Natalia Dudysheva1, Michel Luong2, Alexis Amadon1, Nicolas Boulant1, and Vincent Gras1
1BAOBAB, NeuroSpin, University Paris-Saclay, CEA, CNRS, Gif-sur-Yvette, France, 2IRFU/DACM, University Paris-Saclay, CEA, Gif-sur-Yvette, France
Synopsis
Keywords: Safety, Safety, SAR, ultra-high field, pTX, pediatric
Motivation: Pediatric MRI neuroimaging has become common practice at 1.5 and 3 Tesla and we see the emergence of 7T and parallel transmission (pTX). However, today relevant local SAR prediction models are based on adult standards.
Goal(s): In this work, we study the local SAR at 7T with pTX for children population (6 to 14 years old) using RF electric field simulations.
Approach: We exploit a vast simulation database to build a pediatric local SAR prediction model and propose a methodology for its initial validation using convex optimization.
Results: A large simulation database (above 25) is desirable to combine RF safety and pTX performance.
Impact: This work aims to push
pediatric MRI to ultra-high fields by developing safe SAR control for the children
population. It also introduces a tool to determine appropriate safety margins to
avoid excessive penalizing in the pTX pulse design.
Introduction
Local SAR control in parallel transmission (pTX)
conventionally relies on virtual observation points (VOPs)1. These
SAR control matrices
are generally obtained from electromagnetic (EM) simulations on virtual body
models. Due to modeling errors, inter-subject anatomical variability, and limited control of head position in the coil, the designed VOPs must
incorporate safety margins2,3. In pediatric neuroimaging, the head
size and position are more likely to vary, which makes adult VOPs possibly inapplicable
without revising the safety margins. Increasing them will reduce the risk of
SAR hotspots but will result in RF power over-restriction and suboptimal RF pulses. This
work aims to develop a dedicated local SAR model for children aged 6 to 14 years and to compute adapted safety factors. Using EM simulations for various
numerical head models ($$$\small{NHMs}$$$) for
a pTX home-made coil, we construct pediatric VOPs and propose a method
to test their safety level with a convex optimization algorithm.Theory
Let us denote by $$$\small{\left\{\mathbf{Q}\right\}_{n}≔\left\{\mathbf{Q}_{n}\left(\mathbf{r}\right)\in\mathbb{C}^{N_{ch}\text{x}N_{ch}}\middle|\mathbf{r}\in{NHM}_{n}\right\}}$$$ the local SAR matrices for
the nth $$$\small{NHM}$$$ and by $$$\mathcal{V}$$$ the
pTX RF excitation vector4. Suppose that VOP matrices $$$\small{\left\{\mathbf{Q^{*}}\right\}}$$$ are constructed for M $$$\small{NHMs^{VOP}}$$$, and
we want to verify their safety potential on other set of N $$$\small{NHMs^{test}}$$$ represented
by $$$\small{\left\{\mathbf{Q}\right\}_{n=1..N}}$$$. To test the set $$$\small{\left\{\mathbf{Q^{*}}\right\}}$$$ against each $$$\small{\mathbf{Q}_{n}\left(\mathbf{r}\right)\in\left\{\mathbf{Q}\right\}_{n}}$$$ independently on the RF excitation, we use the R-criterion: $$\small{R\left(\mathbf{Q}_{n}\left(\mathbf{r}\right),\left\{\mathbf{Q}^{*}\right\}\right)=\max_{\mathcal{V}\in\mathbb{C}^{Nch}}\left(\frac{SAR(\mathbf{Q}_{n}\left(\mathbf{r}\right),\mathcal{V})}{{SAR}^{*}\left(\left\{\mathbf{Q^{*}}\right\},\mathcal{V}\right)}\right) [Eq.1],}$$ where the maximization is amongst all static RF shims $$$\mathcal{V}$$$, and $$$\small{{SAR}^{*}\left(\left\{\mathbf{Q^{*}}\right\},\mathcal{V}\right):=\max_{\mathbf{Q^{*}}\in\left\{\mathbf{Q^{*}}\right\}}{\left(\mathcal{V}^{H}\mathbf{Q^{*}}\mathcal{V}\right)}}$$$. It was shown5
that i) computing R reduces to a numerically tractable convex optimization
problem, and ii) the R criterion is in fact equal to the worst-case ratio of $$$\small{SAR}$$$ to the VOP-calculated $$$\small{SAR^{*}}$$$considering all dynamic
RF excitations. Thus, the condition R<1 is sufficient for the VOP set to overestimate
the SAR for the given $$$\small{\mathbf{Q}_{n}\left(\mathbf{r}\right)}$$$ for
any pTX pulse. Moreover, since for any k>0: $$\small{R\left(\mathbf{Q}_{n}\left(\mathbf{r}\right),\left\{{k\mathbf{Q}}^{*}\right\}\right)=\frac{1}{k}R\left(\mathbf{Q}_{n}\left(\mathbf{r}\right),\left\{\mathbf{Q}^{*}\right\}\right) [Eq.2]}$$ the factor $$\small{k:=\max_{\mathbf{Q}_{n}\left(\mathbf{r}\right)\in\left\{\mathbf{Q}\right\}_{n}}\left(R\left(\mathbf{Q}_{n}\left(\mathbf{r}\right),\left\{Q^{*}\right\}\right)\right) [Eq.3]}$$ gives precisely the minimum multiplicative safety margin that we shall apply to the VOP set $$$\small{\left\{ \mathbf{Q}^{*} \right\}}$$$ to make them safe with respect to nth $$$\small{NHM^{test}}$$$.Methods
The SAR analysis builds on EM
simulations made for 8TX/32RX head coil6 at 298MHz with the FDTD
method (2x2x2mm3). We used a home-made NHM database7 containing 68
subjects aged between 4 and 16 years (Fig.1). This database was divided on two
parts: subgroups $$$\small{NHMs^{VOP}}$$$ of different sizes were used to construct VOPs,
other subgroups $$$\small{NHMs^{test}}$$$ represented the test sample.
