Geon-Ho Jahng1, Jeonin Jeong2, Mun Bae Lee3, Jiyoon Lee2, and Oh In Kwon3
1Radiology, Kyung Hee University Hospital at Gangdong, Seoul, Korea, Republic of, 2Biomedical Engineering, Kyung Hee University, Yongin-si, Korea, Republic of, 3Mathematics, Konkuk University, Seoul, Korea, Republic of
Synopsis
Keywords: Electromagnetic Tissue Properties, fMRI
To investigate the neuronal response of
conductivity during visual stimulation and compare that with BOLD, 30
young healthy volunteers were recruited from the local
community. We performed two independent experiments of functional magnetic resonance electrical properties tomography (MREPT)
MRI. We found that the conductivity value was increased during visual stimulation
to some brain areas, indicating that functional MREPT
MRI can be used to measure neuronal activity; therefore, conductivity-based
fMRI signals may be helpful for measuring neuronal activation during
stimulation.
Introduction
Because blood oxygen level-dependent (BOLD)
functional MRI (fMRI) signals depend
on cerebral blood flow (CBF), cerebral blood
volume (CBV), and oxygen consumption rate
(CMRO2) altered by local
electric synaptic activity (1,2), magnetic
resonance electrical properties tomography (MREPT)-based fMRI signals may provide additional
information about electric activity caused by alteration of ion concentrations
and mobilities (3-5).
The objective of
this study was to investigate the neuronal response of conductivity during
visual stimulation and compare that with BOLD.Methods
Participants: In total, 30 young healthy volunteers were recruited from the local
community. In this study, we performed two independent experiments. The
first experiment was performed in 14 young participants.
The second experiment was performed on 16 young participants.
Functional MRI paradigm: Two
sets of independent experiments were performed in this study with
different imaging sequences for MREPT data. Figure 1 shows the paradigms for both experiments for the
three different sequences of 3D bFFE, BOLD, and SE-EPI. In the first
experiment, both the BOLD and two-echo SE-EPI MREPT fMRI sequences were run
with three fixation and three stimulation blocks. For MREPT, the multi-echo (me) SE-EPI
sequence was used. The me-SE-EPI fMRI was run with 60 s per block, 10 scans per
block, and 60 volume scans. The running time was 6 min 0 s. The detailed
stimulation paradigms are summarized in Table
1. In the second experiment, we added a single-echo 3D bFFE sequence for
MREPT. All three fMRI sequences were run with two fixation and two-stimulation
blocks. For MREPT, the single-echo SE-EPI
and single-echo 3D bFFE sequences were used. The single-echo SE-EPI fMRI was
run with 60 s per block, 30 scans per block, and 120 volume scans. The running
time was 4 min 0 s. The 3D bFFE fMRI was run with 90 s per block, 15 scans per
block, and 60 volume scans. The running time was 6 min 0 s. Table 1 also summarizes the detailed
information.
MRI acquisition: The fMRI study was performed on a 3 T MRI System
(Ingenia, Philips Medical System, Best, the Netherlands). First, the GE-EPI sequence was
run to obtain BOLD signals for both experiments. Second, the SE-EPI sequence was run to obtain both magnitude and phase
to then calculate the high-frequency conductivity for a dynamic scan point. The
numbers of echoes were two for the first experiment and one for the second
experiment. Third, the sagittal 3D bFFE
sequence was run to obtain both magnitude and phase to then calculate the high-frequency conductivity. For image registration, sagittal
structural 3D T1-weighted (3D T1W) images were acquired.
Conductivity
mapping for both spin-echo and 3D bFFE MREPT scans: A homemade software was used to map the HFC at the Larmor
frequency of 128 MHz at 3T (6). The MREPT formula based on a convection reaction equation was derived by
adding the regularization coefficient (4). To solve the
convection reaction partial differential equation, we used the 2-dimensional
finite-difference method.
The
MREPT formula based on a convection reaction equation can be derived by adding
the regularization coefficient c. MREPT depends upon the relatively weak phase signal by
a secondary RF magnetic field from the induced electrical current by the
time-varying RF field.
fMRI
data processing: Because visual
stimulation may produce changes in both magnitude through BOLD effect and
conductivity through the phase change, we analyzed both magnitude and
conductivity data. Statistical parametric mapping version 12 software (SPM12;
Wellcome Department of Imaging Neuroscience, University College, London, UK) was used for data preprocessing and
voxel-based statistical analysis.Results
In the voxel-based individual-level analysis, the
conductivity values in the multi-echo SE-EPI sequence were slightly increased
during visual stimulation. However, the conductivity values in the 3D bFFE
sequence fluctuated inconsistently. The mean conductivity values over all
subjects were significantly different between the fixation and visual
stimulations at the primary visual cortex, secondary visual cortex, and cuneus
for both experiments.Conclusion
Conductivity-based fMRI would not be based on measuring
changes in BOLD effect, but rather on the direct detection of neural activity,
which is expected to have the potential for imaging electrical activity in the
brain and would potentially be useful in
several neurophysiological studies. Because the BOLD signal does not correlate
perfectly with action potentials, the conductivity-based fMRI signal may be
helpful for measuring the action potential or membrane potential in the future.
Although the conductivity-based fMRI signal was not stronger than BOLD, the
conductivity value was increased during the visual stimulation at some brain
areas, thus indicating that functional MREPT can be used to measure neuronal
activity. It is unclear whether the slight changes of conductivity in the brain
during the functional activity were due to true physiological mechanisms.
Therefore, further studies are recommended with further optimization of signal
acquisitions of an MREPT technique.Acknowledgements
The research was supported by the National Research
Foundation of Korea (NRF) grants funded by the Ministry of Science and ICT
(2020R1A2C1004749, G.H.J.; 2019R1A2C1004660, O.I.K.;
2020R1F1A1A01074353, M.B.L.), Republic of Korea. References
1.Kwong
KK, et al. Proc Natl Acad Sci U S A 1992;89(12):5675-5679.
2.Ogawa
S, et al. Proc Natl Acad Sci U S A 1992;89(13):5951-5955.
3.Gurler N and Ider
YZ. Magn Reson Med 2017;77(1):137-150.
4. Katscher U, et
al. IEEE Trans Med Imaging 2009;28(9):1365-1374.
5.Leijsen R, et al.
Diagnostics (Basel) 2021;11(2).
6.
Gabriel C, et al. Phys Med Biol 2009;54(16):4863-4878.