Sander Brinkhof1, Aidin Ali Haghnejad2, Keita Ito3,4, Karin Markenroth Bloch5, and Dennis Klomp1
1Radiology, University Medical Center Utrecht, Utrecht, Netherlands, 2WaveTronica, Utrecht, Netherlands, 3Biomedical Engineering, Eindhoven University of Technology, Eindhoven, Netherlands, 4Orthopaedics, University Medical Center Utrecht, Utrecht, Netherlands, 5BioImaging Center, Lund University, Lund, Sweden
Synopsis
The
goal of this work is to implement a dual tuned sodium-proton coil as
transceiver for sodium and transmitter for hydrogen with a high-density proton receive
array and compare the proton imaging performance with a state-of-the-art single
tuned knee coil. A double-tuned knee
coil was constructed as a shielded birdcage and 15 channel proton receiver coil
embedded within the double-resonant birdcage. The double-tuned coil was implemented
with comparable proton quality and acceleration possibilities compared to the single-tuned
alternative while also being able to acquire high SNR sodium images.
INTRODUCTION
Cartilage
degeneration is characterized by loss of glycosaminoglycans (GAG) on the
surface of the cartilage. This GAG loss can be quantified by using sodium MRI
due to its direct relation with GAG content 1,2. Sodium imaging requires double tuned RF coils,
but the proton image quality of such coils is often severely compromised.
Reasons for this is that the number of proton receive channels are often
severely reduced and that double tuning may degrade the intrinsic sensitivity
of the RF coil. However, when incorporating an array of single tuned 1H coils
inside a volume sodium transceiver, proton imaging performance may remain
intact. Therefore the goal of this work is to implement a dual tuned
sodium-proton coil as transceiver for sodium and transmitter for hydrogen with
a high-density proton receive array and compare the proton imaging performance
with a state-of-the-art single tuned knee coil. METHODS
A
double-tuned knee coil was constructed as a shielded birdcage (12 rods with a
length of 15 cm) and 15 channel proton receiver coil embedded within the
double-resonant birdcage. The 1H transmit and receive coils could be actively
detuned using standard PIN diode circuitry. The fifteen overlapping proton
receive elements were each 5 cm width and 9.5 cm in length and connected to low
impedance preamplifiers used for preamplifier decoupling and signal
amplification before interfacing to the 7T MRI system (Achieva; Philips
Healtcare, Best, Netherlands).
To validate the efficiency of the proton coil, our double tuned (DT) coil was
compared with a vendor-built single tuned (ST) alternative (28 channel receive;
Quality Electrodynamics LLC, Ohio, USA). SNR, g-factor acceleration maps and
B1+ measurements were carried out in the DT coil (4 volunteers) and ST coil (8
volunteers) after informed consent was signed. SNR maps were constructed from
noise scans, whereas the signal maps were corrected for B1+ performance by
normalizing with the B1+ maps. G-factor maps were reconstructed to analyze the
acceleration possibilities in both coils. RESULTS
G-factor maps were reconstructed with SENSE acceleration
factors of up to three in both directions (AP and RL). Figure 1 shows the axial
g-factor maps of our DT coil, which indicated that a SENSE acceleration of 9 was
feasible in this coil (AP = 3, RL = 3, maximum g-factor 1.9). Figure 2 shows
the same axial g-factor maps, acquired with the ST coil where the g-factor maps
had a similar hotspot at SENSE acceleration of 9, with a maximum g-factor of
2.2. Figure 3 shows a typical axial and sagittal slice for each coil with
corresponding g-factor maps (with SENSE AP = 3, RL = 3).
SNR maps are shown in figure 4 for our DT coil and the ST coil,
indicating that both had similar SNR. The SNR maps were corrected for B1+
performance, hence reflecting intrinsic coil sensitivity. Average SNR in the
trochlear cartilage was 26.6 in the DT coil (standard deviation = 4.1, N = 4)
and 28.3 in the ST coil (standard deviation 1.6, N = 8). Figure 5 shows a
sodium scan from the DT coil overlaid on a proton density weighed anatomical
scan. DISCUSSION / CONCLUSION
The g-factor maps of the DT coil showed that its having the
same acceleration possibilities compared to the ST coil, both coils lost some performance
with acceleration factor of 9 (AP = 3, RL=3, g-factor > 2). The patterns
within the g-factor maps showed some differences, which could be attributed to
the differences in receive array designs.
The SNR maps did not show substantial differences,
indicating that the proton performance was not hampered by the addition of a
sodium receive/transmit coil. This is underlined by figure 5, showing that we
achieved high SNR sodium images while maintaining good quality proton scans.
The addition of a sodium transmit and receive coil is
beneficial because both nuclei can be scanned in the same session, without changing
coils. By implementing an interleaved scanning protocol,
sodium and proton scans can be acquired at the same time to be even more time
efficient 3.
In conclusion, a DT coil was implemented with comparable
proton quality compared to the state-of-the-art ST alternative while also being
able to acquire high SNR sodium images. Acknowledgements
No acknowledgement found.References
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