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Enabling Fast Metabolic Mapping of the Brain using Lipid Crushing and an EPSI Readout at 7T
Kyung Min Nam1, Arjan Hendriks1, Vincent O. Boer2, Dennis D.J. Klomp1, Jannie P. Wijnen1, and Alex Bhogal1
1Imaging & Oncology, UMC Utrecht, Utrecht, Netherlands, 2Danish Research Centre for Magnetic Resonance, Centre for Functional and Diagnostic Imaging and Research, Copenhagen University Hospital Hvidovre, Hvidovre, Denmark

Synopsis

Metabolic mapping at ultra-high field benefits from increased SNR and large chemical shift dispersion, enabling high spatial resolution and more resolved metabolite resonances. By exploiting increased SNR, MRSI acquisitions can be accelerated using echo-planar readout gradients (EPSI) or parallel imaging techniques. However, signal contamination from extra-cranial lipids can degrade the spectral quality and/or introduce fold-over artefacts. Therefore, suppression of extra-cranial lipids during acquisition is imperative for fast spectroscopic imaging. This work aimed to use a “crusher coil” to suppress extracranial lipid signals while acquiring metabolic information using a pulse-acquire acquisition with EPSI readout.

Introduction

Metabolic mapping at ultra-high field benefits from the increased SNR and large chemical shift dispersion, enabling high spatial resolution and more resolved metabolite resonances. However, increasing spatial resolution comes at the cost of prohibitively long scan-times. Moreover, lipid signal contamination due to the far-reaching the point-spread function associated with magnetic resonance spectroscopic imaging (MRSI) can cause unwanted artefacts that impede spectral quality. These effects can be amplified when using acceleration techniques such as SENSE 1,2 which can lead to fold-over artefacts 3. This is a critical problem considering the need to quantify metabolite distributions accurately. Lipid contamination can be avoided by using volume selection schemes such as semi-LASER 4; however, at the cost of long TR due to the specific absorption rate (SAR) limitations and limited spatial coverage. Another method for removing the lipid contamination is using L2 regularization 5 with short repetition times (i.e., TR<1000 ms) and very high spatial resolution (i.e., 128x128 matrix).6 Boer et al. 7 had shown that a crusher coil can effectively reduce lipid artefacts without any RF deposition in the brain. The sequence 8 enables the fast lipid suppression with high SNR per time unit using the crusher coil. To this end, this work aimed to present a pulse-acquire echo planar spectroscopic imaging (PA-EPSI) acquisition 9,10 including the lipid suppression using an external crusher coil at 7T.

Methods

Measurements were performed in a healthy volunteer using a 7T MR scanner (Achieva, Philips, the Netherlands) with a quadrature transmit and a 32 channel receiving head coil (Nova Medical, USA). Informed consent was obtained from the volunteer and the local ethics committee approved the experiment.
2D EPSI readout was acquired with the following parameters: FOV=192x192 mm2, one 12x12 and the other 6x6 mm2 voxel sizes, slice thickness=12 mm, temporal samples=512, VAPOR water suppression, and acquisition bandwidth=128 kHz. Additional parameters that differed between acquisition techniques are summarized (Table 1). For each acquisition, a non-water suppressed reference was acquired using similar parameters with 1 average. For all measurements, B0 shimming 11 was performed using up to 2nd order shim terms and an additional 3rd order shim amplifier was used to drive the crusher coil 7. A series of 3 measurements were performed to evaluate lipid signal leakage and suppression at the centre and periphery of the brain: 1) semi-LASER localization 4; 2) pulse-acquire (PA) with EPSI readout and no lipid suppression; 3) pulse-acquire with EPSI readout including lipid suppression using the crusher coil in figure 1. To compare the semi-LASER and pulse acquire techniques, the TR and flip angle were kept constant for the low-resolution acquisitions. To show the benefit of accelerated lipid suppressed MRSI, an additional measurement was performed at a higher spatial resolution using a shorter TR and optimized flip angle (for T1=1700: see table 1).12
During reconstruction, k-space lines of even EPSI echoes were reversed along the temporal dimension. A 2D phase correction was performed on both the water reference raw data and water suppressed raw data. Coil sensitivity maps were generated using the water reference raw data and subsequently used for channel combinations of water suppressed MRSI data. Further processing steps included the apodization function with a 2D hamming filter, spectral alignment, residual water removal, and eddy current correction. All data reconstruction steps were performed using in-house MATLAB scripts.

