Pu-Yeh Wu1, Ying-Hua Chu1, Aapo Nummenmaa2, Thomas Witzel2, Shang-Yueh Tsai3, Wen-Jui Kuo4, and Fa-Hsuan Lin1
1Institute of Biomedical Engineering, National Taiwan University, Taipei, Taiwan, 2Athinoula A. Martinos Center for Biomedical Imaging, Massachusetts General Hospital, Charlestown, MA, United States, 3Institute of Applied Physics, National Chengchi University, Taipei, Taiwan, 4Institute of Neuroscience, National Yang Ming University, Taipei, Taiwan
Synopsis
We tested how TMS pulses and the
separation between TMS pulse and RF excitation affect MRI SNR and tSNR using
our tailored 8-channel TMS-compatible MRI coil array. Result from an in vivo
experiment using this integrated system to record the BOLD signal elicited by
TMS pulses at human primary motor cortex is also reported.Purpose
Transcranial
magnetic stimulation (TMS) uses transient and strong magnetic fields to elicit
neuronal activity non-invasively 1. Combining TMS with fMRI provides
the unique opportunity to not only observe but also manipulate brain responses.
Different from TMS-EEG, TMS-fMRI holds the promise of detecting deep brain
responses to exogenous magnetic field stimulation.
Here we report our recent advance in TMS-fMRI
technical development. Specifically, we tested how TMS pulses and the
separation between TMS pulse and RF excitation affect MRI SNR and time-domain
SNR (tSNR) using our tailored 8-channel TMS-compatible MRI coil array 2.
Results from an in vivo experiment using this integrated system to
record the BOLD signal elicited by TMS pulses at human primary motor cortex is
also reported. Taken together, our TMS-compatible MRI coil array can be a
valuable tool in studying the immediate hemodynamic responses to TMS with high
sensitivity.
Methods
An
8-channel surface coil array was designed and tested on a 3T MR system (Skyra,
Siemens). All loop coils (center coil diamter = 9 cm, side coils diameter = 7
cm) were tuned to 123.25 MHz and connected to a low noise pre-amplifier (LNA)
integrated with a mixer through a coaxial cable and a matching circuit,
which transformed the impedance to 50 Ω in order to obtain the lowest noise
figure. An active detuning circuit was formed using a variable inductor and a
PIN diode. To minimize the coil array thickness for the maximal TMS stimulation
efficacy, the coil inductor loops was formed by copper foil tape. The matching
circuit and LNA were extended outside the coil loops through coaxial cables
with 10-20 cm in length. Coil loops were hexagonally arranged on the mechanical
housing (Fortus, 400mc) fitting to the TMS coil (MRI-B91, MagVenture). A hole
in the center of coil array was designed to minimize the distance between the
tangential plane of the head and the TMS coil to less than one millimeter. To
mutually decouple between neighboring coils in the array, coils were critically
overlapped. We first tested how
MRI quality was affected by the presence of the TMS coil. Subsequently, we evaluated
how TMS pulses modulated MRI quality. Both experiments used an EPI pulse
sequence (FoV: 224x224 mm, Resolution: 3.5 mm isotropic, TR: 2000 ms, TE: 30
ms, Flip angle: 90
o). Two delays were added between consecutive EPI
acquisitions. Type 1 had a delay of 1 s, including 0.7 s TMS pulses and 0.3 s
silence; Type 2 had a delay of 0.75 s, including 0.7 s TMS pulses and 0.05 s
silence (Figure 1B). One subject participated the in vivo experiment. We compared the SNR and tSNR maps using data
acquired from our coil array and a commercial 32-channel whole-head array. TMS
stimulation (110% of the subject’s motor threshold) at the human left M1 was
delivered to the subject inside MRI using a blocked design (5 “on” and 5 “off”
30 s blocks). BOLD activities were estimated using the General Linear Model.
Results
Figure
1A shows SNR and tSNR maps using a commercial 32-channel whole-head array and our
8-channel TMS-compatible array. Both showed higher sensitivity at the bottom of
the phantom. Note that the phantom sat directly on top of our 8-channel array. Figure
1C shows the SNR and tSNR profiles acquired from the middle line (white dash
line) of all images. The improved SNR and tSNR by our array was found
significant at depth no farther than 4 cm. With the TMS coil combination, both
SNR and tSNR maps changed minimally. There was no visible distinction in SNR
and tSNR maps between delivering TMS pulses (both type 1 and type 2) and
delivering no TMS pulse. Figure 2 shows the experimental setup and the SNR as
well as tSNR maps at an axial slice passing through the primary sensorimotor
cortex. We found significant BOLD signal at the left hemisphere primary
sensorimotor area, whose hemodynamic response shows good agreement with the
expected fluctuation due to blocks of TMS pulse delivery (Figure 3).
Discussion
Our preliminary results successfully
demonstrate that our TMS-compatible MRI coil caused neither visible image
distortion nor SNR and tSNR degradation. The temporal separation between TMS
pulses and the onset of EPI acquisition can be as short as 50 ms without clear
effects. This suggests that the delivery of TMS pulses can be tightly packed
between silent intervals of MRI acquisition. Further experiments at other
functional areas, such as visual cortex, will be attempted to investigate the
brain activity due to phosphene induced by TMS.
Acknowledgements
This study was supported by Ministry
of Science and Technology, Taiwan (MOST 104-2314-B-002-238, MOST
103-2628-B-002-002-MY3), National Health Research Institute, Taiwan
(NHRI-EX104-10247EI), and Ministry of Economic Affairs, Taiwan
(100-EC-17-A-19-S1-175).References
1. Barker AT, Jalinous R, Freeston IL.
Non-invasive magnetic stimulation of the human motor cortex. Lancet. 1985;
1(8437):1106-1107.
2. Wu PY, Chu YH, Nummenmaa A, et al. A
10-channel TMS-compatible planar RF coil array for human brain MRI at 3T. ISMRM 23rd Annual
Meeting. 2015; #4590.