Christoph Stefan Aigner1, Manuel Fernando Sánchez Alarcon1,2, Alexandre D'Astous3,4, Eva Alonso-Ortiz3,4, Julien Cohen-Adad3,4,5,6, and Sebastian Schmitter1,7,8
1Physikalisch-Technische Bundesanstalt (PTB), Berlin, Germany, 2Charité – Universitätsmedizin Berlin, Berlin, Germany, 3NeuroPoly Lab, Institute of Biomedical Engineering, Polytechnique Montréal, Montreal, QC, Canada, 4Centre de recherche du CHU Sainte-Justine, Université de Montréal, Montréal, QC, Canada, 5Functional Neuroimaging Unit, CRIUGM, Université de Montréal, Montréal, QC, Canada, 6Mila-Quebec AI Institute, Montréal, QC, Canada, 7Medical Physics in Radiology, German Cancer Research Center (DKFZ), Heidelberg, Germany, 8Center for Magnetic Resonance Research, University of Minnesota, Minneapolis, MN, United States
Synopsis
Keywords: Parallel Transmit & Multiband, Parallel Transmit & Multiband, 7 Tesla, Spinal Cord, Universal Shim
Motivation: Addressing the issue of lengthy parallel transmit (pTx) adjustment times caused by the absence of a dedicated spinal cord (SC) coil setting, which limits SC imaging at ultra-high field.
Goal(s): Enhance imaging efficiency by universal shim modes that can be applied without the need for additional adjustment time for different SC regions and coils.
Approach: We have built a library of channel-wise B1+ maps and optimized universal RF shims to optimize transmit homogeneity and efficiency.
Results: The proposed universal shims significantly improve B1+ efficiency, achieving a 50% enhancement compared to the default shim mode, while eliminating the need for subject-specific pTx adjustments.
Impact: The development of universal shims not only enhances SC imaging efficiency at ultra-high field but also streamlines the
process by eliminating lengthy subject-specific pTx adjustments, expecting SC
imaging to become more usable for non-pTx experts.
Introduction
Ultrahigh-field (UHF) MRI has shown to improve the diagnosis
of neurological disorders within the human brain.1 However,
extending it to the spinal cord (SC) still faces challenges like spatial
flip-angle (FA) variations, limited transmit efficiency, and motion interference.2
To address spatial FA variations, tailored and universal parallel transmission
(pTx) techniques have been proposed.3-6 However, dynamic pTx
is more susceptible to ΔB0 variations and exhibit reduced lower
temporal B1+ efficiency than static pTx (RF
shimming). These challenges are amplified in SC imaging due to the lower B1+ efficiency and more pronounced ΔB0 variations compared to the human
brain. Therefore, universal RF shim solutions have recently been proposed for
the brain and cervical spine in a simulation study.7
In this in-vivo study, we investigate the feasibility and
benefits of using universal RF shims (US) to optimize FA distributions in the
cervical, thoracic, and lumbar spine. The US solutions were successfully
validated at 7T in three previously unexamined volunteers, covering the
cervical and the thoracolumbar SC, respectively.Methods
MRI
scans were performed on 21 healthy volunteers (9M/12F, 21-56years, 18-35kg/m2)
at 7 Tesla (Magnetom 7T, Siemens, Germany) using pTx (step2.3) and two certified
RF coils (MRI.Tools GmbH, Germany). One coil was tailored for carotid imaging
(8TX/8RX), while the other was optimized for heart imaging (8TX/32RX).
Relative
B1+ maps
for US calculations were acquired differently for the cervical spine (C-Spine)
and thoracolumbar spine (T/L-Spine) under free-breathing. For C-Spine, 2D B1+ maps
were obtained with a Cartesian gradient-echo (GRE) sequence8 (nominalFA=15°,
TE/TR=1.78/4ms, FOV=384x224mm2, voxel-size=2x2x4mm3). In
T/L-Spine, 3D B1+ maps
were collected for each volunteer using a radial phase-encoding GRE scan9 (nominalFA=20°,
TE/TR=2.02/40ms, FOV=250x312x312mm3, voxel=2x2x2mm3,
TA=205 seconds).
Universal
phase-only RF shims were individually optimized for the C- and T/L-Spine using
a training library of 6 and 9 volunteers, respectively. The US design aimed to
balance homogeneity using the coefficient of variation (CV): $$CV=\frac{std(\left|\sum_{ch=1}^{N_c}{B_{1,ch}^+b_{ch}}\right|_{ROI})}{mean(\left|\sum_{ch=1}^{N_c}{B_{1,ch}^+b_{ch}}\right|_{ROI})},$$ and
the transmit efficiency (η):
$$\eta=\frac{\left|\sum_{ch=1}^{N_c}{B_{1,ch}^+b_{ch}}\right|_{ROI}}{\sum_{ch=1}^{N_c}\left|B_{1,ch}^+\right|_{ROI}},$$ based
on channel-wise B1+ maps in the library combined with one global set of complex
RF phase factors for
manually selected SC regions of interest (ROIs).
Three
unseen test-cases underwent additional, vendor-provided absolute B1+ mapping10
w/wo the US (nomFA=8°, TE/TR=2.18/5000ms, FOV=384x384mm2,
slice-thickness=5mm).
2D
GRE-based ΔB0 maps
were obtained in the C-Spine (nomFA=20°, TE1/TE2/TR=3.06/4.08/818ms,
FOV=256x256x256mm3, voxel=2x2x2mm3) for subject-tailored B0 shimming
(up to the 2nd order) using SC Shimming-Toolbox.11 The regularized
least-squares B0 shimming
process involved the following pre-processing steps: manual selection of the
C-Spine centerline, automated cylindrical mask generation (d=20mm), and phase
unwrapping (scikit-image;
threshold=0.05).
