Synopsis
High field MRI systems offer better performance
in terms of signal-to-noise ratio but are burdened with dielectric resonance
artefacts inducing zones of weak excitation with major consequences on Signal
and Contrast to Noise Ratios. In this work, the interest of subject-tailored kT-points
pulse design with joint SAR control over current patient-specific RF-shimming
technique is investigated, in the context of human liver imaging at 3T. T1w
acquisitions are performed in-vivo to compare quadrature, tailored RF-shimming,
and kT-points pulses. The interest of kT-points is
clearly demonstrated in terms of signal, contrast and diagnostic power.
Introduction
3T MRI
systems are now widely available and extensively used in clinical environments
as they provide a better signal-to-noise ratio (SNR), which can be used to
improve spatial or temporal resolution.1 However, the dielectric resonance artefacts induced in
regions whose size is close to the radiofrequency (RF) wavelength lead to loss
of signal and contrast in some areas of larger organs such as the liver.1-3
Since the
advent of two-channel parallel transmission (pTX) clinical scanners,
subject-specific static RF shimming has been admitted as an efficient solution
to this issue. 4,5 Dynamic pTX approaches 3,6 have been
introduced, following the example of ultra-high field MRI, but without explicit
nor look-ahead SAR control. The kT-points approach,
however, has demonstrated excellent flip angle (FA) homogenisation performance
for non-selective excitation in the brain at 7T, 7,8 while ensuring
a safe SAR level. In this work, the applicability of kT-points to
achieve excitation homogeneity over a human abdomen in a clinical environment
on a CE-labelled 3T scanner is analysed. To the authors’ knowledge, this is the
first evaluation of dynamic excitation homogenisation in the abdomen at 3T
under strict SAR constraint. Materials and Methods
Acquisitions
were carried out on a clinical Siemens MAGNETOM Skyra 3T scanner (Siemens
Healthineers, Erlangen, Germany), fitted with a product two-channel pTX system.
Measurements were performed on the abdomen of a 38-year-old female patient (BMI
= 30) investigated for characterisation of a hepatic nodule. In order to rely
as much as possible on tools available on product scanners, B1+ maps
were obtained through a manufacturer standard adjustment procedure, along with the
associated virtual observation points 9 (VOP) used for SAR
calculation. Although an f0 map –
needed for the pulse design – was also provided to inform of local variations in
resonance frequency with respect to the main field (B0 inhomogeneity, chemical
shift), it was subject to breathing artefacts and its spectral resolution was insufficient
for fatty tissues. A custom-made breath-hold f0 sequence was
therefore inserted instead. Three pulses were then compared: standard circularly
polarised (CP) mode (“TrueForm C”), manufacturer subject-tailored RF-shimming
(so called “Volume-selective“), and kT-points. A 7° flip angle was
targeted and each pulse was incorporated in a “dynamic enhancement” 3D GRE
T1-weighted-like sequence performed in a single breath-hold, before contrast
agent injection. Acquisition parameters were: 320x220x72 matrix, 1.1x1.1x3mm3
resolution, TE/TR= 3/6ms, iPAT factor 2, 80%/50% phase/slice resolution, TA=
23s). The 7° 7-kT-point pulse was designed using
MATLAB’s (The Mathworks, Natick, MA, USA) built-in active-set algorithm; flip
angles were evaluated by numerical Bloch integration. The number of kT-points
was chosen to be seven to allow as many degrees of freedom as possible while
maintaining a reasonably short pulse duration.
Flip angle NRMSE (normalised root-mean-square error from the target over
the volume of interest) was minimised by optimising simultaneously RF complex
coefficients, kT-points locations and durations under SAR and
hardware constraints.10,11 Taking advantage of general-purpose GPU
computing allowed to design the pulse in less than one minute. Results
Axial views
of the T1w acquisitions are shown in Figure 1: results were compared between the
three transmit modes. Pre-acquisition normalisation was performed to eliminate
reception profiles as much as possible. The characteristic shading due to
dielectric resonance has almost disappeared on the kT-points images,
while it was still present with tailored RF-shimming. Anatomical structures inside
and near the liver, such as the aorta, the portal system and the gallbladder, are
also much better resolved. These results are confirmed in Figure 2, where one
can see that kT-points achieve homogenisation not only in the
presented slices, but in the whole volume. For instance, artefacts are greatly
reduced in the left lobe of the liver below the heart, as well as in the hepatic dome. Characteristics of the
three pulses used are gathered in Table 1. Conclusion
Excitation
homogenisation in the abdomen is necessary to ensure reliable diagnostic in the
liver at 3T. These preliminary results highlight the fact that tailored static
RF-shimming is not satisfactory enough to justify the use of two-channel pTX.
The kT-points technique, on the other hand, fully embraces pTX capabilities and
allows better SNR and contrast recovery than RF-shimming, thus an increased
diagnostic power in the liver. This is achieved with a controlled SAR, and requires
less than one minute of computation time. A study is currently being done to analyse
the robustness of the approach. In the near future, we plan to extend this
method to slab-selective excitation and fat-saturation pulses. Acknowledgements
The authors wish to thank all the MRI
technicians of Henri Mondor Hospital for their patience, understanding and helpful
clinical advices. This project was funded by CEA’s Programme Transversal, Technologies pour la
Santé (Transversal Programme for Health Technologies). References
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