Jiying Dai1,2, Mark Gosselink1, Alexander J. E. Raaijmakers1,3, and Dennis W. J. Klomp1
1UMC Utrecht, Utrecht, Netherlands, 2Tesla Dynamic Coils B.V., Zaltbommel, Netherlands, 3Eindhoven University of Technology, Eindhoven, Netherlands
Synopsis
Keywords: Image Reconstruction, Spectroscopy
We utilized a quintuple-tuned RF head coil array by
using the high-SNR
23Na signals from the brain to optimize the weighting for
combining signals from the same coil array elements for the low-concentrated
31P
metabolites.
23Na-weighted Roemer combination of
31P MRSI
signals is verified on EM simulations and MR experiments. Comparing to
31P
self-weighted combination,
23Na-weighted combination shows higher
SNR and better-combined spectra in regions with low intrinsic SNR. It also
shows potential of mitigating the
signal contaminations when using
31P-self-weights for
31P
data acquired with large voxels.
Introduction
31P MRSI is a powerful tool to study energy
metabolism1 and cell proliferation and therefore being used in cancer
treatment efficacy monitoring2. However, 31P MRSI is not
widely used because of the low 31P SNR, (caused by low natural
abundance and low gyromagnetic ratio compared to 1H). To harvest
all potential SNR, some researchers use close-fit loop arrays for signal reception.
However, the multi-channel signal combination3 can be challenging at
low-SNR regions because coil sensitivity distributions are difficult to measure.
Self-weighted techniques like WSVD4 combination and PCA based
denoising have made significant progress in this area5. In this
study, we explore the feasibility of another approach enabled by a coil array
design which contains 15 loop-coils tuned to phosphorous, sodium and carbon6.
We will investigate combining multi-channel 31P signals using the
sensitivity distributions of 23Na
which is expected to be similar because they share the same coil array geometry
and the frequencies of operation of both nuclear species are still in near-field regime.
Self-weighted Roemer
combination method works reasonably well if SNR is sufficiently large (e.g. brain).
However, when it comes to the body region, or regions surrounded by highly
concentrated 31P signals (i.e. muscle), the low-SNR makes
self-weighted combination more problematic, while on top of this the signals contain
a significant portion of voxel bleeding from neighboring voxels and therefore
no longer represent the coil sensitivity.
This study will
investigate the potential for using 23Na sensitivity maps for signal
combination of 31P MRSI. We will test the applicability by EM
simulations and brain MRSI scans. As the self-weighted Roemer combination is
still robust in most brain regions, our experiment with 23Na-weights
can be validated. Methods
Simulations: We performed EM simulations on Sim4Life (Zurich
Med Tech, CH). We simulated the B1- fields at the
frequencies of 31P and 23Na on DUKE7. Figure 1a
shows the simulated model. By approximating 31P signals with
simulated B1-*, we compared self-weighted and 23Na-weighted
Roemer combinations by evaluating the theoretical SNR. Equation 1 is used for SNR
evaluation3, omitting all global scaling factors:
$$SNR^2=\frac{(\omega MV)^2 \sum_{i=1}^N \sum_{k=1}^N n_i n_k B_{ti} B_{tk}}{4KT\Delta f \sum_{i=1}^N \sum_{k=1}^N n_i n_k R_{ik}\cos(\theta_i - \theta_k)} \qquad \text{(Eq1)}$$
MR experiments: The MR experiments were performed on a 7T MRI
system (Philips Healthcare, Best, the Netherlands). An embedded-in-bore
birdcage coil is used for 31P transmission. A Helmholtz coil is used
for 23Na transmission. A quintuple-tuned head coil6 is
used for reception. Figure 1b-c show the coil. 31P MRSI is acquired
with the following specs: FOV = 320(FH)x260(AP)x240(RL) mm3,
resolution = 20x20x20 mm3, TR = 300 ms, TE = 0.5 ms, FA = 20°,
readout bandwidth=5000 Hz, 18 averages. 23Na MRI was acquired with
the same resolution.