3D
high-resolution Cartesian multi-echo GRE scans were obtained for C-Spine under
free-breathing (nominalFA=10°, TE1/TE2/TE3/TR=2.04/4.08/6.12/27.69ms,
FOV=352x212x192mm3, voxel=1x1x1mm3), and during
breath-hold in 2D for T/L-Spine (nominalFA=30°, TE1/TE2/.../TE5/TR=2.25/5.25/.../14.25/40ms,
FOV=384x244mm2, voxel=1x1x2mm3).Results and Discussion
Figs. 1 and 2 compare the default shim (not optimized
for the SC) with C- and T/L-Spine universal shims (US). In C-Spine test cases,
the US showed a slight CV reduction (29% to 28%) and a two-fold η increase
(0.44 to 0.83). Similar trends were observed in the T/L-Spine. Across all test cases,
US reduced the CV by two-fold (30% to 13%), and η doubled (0.42 to 0.78). Note,
that the cost function was weighted 90% by η and 10% by CV, which could be
changed if desired.
Fig.3 displays the absolute FA measurements. On
average, measured FAs in the C-Spine increased by 51% from 52° (default) to 79°
(US). Similarly, in the T/L-Spine region, a 48% FA increase is observed, with measured average FAs of 25° (default) and 37° (US).
Fig.4 displays the measured ΔB0 variations in the C-Spine using the vendor-supplied tune-up and optimized B0
shims. A notable reduction in
RMSE (296Hz vs. 102Hz) and standard deviation (117Hz vs. 102Hz) is observed.
Tailored B0 shimming
in the T/L-Spine region was not possible due to substantial motion artifacts in the Cartesian ΔB0 maps,
necessitating further work to develop a motion-robust approach.
Fig. 5 presents a sagittal slice of the 3D GRE images
acquired during free-breathing using US in the C-Spine and customized B0
shims. Additionally, a 2D GRE image was acquired during a breath-hold using US
in the T/L-Spine for all three test subjects. Qualitatively, good image quality
is evident, even at longer echo times, confirming the feasibility of
calibration-free pTx across the entire SC. Conclusion
This in-vivo study highlights the efficacy of US for calibration-free SC imaging at 7T for different SC
regions and RF coils. The application of US enables seamless pTx in the SC,
eliminating the requirement for time-consuming calibration procedures. This
approach, in combination with motion-robust non-Cartesian encoding, holds
promise for advancing SC-imaging capabilities at 7T and higher field strengths.Acknowledgements
We gratefully acknowledge funding from the
German Research Foundation SCHM 2677/2-1, SCHM 2677/4-1 and GRK2260, BIOQIC.References
[1] Ladd, E, Bachert, P, Meyerspeer, M, et al. Pros
and cons of ultra-high-field MRI/MRS for human application, Prog. Nuc. Magn.
Reson. Spec. 2018; 109:1-50. doi: 10.1016/j.pnmrs.2018.06.001
[2] Barry, RL, Vannesjo, SJ, By, S, Gore, JC, Smith,
SA. Spinal cord MRI at 7T. Neuroimage 168, 437–451. doi: 10.1016/j.neuroimage.2017.07.003.
[3] Padormo, F., Beqiri, A., Hajnal, J. V., and Malik,
S. J. (2016), Parallel transmission for ultrahigh‐field imaging. NMR Biomed.,
29: 1145– 1161. doi: 10.1002/nbm.3313
[4] Gras, V., Vignaud, A., Amadon, A., Le Bihan, D.
and Boulant, N. (2017), Universal pulses: A new concept for calibration‐free
parallel transmission. Magn. Reson. Med., 77: 635-643. doi:10.1002/mrm.26148
[5] Aigner, CS, Dietrich, S, Schaeffter, T, Schmitter,
S. Calibration-free pTx of the human heart at 7T via 3D universal pulses. Magn
Reson Med. 2021; 87: 70– 84. doi: 10.1002/mrm.28952
[6] Papp, D, Boulant, N, Massire, A, Mauconduit, F,
Gras, V, Cohen-Adad, J. Universal pulses for the cervical spinal cord at 7T: a
feasibility study, ISMRM 2023, 0199.
[7] Kazemivalipour, E, May, MW, Rangaprakash, D, Bilgic, B, Stockman, JP, Barry, RL,
Keil, B, Wald, LL, Guerin, B. Design of a universal RF-shimming drive mode for
head and neck imaging at 7 Tesla using a 16-channel pTx array, ISMRM 2023, 4406
[8] Schmitter, S., DelaBarre, L., Wu, X., Greiser, A.,
Wang, D., Auerbach, E.J., Vaughan, J.T., Uğurbil, K. and Van de Moortele, P.-F.
(2013), Cardiac imaging at 7 tesla: Single- and two-spoke radiofrequency pulse
design with 16-channel parallel excitation. Magn. Reson. Med., 70: 1210-1219.
https://doi.org/10.1002/mrm.24935
[9] Dietrich, S, Aigner, CS, Kolbitsch, C, et al. 3D
Free-breathing multichannel absolute B1+ Mapping in the human body at 7T. Magn
Reson Med. 2021; 85: 2552– 2567. doi: 10.1002/mrm.28602
[10] Fautz HP, Vogel M, Gross P, Kerr A, Zhu Y. B1
mapping of coil arrays for parallel transmission. In Proceedings of the 16th
Annual Meeting of ISMRM, Toronto, Canada, 2008. Abstract 1247.
[11] D'Astous A,
Cereza G, Papp D, Gilbert KM, Stockmann JP, Alonso-Ortiz E, Cohen-Adad J.
Shimming toolbox: An open-source software toolbox for B0 and B1 shimming in
MRI. Magn Reson Med. 2022; 1-17. doi:10.1002/mrm.29528