Junghwan Kim1,2, Changyu Sun1,3, Chan-Hong Moon4, Hoby Hetherington1,5, and Jullie Pan1
1Radiology, University of Missouri, Columbia, MO, United States, 2EECS, University of Missouri, Columbia, MO, United States, 3BBCE, University of Missouri, Columbia, MO, United States, 4Radiology, University of Pittsburgh, Pittsburgh, PA, United States, 5Resonance Research Inc., Billerica, MA, United States
Synopsis
Keywords: High-Field MRI, RF Arrays & Systems, Rx array
While the Tx performance of the 8x2 transceiver has been shown to
achieve excellent amplitude and homogeneity, with its limited coil numbers
(16), it is thought to give substantially lower SNR and acceleration in
comparison to conventional arrays (8Tx/32Rx). It is recognized however, that the
Tx decoupling is also constructive for Rx since the SNR and g-factors benefit
from the decreased noise correlation. We evaluated the SNR, g factors, and
noise covariance and found that up to an in-plane acceleration value of
approximately <=4, the transceiver gives comparable performance to a
commercial reference coil.
Introduction
The 8x2 decoupled transceiver array has been shown1,2 to provide
excellent RF transmission characteristics for amplitude and homogeneity at 7T. This
array uses RID and TD circuits1-3 to achieve coupling values of <-20dB. However,
it has been perceived that the transceiver array does not provide sufficient
SNR with high acceleration because of the fewer Rx elements compared to
conventional 32 Rx-only arrays. It
should be recognized however that to minimize coupling, traditional receive
only arrays use preamplifier decoupling and coil overlap, while the transceiver
obviously has substantially lower coupling which is important for minimizing noise
correlations. To understand the impact of improved decoupling for Rx
performance, we evaluated the noise covariance, g-factor map, SNR and
compared it to the commercial reference 8Tx/32Rx RF coil (Nova Medical, Wilmington, MA). In
vivo turbo spin echo TSE images were also acquired and compared.Methods
A whole body 7T MRI (Terra, Siemens
Healthineers, Erlangen, Germany) was used. To measure the array performance, multi-slice
2D-GRE images were acquired with TR/TE=10sec/3.8msec, FA=30º, slice thickness 3mm,
matrix 64x64, FOV 220x220mm2. The noise covariance was calculated
from the prescan data. To assess the decoupling effectiveness, the mean and SD
of the noise correlations between all coil loops were calculated. Given that
there is commonly poorer decoupling between adjacent and second neighboring
loops, the mean and SD of the noise correlations at these locations were also calculated.
g-maps were calculated using a SENSE reconstruction4. The SNR map was calculated using SENSE SNR5 . For the SNR evaluation, Coefficient of
Variation (CoV) of SNR within/between slices were calculated. High resolution
TSE imaging at R=3 (TR/TE=4sec/55msec, FA=128º, thickness=3mm, in-plane res.=
0.2mm2, TA=4min., n=5 subjects) demonstrate the overall performance. Results
Noise Covariance: The transceiver array measured mean correlation of 10±5% for all channels and 11±6% for the 1st&2nd neighboring loops whereas 12±9% and 30±14% was measured in the reference coil respectively (Fig. 1).
G maps: The average g for the transceiver array was similar to the reference coil with the max g at 9% higher in transceiver array (Fig. 2 and Table 1A).
SNR and B1+: The average SNR variation within the slice was higher in transceiver (CoV per slice = 0.49 vs 0.43, Fig. 3 and Table 1B) whereas the average SNR variation between slices was higher in the reference coil (0.17 vs 0.25, Fig. 3). Nonetheless, over the entire brain, there was no major difference in SNR (65 vs 67, Table 1B). For the B1+ performance, target FA@30°, the mean B1+ [degree] and CoV over the entire volume measured 29±5° vs 25±5° and 14±1% vs 20±2% (transceiver vs reference coil).
In vivo TSE imaging (R=3): High resolution T2W TSE imaging demonstrates that the transceiver array shows higher SNR in the low-mid brain area (yellow, Fig. 4). In the row-row gap region where no coil is present, a SNR drop was seen, substantially over the extracranial regions (red, Fig. 4). For superior brain areas, the SNR was similar.Discussion
With the
decoupling generated through reduction of the “true” mutual impedance in the
transceiver, the noise covariance is significantly lower than the reference coil (Fig. 1). As calculated from the sensitivities and noise covariances, Fig. 2
compares the g-maps for R=2, 3, 4, 2x2, and 3x2 for the two coils. At R=4, the transceiver array calculated $$$ {SNR_p^{full}}/{SNR_p^{red}}=g_p\sqrt{R}=2.48 $$$ while reference coil calculated 2.40 respectively;
for R=3x2, the estimated average SNR drop for transceiver and reference
arrays were 2.65 and 2.62. These g-maps are
consistent with the notion that the low noise covariance and high sensitivity
lift the performance of the transceiver in spite of half the receive coil
numbers than the reference array.
A direct
comparison of non-accelerated SNR (Fig. 3) shows that in the superior slices,
the transceiver exhibits lower SNR centrally but higher SNR peripherally
compared to the reference array, this being consistent with the ultimate
intrinsic SNR analysis6. However in the more inferior slices, this
central-peripheral SNR difference is less. Overall, the transceiver exhibits a
larger SD of the SNR compared to the reference coil, 33 vs. 27 although the
absolute average SNR was not significantly different, at 65±33 and 67±28 for
the transceiver and reference coil respectively. With better B1+ performance1 and comparable g maps, comparison of in vivo
TSE images (R=3) between the two arrays show the characteristics of the
transceiver array: inferior brain regions with higher SNR (yellow, Fig. 4), inter-row
slices with decreased SNR that is substantially extracranial (red, Fig. 4) and
the remaining superior brain slices with similar SNR.Conclusion
We
have evaluated receive characteristics and SNR of the transceiver array. In
comparison with the commercial reference coil, the transceiver performs
similarly in overall SNR and with the improved decoupling (despite 50% fewer Rx coils), the g maps are also comparable. With superior B1+
homogeneity (14% v 20%) and greater coverage in the head to foot direction,
sequences utilizing spin echo acquisitions (which have enhanced pulse angle
dependence) will show significantly improved image quality in inferior brain
structures. For TSE images, contrast is better preserved and SNR is enhanced in
the temporal lobe and cerebellum with the transceiver array in comparison to
the reference coil.Acknowledgements
The authors are grateful to Bernd Stoeckel and John Grinstead from Siemens Healthineers (Siemens Healthcare, Erlangen, Germany) for the technical support and discussions. This work is supported by the National Institute of Health [R01-EB0244408]
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