Data processing: Data processing is performed in Python for
simulations and on MATLAB (The MathWorks, Inc.) for MR data. PCA-based
denoising5 is performed after signal combination. Roemer’s
optimal-SNR method is used for multi-channel signal combination (Eq2 below). We
implement the 23Na weights by replacing the $$$b$$$ in Eq2 with 23Na
MRI of identical resolution. The channel-wise constant 31P/23Na
phase offset due to arbitrary phase shifts in the Rx chain is calibrated according
to the 31P/23Na phase discrepancy at the maximum-23Na-signal
locations.
$$P=C \frac{p^T R^{-1} b}{\sqrt{b^T R^{-1}b^*}} \qquad \text{(Eq2)}$$
Results
B1- maps comparison: Figure 2 shows the simulation-based comparison
between the two combination methods on two sampled slices. The SNR can drop by 10%
to 20% when using 23Na weights.
In
vivo MR: Figure
3 shows the SNR analysis of combined 31P MRSI from an in vivo scan. The second and the third
row correspond to the SNR of the combined signals with 31P-self-weights
and with 23Na weights respectively. Figure 4 compares these two
methods by presenting the combined MRSI of slice 4. Figure 5 presents combined spectra
comparisons of more sampled voxels.Discussion
Simulations
demonstrate that the weights for 31P coil element combinations can
be correctly determined from 23Na signals of the same coil elements
to maintain highest sensitivity. Also for most in vivo slices the 23Na weights are well assessed.
However, looking at the first three columns of Figure 3, it seems like
self-weighted Roemer combination generates undoubtably higher SNR for 31P MRSI. In fact, in center voxels the 23Na-weighted method shows almost no signal where self-weights
combination shows outstanding SNR. It should be noted however that these center
voxels are mainly in CSF where 31P concentration is low and sodium
content high. Moreover due to the large voxels, there
will be substantial point-spread contributions from higher signals from neighboring
voxels towards the coils. Consequently, the observed signal will not provide
the correct amplitude and phase weighting information for coil combinations. In
the 31P-(self)-weighted reconstruction, SNR seems high, but this may
be severely biased by optimizing the weights for the point-spread contribution.
This is confirmed by substantial artefacts in 31P spectra from areas
in the head close to tissue interfaces when using self-weighting while the
spectra have good quality when using 23Na weighting.Conclusion
By using the same
receive elements, 23Na-weighted
Roemer combination of 31P CSI performs well in brain, and it even
shows potential advantage over 31P-self-weights. Acknowledgements
Great thanks to Lieke van den Wildenberg and Ayhan Gursan for their guide in data precessing!References
[1] Chen C, Stephenson
MC, Peters A, Morris PG, Francis ST, Gowland PA. 31P magnetization transfer
magnetic resonance spectroscopy: assessing the activation induced change in
cerebral ATP metabolic rates at 3 T. Magn Reson Med. 2018;79(1):22-30.
[2] van der Kemp WJM, Stehouwer BL, Luijten
PR, van den Bosch MAAJ, Klomp DWJ. Detection
of alterations in membrane metabolism during neoadjuvant chemotherapy in patients
with breast cancer using phosphorus magnetic resonance spectroscopy at 7 Tesla.
Springerplus. 2014;3(1):1-7.
[3] Roemer PB, Edelstein WA, Hayes CE, Souza
SP, Mueller OM. The NMR phased
array. Magn Reson Med. 1990;16(2):192-225.
[4] Rodgers CT, Robson
MD. Receive array magnetic resonance spectroscopy: whitened singular value
decomposition (WSVD) gives optimal Bayesian solution. Magnetic Resonance in
Medicine: An Official Journal of the International Society for Magnetic
Resonance in Medicine. 2010;63(4):881-891.
[5] Froeling M, Prompers JJ, Klomp DWJ, van
der Velden TA. PCA denoising and
Wiener deconvolution of 31P 3D CSI data to enhance effective SNR and improve
point spread function. Magn Reson Med. 2021; 85: 2992–
3009. https://doi.org/10.1002/mrm.28654
[6] Dai J, Meliadò EF, Gosselink WJM, Arteaga
C, Raaijmakers AJE, Klomp DWJ. Generalized
approach of quadruple or quintuple-tuned RF coil setups for metabolic MRI
throughout the body at 7 Tesla. ISMRM2022 Annual meeting, Abstract number 0711.
[7] Christ A, Kainz W,
Hahn EG, et al. The Virtual Family—development of surface-based anatomical
models of two adults and two children for dosimetric simulations. Phys Med
Biol. 2009;55(2):N23.