Seong-Gi Kim1
1Institute for Basic Science and Sungkyunkwan University, Korea, Republic of
Synopsis
Keywords: Contrast mechanisms: fMRI, Neuro: Brain function, Neuro: Brain connectivity
Laminar
fMRI has been increasingly used for determining feedforward and feedback
inputs to the cortex. To properly design
and interpret laminar-resolution fMRI experiments, it is critical to examine biophysical
and physiological sources of hemodynamic and fMRI signals. In this education talk, we will discuss 1) laminar
fMRI contrasts such as GE-BOLD, SE-BOLD, CBV and CBF, 2) up-to-dated depth-dependent
neurophysiological findings, and 3) relationships between laminar-specific electrophysiology
and hemodynamic responses.
High-resolution fMRI at ultrahigh
fields is getting popular to map functional sites and connectivity with high
sensitivity and specificity. To advance brain research further, it is critical to
dissect different circuits, such as ascending feedforward and descending feedback
circuits, with fMRI. Since cortical depth-dependent
fMRI (often referred to as ‘layer fMRI’, ‘laminar fMRI’) may determine
layer-specific neural circuits, it has been of great attention to fMRI
scientists (see https://layerfmri.com/category/layer-fmri-papers/). However, fMRI is an indirect measure of neuronal
responses via the vascular or hemodynamic responses, thus it is critical to
understand the relationship between laminar fMRI and physiology for designing
fMRI studies and interpreting the laminar fMRI signal properly (e.g., review
articles of neurophysiological basis: Poplawsky et al., 2019; Self et al,
2019).
Initially, we need to review
existing fMRI contrasts in terms of vascular specificity and sensitivity (see Fukuda
et al., 2021). The vasculature is
hierarchically connected so that local responses will have up- and downstream
effects on vessels far from the site of neuronal activity. Because the utility
of laminar-resolution fMRI is contingent on separating these neural-specific
responses from the nonspecific, many different forms of fMRI contrasts have
been examined (Jin & Kim, 2008a).
The most popular approach is GE BOLD due to its high sensitivity, high
temporal resolution and whole-brain coverage. However, this high sensitivity is
partly due to the contributions of non-specific draining vessels, including
pial veins. Thus, it is crucial to remove non-specific contributions to improve
spatial specificity with differential analysis (Olman et al., 2012) and
model-basis deconvolution (Markuerkiaga et al., 2016; Marquardt et al., 2020). Alternatively,
the SE-BOLD approach refocuses dephasing signals around the large vessels,
improving spatial specificity to microvessels. Thus, SE-BOLD fMRI is a better approach
for laminar fMRI (Zhao et al., 2004; Han et al., 2021), compared to GE BOLD, but
with reduced sensitivity.
Since the majority of CBF originates
from capillaries, fMRI with arterial spin labelling was shown to have improved
neural specificity compared to GE BOLD and to overlap well with layers that
have increased synaptic activity (Duong et al., 2000). However, CBF fMRI has a
lower sensitivity compared to BOLD fMRI. Similar to CBF, the CBV contrast also provides
better laminar specificity compared to GE-BOLD fMRI (Zhao et al., 2006), since
it originates from arterial macrovessels and microvessels. Consequently, noninvasive
CBV-weighted vascular space occupancy (VASO) fMRI-based techniques (Huber
et al., 2017; Jin & Kim, 2008b; Lu et al., 2003) are increasingly adopted for laminar
fMRI.
Next important point is the
relationship between laminar neural activity and hemodynamic responses. The
most intuitive model for laminar neurovascular coupling studies is the primary
sensory cortex such as V1 and S1. Sensory cortices generally consist of six
layers; however, these layers typically function as three. Sensory stimulation
evokes a transient change in neuronal activity first in layer IV (i.e.,
granular layer) and, subsequently, activity spreads immediately into the
supragranular (layers I – III) and infragranular (V and VI) layers, and
recruits recurrent and feedback circuitry to produce sustained neuronal
activity across all the layers. Indeed, sensory stimuli induced the highest fMRI
response in layer IV where has the highest local field potentials and multiunit
activity (Self et al., 2019; Jung et al., 2022). Similar correspondence between
CBV and electrophysiology was observed in the olfactory bulb (Poplawsky et al.,
2015). These suggest that fMRI can identify
the synaptic input layer.
