Lucia Navarro de Lara1,2, Padmavathi Sundaram 1,2, Lena Nohava3, Elmar Laistler3, Mohammad Daneshzand1,2, Lawrence Wald1,2, Jason Stockmann1,2, and Aapo Nummenmaa1,2
1Martinos Center - MGH, Charlestown, MA, United States, 2Harvard Medical School, Boston, MA, United States, 3High Field MR Center, Center for Medical Physics and Biomedical Engineering, Medical University of Vienna, Vienna, Austria
Synopsis
To enable concurrent non-invasive stimulation (TMS) and
whole-head multimodal imaging (EEG-fMRI), we propose to apply flexible RF
coil technology to build a first-of-its-kind TMS compatible integrated multimodal imaging
array, the “RF-EEG cap”. The proposed system allows unrestricted positioning of
the TMS coil across the entire scalp. We built a 2-channel prototype and
conducted a feasibility study analyzing the effects of a TMS coil and EEG-electrodes
on the imaging quality (SNR/B0 maps), the in-bore EEG data quality and EPI
timeseries stability. Our results indicate that the flexible
coaxial RF technology is a feasible choice to build the proposed “RF-EEG Cap”.
Introduction
There is
mounting evidence that the effects of TMS and its therapeutic efficacy depend
on the primary stimulation target region as well as its connectivity pattern (spatial
dependency)1,2. Additionally, the neuromodulation effects depend
on the brain state at the time of stimulation (time dependency)3 defined
by neural oscillations. Combining TMS/fMRI/EEG offers the next-generation capabilities for causal-functional mapping
of the human brain circuits in a non-invasive way with unprecedented spatial
and temporal resolution potentially enhancing therapeutic protocols through
closed-loop applications. However, the triple combination presents
technological challenges especially due to the lack of dedicated hardware to
allow optimal performance of TMS and MRI (see Fig.1 column 1-4).
Feasibility
of concurrent human TMS/EEG/fMRI measurements at 3T has been recently
demonstrated4,5.
However, the presented data were acquired either with the body coil (extremely low-sensitivity)
or a birdcage coil (Fig.1 column 2). Moreover, no parallel
imaging acquisition methods6,7,8
were used due to the lack of multichannel RF-coils, limiting the spatiotemporal
resolution of the acquisition. Nevertheless, these results rigorously
demonstrate the basic feasibility and safety of the technology.
Our
overarching goal is to build the first-of-its-kind wearable “RF-EEG Cap” to
allow full-head coverage concurrent TMS/fMRI/EEG acquisition (Fig.1,
column 5, Fig.2A and 2B). Here, to assess the feasibility of the
proposed “RF-EEG Cap” we have constructed a 2-channel prototype shown in Fig.2C.
Methods
For the prototype
construction we implemented flexible coaxial RF elements9,10 easily
attachable to soft materials. We built two 8cm diameter coils using flexible coaxial
cable (Molex 047SC-2901, IL, USA) following proposed tuning/matching circutry11
(see Fig.2D). Active detuning and preamplifier decoupling were implemented.
Both elements were sewn onto a cloth cap and connected through 22.5 cm coaxial
cables to an interface box containing one 3T preamplifier (Siemens, Germany)
and a 3T Skyra plug. Placeholders for EEG-electrodes in the middle of each
element were made on the cap to facilitate the positioning.
The prototype
was tested on the Bench using a VNA (Keysight Technologies, CA, USA) as: (i)
stand-alone (only having RF elements), referred as RF-Cap; (ii) placing two
bipolar MR compatible EEG-electrodes (Brain Products GmbH, Germany), referred
as RF-EEG
Cap and (iii)
placing the EEG-electrodes and the MRi B91 TMS coil (MagVenture, Denmark) over
the cap, referred as RF-EEG Cap+TMS.
To evaluate the
effects on the imaging of the two additional modalities, we acquired SNR maps (FOV=256
mm, 1 slice, FA = 30, TR= 9.1 ms, TE=4.8 ms, SL= 2mm, 1 mm in-plane) and B0
maps (FOV=220mm, 18 slices, FA=75, TR=300ms, TE1=5ms, TE2=7.46ms, SL=5mm, 2.2mm
in-plane) which were processed with in-house MATLAB scripts for visualization.
Additionally,
to assess the feasibility of using the proposed technology to acquire high
quality EEG data and functional imaging, we conducted a concurrent TMS/EEG/fMRI
experiment using a phantom. To produce synthetic EEG data, the phantom’s head
was covered with a cloth immersed in a 9% NaCl solution with the 2-channel “RF-EEG
Cap” placed above it. The cloth was connected to a signal generator outside
the scanner delivering a 5.1Hz square signal at 20mVpp (see Fig.5A).
TMS pulses were delivered as indicated by the dots in the TMS “ON” block shown
in the timeseries of Fig.5C, at 50% maximum stimulation output.
Functional imaging (SL=3mm, TR=1000ms, TE=37ms, FA,90, 6slices, 2.4mmx2.4mm
in-plane) was interleaved with the TMS pulses that were delivered just before
the acquisition of the 5th slice (650ms after a volume starts). EEG
data was recorded using the BrainAmp ExG MR 16 (Brain Products GmbH, Germany)
and processed using EEGLab software package12,13.Results
The Qu/Ql of the RF coil elements were 2.24 and 2.19. Bench
test results for each condition are shown in Fig.3A and Fig.3B. A
summary of the main effects on the S-parameters when adding the different
modalities is shown in Fig.3C.
SNR maps of the 2-channel
“RF-EEG Cap” as stand-alone, without EEG-electrodes and TMS are shown in Fig.4A-Top.
The relative SNR is shown for the case when the EEG-electrodes or the TMS
(placed over the left hemisphere of the phantom) are included. When the EEG-electrodes
are placed, no significant SNR change was observed over the region with
sufficient SNR. In contrast, when the TMS coil was placed over the phantom, the
well-known characterized B+1 effect of TMS14
can be observed. No additional SNR changes are expected due to the presented
technology. Sagittal B0 maps directly over the EEG-electrodes are shown in Fig.4B.
No significant effects on the phantom brain due to the EEG-electrodes are
visible.
The results of the quality
analysis of the acquired EEG and fMRI data are presented in Fig.5B and Fig.5C
respectively. The TMS pulses and EEG acquisition did not affect the fMRI image
quality as shown in the timeseries. Discussion
From the findings presented
above we conclude that the flexible coaxial RF technology is a feasible choice to build the proposed “RF-EEG Cap”. The shifting effect on the
resonance when placing the TMS over them was reported to be less than 0.4MHz
compared to 4-5MHz when using standard copper wire coils15. The
minimal effects observed on the SNR, B0 maps, EEG quality signal and fMRI
volumes and timeseries justify the further development of the “RF-EEG Cap” to
enable high quality data acquisition for concurrent TMS/EEG/fMRI experiments. Acknowledgements
This work was funded by NIH
R00EB015445, R01MH111829, NIH R00EB021349 and the Rappaport Foundation. References
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