Maxim Terekhov1, Ibrahim A. Elabyad1, and Laura M. Schreiber1
1Chair of Cellular and Molecular Imaging, Comprehensive Heart Failure Center, University Hospital Würzburg, Wuerzburg, Germany
Synopsis
Cardiovascular
MRI at the ultra-high-field is an
emerging modality promising a significant increase of the spatial resolution
and physical sensitivity of routine cardiac imaging. Pig models play an important
role in the establishment and translation of 7T cMRI to humans. The
prerequisite for high-quality 7T cMRI data
in pigs is dedicated transceiver arrays adapted to the shape of the pig’s thorax.
We validated the proof-of-concept of the transceiver pTX cardiac array with adjustable
parabolic shape housing for longitudinal studies with pigs. The stability of
the transmit and receive characteristics by shape adjustments are tested
in-silico and in phantom measurements.
Introduction
Cardiovascular
MRI (cMRI) at ultra-high field is an emerging modality promising a significant
increase in the spatial resolution and physical sensitivity of routine cardiac
imaging. Using multiple-element transceiver arrays with parallel transmit (pTX)
support allows overcoming the problem of destructive interferences of B1+-field
in the thorax caused by dielectric resonances [1,2]. Porcine models play an important
role in the establishment and translation of the 7T
cMRI techniques to humans. The prerequisite of high-quality 7T porcine cMRI
is the adaptation of the array to the shape of the pig’s thorax [3,4]. In longitudinal
studies with a duration of several weeks or months, the upper range of the
animal’s weight and, therefore, thorax dimensions are difficult to estimate. We present the proof of concept of the array
for cMRI in pigs up to 100 kg weight with an adjustable parabolic shape. The work aimed to ensure the stability of the
transmit and receive characteristics of the 8Tx/16Rx array while the shape is
being accommodated to the growing dimensions of the animal thorax. Materials and Methods
Electromagnetic
simulations of the 16-element transceiver array were done using
CST-Microwave-Studio. For matching and
tuning the RF-circuit co-simulation was employed in CST-Design-Studio (CST-DS).
The adjustable array shapes were described by the cylindrical paraboloid
surfaces. The steepness of the parabolas was adjusted to fit the thorax of the
pig in a range of 60 to 100 kg based on the MR-images of the real pig thorax
(Figure 1a,b). Three array shapes (S1, S2, S3)
were simulated to check the variation of the B1+-field profile while adjusting
the housing to the pig thorax. The computation of the hardware-integrated
driving phases of elements providing optimized default B1+ profile for single-Tx
mode was performed using the multi-start approach [3], genetic algorithm
(Matlab Global Optimization Toolbox), and basin-hopping solver (SciPy
Python package). The phase vector optimized for the shape S2 was
used to check the B1+-profile for all 3 shapes.
Experimental testing
of the adjustable parabolic shape array concept and its influence on the array
characteristics was done using the prototype of the 8Tx/16Rx array with
antisymmetric L-shaped elements [3] printed on the flexible substrate (Figure
1c). To make the array compatible with the pTx system, every two neighboring
elements are interfaced to one Tx-channel. The adjustment of the array shape was
done for 3 positions gradually increasing the distance between bottom margins.
The MRI measurements with the array loaded by a pig body phantom were performed
on a 7T whole-body MAGNETOM™ Siemens Terra scanner. For each array shape the
measurements of the absolute B1+-maps, relative B1+-maps of individual
Tx-channels, g-factor, and noise correlation matrix was done. The reference
voltage for 1ms 180◦ pulse
was determined by a vendor-integrated routine for each array shape. Relative
B1+-maps were used for the B1-shimming in the pTX mode performed off-line using an
in-house designed Matlab toolbox. Results
Figure 2
demonstrates the variation of the B1+ maps in the central transversal slice for
three array shapes using three different optimized phase vectors for elements
driving voltages. Figure 3(a) shows the absolute B1+ map measured by
vendor-integrated protocol. Figure 3(b,c) shows the sum-of-magnitudes (SoM) of
the relative SNR maps of the individual transmit channels. Figure 4
demonstrates the result of the pTX-based B1-shimming for all three array
shapes. Finally, Figure 5 shows the effect of the array shape on the g-factor and
noise correlation matrices. Discussion
The results
of EM-simulation demonstrate that an optimized B1+-profile remains relatively stable
while array shape changes through all three considered variants. The B1+-profiles formed by the same optimized phase vector for all three simulated
shapes show a similar coefficient of variation and mean B1+. This should allow
using shape adjustment once an array hardware phasing is pre-optimized for the single
Tx-mode [5]. This finding also agrees with the stability of the absolute B1-map
measured with the experimental setup (Figure 3a). The increased array flatness for
shape S3 leads to an insignificant increase of the reference voltage
(on 10%) compared to shape S1. The sum-of-magnitude SNR maps of individual Tx
channels show that variation of the shape may have an essential effect on the
performance of the array in the periphery of the thorax. In theory, however,
the peak SNR remains stable in the central region of the thorax phantom
corresponding to the animal heart position. The results of pTX-based
B1-shimming demonstrate that even with the different initial states a very
close coefficient of variation of the SNR in the targeted region can be shaped by
pTX-B1-shimming for all three arrays shapes. Finally, g-factor mapping
demonstrates full stability of the mean value in the region of the pig heart
for all the tested array shapes. Conclusion
Both
simulated and prototype versions of the array for cMRI with parabolic shape
demonstrated steadiness of the most essential transmit and receive
characteristic while the array’s shape is adjusted within a chosen range of
inner dimensions. The final validation will be performed in the longitudinal
in-vivo measurements with the maximal weight of the animals up to 100 kg. Acknowledgements
Financial support: German Ministry of Education and
Research (BMBF, grants: 01EO1004, 01E1O1504).References
[1] Kraff O,
Quick HH. Radiofrequency Coils for 7 Tesla MRI. Top Magn Reson Imaging. 2019
Jun;28(3):145-158. doi: 10.1097/RMR.0000000000000206. PMID: 31188273.
[2] Niendorf,
T., Paul, K., Oezerdem, C., Graessl, A., Klix, S., Huelnhagen, T., Hezel, F.,
Rieger, J., Waiczies, H., Frahm, J., Nagel, A.M., Oberacker, E., Winter, L.,
2016. W(h)ither human cardiac and body magnetic resonance at ultrahigh fields?
technical advances, practical considerations, applications, and clinical
opportunities. NMR in Biomedicine 29, 1173–1197.
[3] Elabyad
IA, Terekhov M, Stefanescu MR, Lohr D, Fischer M, Schreiber LM. Design
of a novel antisymmetric coil array for parallel transmit cardiac MRI in pigs
at 7 T. J Magn Reson. 2019 Aug;305:195-208.
[4] Elabyad IA, Terekhov M, Lohr D, Stefanescu MR,
Baltes S, Schreiber LM. A Novel Mono-surface Antisymmetric 8Tx/16Rx Coil Array
for Parallel Transmit Cardiac MRI in Pigs at 7T. Scientific Reports.
2020;10(1):3117
[5] Terekhov M, Elabyad IA, Schreiber LM (2021) Global
optimization of default phases for parallel transmit coils for ultra-high-field
cardiac MRI. PLoS ONE 16(8): e0255341.