Natalia Gudino1, Jacco A de Zwart1, Qi Duan1, Peter van Gelderen1, and Duyn Jeff H1
1Advanced MRI section, LFMI, NINDS, National Institutes of Health, Bethesda, MD, United States
Synopsis
We demonstrate a new on-coil current-source switch-mode
amplifier and communication setup for 7T imaging, which allows monitoring of
the RF phase, frequency and amplitude at the amplifier output. This information
is made available through a single optical signal per amplifier, making it a
practical approach for safety monitoring and fast calibration of on-coil
amplifier technology for parallel RF transmission.Purpose
Monitoring of the RF excitation allows compensation of
B1 field errors, power
estimation and detection of potential hardware failures that could compromise patient
safety [1-4]. Using the integrated current sensor in a current-source
switch-mode on-coil amplifier [5,6],
B1
amplitude and phase information can be recovered on the basis of three optical
signals (one voltage for amplitude and two optical quadrature voltages for phase
detection) [7]. We propose an improved amplifier design where amplitude, phase
and frequency information are recovered in a remote controller from a single
optical digital down-converted version of the sensed RF current. This prototype
is a first step toward a practical implementation of real-time optical
monitoring of the
B1 field per channel to ensure safe operation of a
pTx system employing on-coil current source amplification.
Methods
An overview of our implementation of on-coil amplification
for RF transmission is show in
Figure 1, highlighting the main aspects
B1
monitoring and integration with the MRI scanner. The on-coil current source
amplifier has a loop integrated in an inner layer of the printed circuit board to
sense output current [6]. Feedback of the detected current envelope is
performed on the board to minimize load sensitivity [5,6]. In this new prototype,
before envelope detection, the sensed current was split through a LC 2-way
splitter to send part of the signal to an active mixer (AD8342) with local
oscillator (LO) input of 297.0 MHz, 200 kHz away from the scanner frequency
(297.2 MHz). An optical receiver and fanout buffer (output skew < 50 ps), located
next to the amplifier board, generated multiple LO signals from a single
optically received LO for future multi-channel implementation. After low-pass
filtering, the output of the RF mixer (IF) was converted to 10-bit serial digital
signal through a low power analog-to-digital converter (ADC AD7277) clocked at
25 MHz (optically transmitted and buffered on the amplifier side as all control
signals). This digital signal was then optically transmitted to a remote
computer that hosts the PCI board that controls the vector modulators in the custom-made
pTx interface [6]. This interface generates multiple optical carriers and
envelope signals from the single RF pulse transmitted by the scanner control to
drive multiple on-coil switch-mode amplifiers[6]. In the current implementation,
digital optical communication from the amplifier to the remote computer was
possible through a remote optical receiver connected to a commercial adapter
board (Nano River Technologies, Denmark) that converted 3-wire serial
peripheral interface (SPI) to full speed universal serial bus protocol (USB2). In
a benchtop demonstration, preliminary data was obtained with a single amplifier
connected to a 6 cm diameter transmit coil. B1
field was measured with a calibrated probe coupled to the coil, and the down
converted sensed signal was simultaneously measured with an oscilloscope probe
at the input of the ADC (located on the amplifier), and monitored on the
computer screen after down-converted RF waveform reconstruction was preformed in
software.
Results
Figure 2 shows the RF output measured with
the calibrated probe on the coil side (B1 = 25 µT at the center of
the coil), the corresponding down converted signal at the input of the ADC and
the signal remotely recovered at the controller side. We can see that the
down-converted signal tracked accurately the B1 field measured with the probe and was successfully
recovered on the remote computer. The modulation on the recovered amplitude is
caused from the implemented sampling rate (~781k Hz).
Figure 3 shows the recovered RF spectrum (for four iterations) while
the RF carrier frequency of a sine pulse transmitted from the pTx interface to
the amplifier was changed from 297.175 MHz to 297.225 MHz. The monitored down
converted frequencies, indicated with different colors, were from 175 kHz to 225
kHz.
Discussion
We have presented preliminary data with a new on-coil
amplifier prototype that performs down conversion and digital optical
transmission of the sensed RF signal. The amplifier size and performance compared
to a previous prototype [6] was not affected by the additional electronics. We successfully
recovered the signal in a remote computer that hosts the pTx interface controlling
the on-coil amplifiers. In addition to safety monitoring, phase and amplitude
information carried in the recovered signal could be processed for automatic
adjustments of the control inputs of the vector modulators located in the pTx
interface [6]. This closed loop operation will allow fast and simple initial
system calibration.
Acknowledgements
This research was supported by the Intramural Research
Program of the National Institute of Neurological Disorders and Stroke.References
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