Many important unresolved issues (discussed
in Fukuda et al. 2020) are 1) why the first synaptically activated
layer induces the highest CBV and CBF response, even though there are recurrent
circuits among layers, 2) why the late CBV response is more specific to the
synaptic active layers (Jin & Kim, 2008a), 3) why the hemodynamic
response time difference is related to laminar processing (Jung et al., 2021; Petridou
& Siero, 2019; Silva & Koretsky, 2002), and 4) whether neural output layers can be identified from synaptic input layers (Huber et al. 2017). These issues will be discussed. Acknowledgements
Supported by Institute for
Basic Science in Korea (IBS-R015-D1)References
Duong
TQ et al (2000) Functional MRI of calcium-dependent synaptic activity: cross
correlation with CBF and BOLD measurements. Magn Reson Med, 43(3), 383-392.
Fukuda
M et al (2021) Time-dependent spatial specificity of high-resolution fMRI:
insights into mesoscopic neurovascular coupling, Phil. Trans. R. Soc. B 376,
20190623.
Jin
T, Kim S-G (2008a) Cortical layer-dependent dynamic blood oxygenation, cerebral
blood flow and cerebral blood volume responses during visual stimulation.
Neuroimage, 43(1), 1-9.
Jin
T, Kim S-G (2008b) Improved cortical-layer specificity of vascular space
occupancy fMRI with slab inversion relative to spin-echo BOLD at 9.4 T.
Neuroimage, 40(1), 59-67.
Jung
WB et al (2021) Early fMRI responses to somatosensory and optogenetic
stimulation reflect neural information flow, PNAS, 118 (11), e2023265118
Jung
WB et al (2022) Dissection of brain-wide resting-state and functional
somatosensory circuits by fMRI with optogenetic silencing, PNAS, 119 (4),
e2113313119.
Han
SH et al. (2021) Improvement of sensitivity and specificity for laminar BOLD
fMRI with double spin-echo EPI in humans at 7 T, Neuroimage, 241, 118435.
Huber
L et al. (2017) High-Resolution CBV-fMRI Allows Mapping of Laminar Activity and
Connectivity of Cortical Input and Output in Human M1. Neuron 96, 1253-1263.e7.
Lu H
et al. (2003) Functional magnetic resonance imaging based on changes in
vascular space occupancy. Magn Reson Med,
50(2), 263-274.
Markuerkiaga
I et al. (2016) A cortical vascular model for examining the specificity of the
laminar BOLD signal. Neuroimage 132, 491–498.
Marquardt
I et al. (2020) Feedback contribution to surface motion perception in the human
early visual cortex. Elife 9, 1–28.
Olman
CA et al. (2012) Layer-specific fmri reflects different neuronal computations
at different depths in human V1. PLoS One, 7.
Petridou
N, Siero JCW (2019) Laminar fMRI: What can the time domain tell us?, Neuroimage
197, 761-77.
Poplawsky
AJ et al. (2015) Layer-Specific fMRI Responses to Excitatory and Inhibitory
Neuronal Activities in the Olfactory Bulb. J Neurosci, 35(46), 15263-15275.
Poplawsky
AJ et al. (2019) Foundations of layer-specific fMRI and investigations of
neurophysiological activity in the laminarized neocortex and olfactory bulb of
animal models, Neuroimage, 199, 718-729.
Self
MW et al., (2019) Benchmarking laminar
fMRI: Neuronal spiking and synaptic activity during top-down and bottom-up
processing in the different layers, Neuroimage, 197, 806-817.
Silva
AC, Koretsky AP (2002) Laminar specificity of functional MRI onset times during
somatosensory stimulation in rat. Proc Natl Acad Sci U S A, 99(23), 15182-15187.
Zhao
F et al. (2004) Cortical depth-dependent gradient-echo and spin-echo BOLD fMRI
at 9.4T. Magn Reson Med, 51(3),
518-524.
Zhao
F et al. (2006) Cortical layer-dependent BOLD and CBV responses measured by
spin-echo and gradient-echo fMRI: Insights into hemodynamic regulation.
Neuroimage, 30(4), 1149-1160.