Yuhui Chai1, Guoqiang Bi2, Liping Wang3, Fuqiang Xu4, Xin Zhou4, Bensheng Qiu2, Hao Lei4, Bing Wu5, Yang Fan5, and Jia-Hong Gao1
1Center for MRI Research, Peking University, Beijing, China, People's Republic of, 2University of Science and Technology of China, Hefei, China, People's Republic of, 3Shenzhen Institutes of Advanced Technology, Chinese Academy of Sciences, Shenzhen, China, People's Republic of, 4Wuhan Institute of Physics and Mathematics, Chinese Academy of Sciences, Wuhan, China, People's Republic of, 5GE Healthcare, MR Research China, Beijing, China, People's Republic of
Synopsis
In-vivo detection of neuronal
current remains a challenging and promising goal in fMRI. Previous work has
demonstrated its feasibility in phantom and cell culture studies, but attempts
in in-vivo studies remain few and far between. As neuronal current is usually comprised
of a series of oscillatory waveforms rather than being a direct current, it is most
likely to be detected using oscillatory current sensitive sequences. In this
study, we explored the potential of using the spin-lock oscillatory excitation
(SLOE) sequence to directly detect optogenetically evoked oscillatory neuronal current
in vivo for the first time.Purpose
In-vivo detection of neuronal current remains a
challenging and promising goal in fMRI. Up to present, progress has been made in phantom
1 and cell culture
2
studies, but no conclusive reports have been made for in-vivo studies
3,4. As neuronal current is usually comprised of a series of oscillatory
waveforms rather than being a direct current, it is most likely to be detected using
oscillatory current sensitive sequences. Spin-lock oscillatory excitation (SLOE) has been reported to be the most
sensitive method up to date and showed sub-nanotesla level detection of
oscillatory current in phantom experiment
5. In this study, we explored
the potential of using SLOE sequence to
directly detect oscillatory neuronal current in vivo for the first time.
Methods
SLOE was implemented with a
spiral readout for minimal TE (Fig. 1a). Phantom
experiment was first performed with a single copper loop
(diameter, 1.1 cm) immersed in a 3.0 mM NiCl2 solution. A function generator was connected
to the loop to generate a 100 Hz sinusoidal current with an amplitude of 0.5 nT
at the center of the loop according to the Biot-Savart law. Optogenetic animal
experiment was performed by first injecting 1 µl virus of AAV5-Syn-ChR2(ET/TC)-EYFP into V1
cortex of Sprague-Dawley rats (200-250
g) and letting it express for
more than 7 weeks. Then optogenetically
evoked oscillatory neuronal current could
be evoked by delivering a series of 473 nm laser pulses at less than 80 mW/mm2
irradiance above the cortex of viral injection (Fig. 3). Such an oscillatory
neuronal current was expected to induce spin-lock excitation only if the oscillatory
frequency equals the spin-lock intensity.
MR data acquisition was performed
using a 7 T Bruker Biospec animal scanner. SLOE was used for phantom and
in-vivo experiments with the same parameters: spin-lock time (TSL) = 70 ms, spin-lock
intensity (BSL) = 100 Hz, TR/TE = 1000/5 ms, resolution =
0.47×0.47 mm2, slice thickness = 1 mm. In
in-vivo experiments, BOLD
signal was acquired before and after the whole ncMRI acquisitions
to confirm the existence of neuronal response, using a GE-EPI sequence with TR/TE = 1000/25 ms, FA = 55⁰ (Ernst angle) and identical geometry
parameters with SLOE. The detailed stimuli pattern of ncMRI experiment is
illustrated in Fig. 5a: light stimulation (4 ms, 100 Hz) is ON only during the
spin-lock time in the first TR out of every 15 consecutive TRs, and polarity of
the stimulation changes every 15 TRs. Acquisition for ncMRI is made in every
first TR. After the data was 2D motion corrected and high-pass filtered at
0.006 Hz, GLM fitted analysis was performed to determine the activation map.
Results
SLOE
acquisitions in phantom are summarized in Fig. 1: with oscillatory currents of opposite
polarities (Fig. 1a), the detected signal also showed opposite polarities inside
and outside the loop (Fig. 1b). The expressions of ChR2-EYFP were verified with
confocal images (Fig. 2a); their overlaying with NeuN (red marker) and DAPI
(blue marker) demonstrates the specific expression in neuron cells (Fig. 2b). Fig.
3 shows the recorded optogenetically
evoked oscillatory LFP signals at different stimulation frequencies (20 Hz,
50 Hz, 80 Hz), along
with their spectrograms. BOLD activation is shown in Fig. 4, and such
activation area was consistent among different rats. However, no consistent
activation pattern was observed in SLOE detection with either polarity of
stimulation as displayed in Fig. 5.
Discussion and conclusion
In this work, SLOE, the most sensitive ncMRI
method reported up to date was implemented on a high field 7 T scanner for in-vivo
experiment. Thorough experiment design was performed including optimizations of
imaging protocol and stimulation pattern, phantom verification of hypothesis,
LFP verification of optogenetical stimulation, and BOLD verification of brain activation. However, SLOE
detection in vivo did not lead to statistically significant results. Given the
shown sub-nanotesla level of sensitivity in phantom, the main hurdle of SLOE in
vivo is the vulnerability to field inhomogeneity, which should be the focus of
technical refinement in the next stage.
Acknowledgements
This work was supported by
China’s National Strategic Basic Research Program (973) (2012CB720700), the
Natural Science Foundation of China (81227003, 81430037, 31421003, 91132307 and
31171061) and the Strategic Priority Research Program of the Chinese
Academy of Sciences (XDB02050002).References
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