaches.

Conclusion

Spiral TSE with non-Cartesian GRAPPA can be used to acquire T2-weighted images of the prostate in a fraction of the time as gold-standard Cartesian acquisitions (8 seconds vs. 61 seconds) with similar contrast properties but enhanced noise/blurring. Corrections can be applied to further reduce artifacts at the expense of additional scan time. The work presented here could help accelerate probe targeting during in-gantry prostate biopsy, though additional acceleration is needed for real-time image guidance.

Acknowledgements

This work was supported by the NIH Grants: F30CA239355 and T32GM07250.

References

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2. Verma S, Choyke PL, Eberhardt SC, et al. The Current State of MR Imaging–targeted Biopsy Techniques for Detection of Prostate Cancer. Radiology. 2017;285(2):343-356. doi:10.1148/radiol.2017161684

3. Li Z, Karis JP, Pipe JG. A 2D spiral turbo-spin-echo technique. Magnetic Resonance in Medicine. 2018;80(5):1989-1996. doi:10.1002/mrm.27171

4. Li Z, Wang D, Robison RK, et al. Sliding-slab three-dimensional TSE imaging with a spiral-In/Out readout. Magn Reson Med. 2016;75(2):729-738. doi:10.1002/mrm.25660

5. Munsch F, Taso M, Zhao L, et al. Rotated spiral RARE for high spatial and temporal resolution volumetric arterial spin labeling acquisition. NeuroImage. 2020;223:117371. doi:10.1016/j.neuroimage.2020.117371

6. Wright KL, Hamilton JI, Griswold MA, Gulani V, Seiberlich N. Non-Cartesian Parallel Imaging Reconstruction. J Magn Reson Imaging. 2014;40(5):1022-1040. doi:10.1002/jmri.24521

7. Fielden SW, Meyer CH. A simple acquisition strategy to avoid off-resonance blurring in spiral imaging with redundant spiral-in/out k-space trajectories. Magn Reson Med. 2015;73(2):704-710. doi:10.1002/mrm.25172

8. Heidemann RM, Griswold MA, Seiberlich N, et al. Direct parallel image reconstructions for spiral trajectories using GRAPPA. Magn Reson Med. 2006;56(2):317-326. doi:10.1002/mrm.20951

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Figures

Figure 1: (A) A sequence diagram for a spiral TSE acquisition with ETL = 8 and ESP = 10ms for a 24 interleave spiral trajectory collected over one TR. (B) Spiral sampling resulting from collection of one TR from (A). Spiral shots are colored based on the echo time of their acquisition shown in (A). Acquisition of one TR of echoes produces a GRAPPA acceleration factor of three for this trajectory.

Figure 2: (A) Images collected in a fat fraction phantom (left) and NIST phantom (right) for each sequence. The fat fraction of each vial is shown in red in the Cartesian TSE image. (B) % change in apparent vial diameter from each vial of the fat fraction phantom by sequence. Measured vial diameter for Cartesian TSE is separated into phase encoding and readout directions due to differences in blurring in these two directions. (C) ISMRM/NIST phantom vial contrast relative to the vial measured to have a T2 of 276.1ms.

Figure 3: Images reconstructed with each sequence variant for all four in vivo volunteers. Intensity artifact (red arrow) reduced when correction acquisition is applied.

Figure 4: Reconstructed images from Figure 3 cropped to show the prostate and surrounding region. Distortion artifact (red arrow) is reduced and the rectal wall sharpness is recovered when correction acquisition is applied. Chemical shift artifact (blue arrow) near seminal vesicles and rectum does not appear in spiral TSE variants.

Proc. Intl. Soc. Mag. Reson. Med. 30 (2022)
0759
DOI: https://doi.org/10.58530/2022/0759