Resuts and discussion

Example spectra from the 3 difference acquisition methods (semi-LASER EPSI with FOCI, PA-EPSI with and without crusher coil) are shown in figure 2. As expected, the spectra acquired in the center of the brain (orange voxel, figure 2A) showed no or very little contamination from extra-cranial lipid signals when using the semi-LASER localization. For the EPSI acquisitions, the similar signal characteristics between 0.8 and 1.5 ppm suggest sensitivity to macromolecular contributions due to short TE rather than the extra-cranial lipid contamination. Moving away from the center of the brain, lipid signal contamination was evident for non-suppressed PA-EPSI in figure 2C. When looking at regions close to the skull, the lipid signal contamination overshadows metabolite signals in figure 2D. However, at these locations (blue voxel, figure 2A), lipid suppressed PA-EPSI provided good spectra while the semi-LASER acquisition did not provide enough spatial coverage to acquire spectra in the region.
This observation is confirmed in the higher resolution of MRSI data shown in figure 3C and D. Even though the semi-LASER localization restricts the signal to the localization volume (VOI), some lipid contamination is present at the corner of the VOI when it is closely positioned to the skull. Furthermore, the semi-LASER is less sensitive to metabolites with short T2 because of the relative long TE and limits relatively long TR by the RF power deposition (i.e., SAR). Therefore the semi-LASER is not an SNR efficient approach at high field. The MR spectra from the lipid suppressed PA-EPSI measurement were of good quality compared to the MR spectra from the PA-EPSI measurement without crushing in figure 4.

Conclusion

In this work, we successfully demonstrate the feasibility of accelerated MRSI acquisition while suppressing lipids using an external crusher coil. This work sets up the possibility to investigate optimal acquisition strategies for the fast whole-brain MRSI at 7T.

Acknowledgements

We like to thank Eurostars IMAGINE and Marie-Curie ITN INSPiREmed for financial support.

References

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3. Nassirpour S, Chang P, Avdievitch N, Henning A. Compressed sensing for high‐resolution nonlipid suppressed 1 H FID MRSI of the human brain at 9.4T. Magn Reson Med. 2018; 80: 2311– 2325.

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7. Boer, VO and van, de Lindt T and Luijten, PR and Klomp, DW. Lipid suppression for brain MRI and MRSI by means of a dedicated crusher coil. Magn Reson Med 2015; 73:2062-8.

8. Ma J, Wismans C, Cao Z, Klomp DWJ, Wijnen JP, Grissom WA. Tailored spiral in‐out spectral‐spatial water suppression pulses for magnetic resonance spectroscopic imaging. Magn Reson Med. 2018 Jan; 79(1):31-40.

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Figures

Figure 1. Schematic of crusher coil control and pulse sequence diagrams for PA-EPSI and semi-LASER EPSI acquisitions A: The trigger signal generated by the spectrometer initializes an external amplifier which drives the crusher coil. Shim power is controlled via an external PC connected to a dynamic shim updating unit. B: Pulse sequence diagram for PA-EPSI acquisition: the duration of the suppression gradient (red) is 1.8 [ms]. C: Semi-LASER EPSI with FOCI shows the high number of required preparation pulses, leading to a long TE, before starting EPSI readout compared to PA-EPSI.

Figure 2. Comparison of semi-LASER EPSI (blue), PA-EPSI with (red)/ without (green) crushing in the lower resolution A: Two anatomical images show a brain image and lipid-suppressed image acquired by a gradient echo without/with crushing. The VOI of semi-LASER is shown by the dotted white line. Spectra from each acquisition of the centre voxel (orange square) and voxel outside of the VOI (blue square) are shown in B and D. C: Spectra from the middle region of the brain (red box). Note the suppressed lipids in the spectra of the two pink boxes when using PA-EPSI with the crusher coil.

Figure 3. Comparison of semi-LASER EPSI (blue), PA-EPSI with (red)/without (green) crushing A: Gradient echo anatomical images showing the effect of crushing (right). The dotted white line represents the semi-LASER localization region. The pink square is located at the center. B: Comparison of spectra obtained using 3 different EPSI acquisition methods in the central brain region. C: Spectra from the central brain region (cyan) demonstrate the effect of lipid suppression for PA-EPSI sequence. D: Spectra shown from regions outside semi-LASER localization box (yellow).

Figure 4. Comparison of PA-EPSI with (red)/ without (green) crushing acquired at voxel size (6 x 6 mm2) A: Lipid map showing the effect of crushing (right), which shifted by 2 voxels based on the anatomical image in figure 3A. The dotted red line represents the region of interest (ROI). The white line shows the chemical shift region. B: Comparison of spectra acquired using 2 different EPSI acquisition methods at ROI.

Table 1. MRSI sequence parameters

Proc. Intl. Soc. Mag. Reson. Med. 28 (2020)
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