VOP construction: thirty-five VOP sets $$$\small{\left\{\mathbf{Q^{*}}\right\}_{[M]}}$$$ were constructed on an increasing number of head models M=2..30 spanning
the age distribution (Fig.2). To compute VOPs, we used the R-criterion-based
algorithm of ref. 5.
VOP testing: Each VOP set $$$\small{\left\{\mathbf{Q^{*}}\right\}_{[M]}}$$$ was
tested on N=30 models not used for VOP construction. For every test subject $$$\small{NHM^{test}_{n=1..N}}$$$, we computed the R-criterion map $$$\small{Rmap(n):=\left\{R\left(\mathbf{Q}_{n}\left(\mathbf{r}\right),\left\{\mathbf{Q^{*}}\right\}_{[M]}\right)\middle|\mathbf{r}\in{NHM}_{n}^{test}\right\}}$$$, the maximum R-criterion value $$$\small{SubjRmax(n):=\max_{\mathbf{r}\in{NHM}_{n}^{test}}{Rmap\left(n\right)}}$$$, and the risk mass $$$\small{SubjRiskMass(n):=numel\left(Rmap\left(n\right)>1\right)·{(2mm)}^{3}·1kg/l}$$$ with numel denoting the voxel
number. This allowed us to define
- strict multiplicative safety factor $$$\small{MSF(M)=\max_{n\in1..N}{SubjRmax(n)}}$$$ needed to provide VOP sets $$$\small{MSF(M)·\left\{\mathbf{Q^{*}}\right\}_{[M]}}$$$
passing the safety test on all the $$$\small{NHMs^{test}}$$$ (Eq. 3).
-
relaxed safety factor $$$\small{{rMSF}(M)}$$$ by which one needs to multiply all
matrices of $$$\small{\left\{\mathbf{Q^{*}}\right\}_{[M]}}$$$
to obtain $$$\small{\max_{n\in1..N}{SubjRiskMass(n)}<1g}$$$
.Results
Fig.3 displays the $$$\small{SubjRmax}$$$ and $$$\small{SubjRiskMass}$$$ distributions as a function of M. The difference between the R-maps for the same test model obtained
with two VOP sets $$$\small{\left\{\mathbf{Q^{*}}\right\}_{[5]}}$$$ and $$$\small{\left\{\mathbf{Q^{*}}\right\}_{[30]}}$$$ is shown in
Fig.4. We can observe that $$$\small{SubjRmax}$$$ and
$$$\small{SubjRiskMass}$$$ decrease with M. Fig.5 provides the plots of $$$\small{MSF}$$$ and $$$\small{rMSF}$$$ showing their convergence with M. A fit with the model: $$\small{MSF=1+A·M^{-p} [Eq.4]}$$ returns p=0.90 for $$$\small{MSF}$$$ and p=1.12
for $$$\small{rMSF}$$$, leading to the safety margins for 30 $$$\small{NHMs^{VOP}}$$$ of 1.57
and 1.31 respectively.Discussion and Conclusion
The described approach allows one to verify in simulation the safety level of a given VOP set and to determine
the appropriate safety margins. The R-criterion gives directly the worst-case ratio of $$$\small{SAR}$$$ to $$$\small{SAR^{*}}$$$ and
thus does not rely on Monte-Carlo simulations across RF shims4.
We showed that, according to the criterion used, using only a few models
for computing the VOPs requires exceedingly restrictive MSFs possibly leading to
pTX performance issues. Reducing the MSF in turn poses a high risk of
underestimating the local SAR due to variations in head size and position.
Based on our simulation data, above 30 NHMs are recommended to compute the
VOPs. To construct final VOPs on the entire database of 68 NHMs, we applied $$$\small{MSF}$$$ of 1.28 according to empirical
formula 1+12.3M-0.9. Note that the form of
the latest depends on additional safety margins. Provided our database is
representative enough, we can use the simulation-based results for pediatric
exams. Acknowledgements
This work received the financial support of the French National research Agency (Collaborative research project MOSAR ANR-21-CE19-0028). We acknowledge the financial support of the Cross-Disciplinary Program on Numerical Simulation of CEA, the French Alternative Energies and Atomic Energy Commission. Edouard Chazel (University of Paris-Saclay, CEA) is thanked for assembling the RF coil.References
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