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Functional MRI as a Constraint
in Multi-Dipole Models of MEG Data
Korvenoja A
(a,b), Aronen HJ (a,b), and Ilmoniemi RJ (b)
a Department of Radiology, Helsinki University Central
Hospital, Helsinki, Finland b
BioMag Laboratory,
Medical Engineering Centre, Helsinki University Central
Hospital, Helsinki, Finland
Corresponding author: Antti
Korvenoja, Address: P.O. Box 442, FIN-00029 HUS, Finland,
E-mail: antti.korvenoja@helsinki.fi
Abstract. The use of physiological constraints in the
solution of the inverse problem of brain electromagnetic fields
has received increasing attention in recent years. A priori
information is needed to constrain the solution of the electromagnetic
inverse problem; other imaging modalities, such as fMRI, can
provide information of this kind. The goal is to combine complementary
information from different imaging modalities and thus achieve
increased resolution in both spatial and temporal domains.
In this article, the application of functional MRI data in
guiding the construction of multi-dipole models for the interpretation
of magnetoencephalographic data is discussed. Comparison of
the differences of fMRI and MEG is made and convergence of
the results obtained with these methods is described.
1. Introduction>
The electromagnetic inverse problem is notorious in that
any magneto- or electroencephalographic data can be explained
by multiple different source current patterns. To select
from the possible solutions, the use of physiological constraints
has become an attractive approach in recent years especially
after functional magnetic resonance imaging has become widely
available [George JS et al 1995, Ilmoniemi RJ 1995, Simpson
GV et al 1995]. Initially, hemodynamic responses from positron
emission tomography (PET) were applied to this purpose.
In a pioneering study of visual attention, [Heinze et al.1994]
used PET data with a two-dipole model to find the location
for equivalent current dipoles. With its better spatial
and temporal resolution and wider availability fMRI appears
somewhat more attractive, however. With recent developments
in the field of event-related fMRI, it seems possible to
use similar experimental setups as those used in electrophysiological
studies [Buckner RL et al 1996, Buckner RLet al 1998, Buckner
RL et al 1998, Dale AM 1999]. Separation of hemodynamic
responses, even to very rapid stimulation rates, may be
achievable in fMRI experiments [Buckner RL et al 1998, Dale
AM 1999].
The goal in combining information from fMRI and MEG is
to make the methods to complement each other so that the
best resolution of each technique in temporal and spatial
domains is achieved. With fMRI, the commonly achievable
spatial resolution is about one millimeter; with high field
strength MR scanners resolution even at cortical column
level has been achieved [Menon RS et al 1997, Menon RS et
al 1998, Kim DS 1998]. Functional MRI does not provide,
however, much information about temporal characteristics
of the cortical network in the millisecond scale. Rather,
it reflects indirectly the activity of neurons integrated
over a period of several seconds. By measuring latencies
of hemodynamic responses though, one might be able to measure
differences in the onset of activity with a 10-millisecond
resolution [Menon RS et al 1998, Menon RS et al 1998]. Given
the long time constants of the hemodynamic responses, information
about more rapid modulation and offset of activity appears
unachievable for fMRI. Electrophysiological measurements
are still the only methods able to provide information directly
of the neuronal activity on the millisecond time-scale.
Design of experimental setups presents a challenge when
hemodynamic and electrophysiological measurements are used
in combination. Naturally, it would be desirable to use
exactly the same experimental parameters, but usually modified
paradigms have to be used. This is due to the different
nature of the measured responses. The signal-to-noise ratio
may limit the use of similar paradigms. For example, electrophysiological
response amplitudes decrease with increasing stimulation
rate, while the hemodynamic response amplitudes increase
[Wikström H et al 1996, Kampe KKK et al 2000]. As the
hemodynamic response is smaller for shorter stimuli [Buckner
RL 1998], use of short stimulus durations conventionally
used in electrophysiology is of limited value. In electrical
stimulation of peripheral nerves, for example, it is common
to use stimulus durations of 0.2 ms.
2. Convergence of the Methods
The use of spatial information from hemodynamic methods
as a constraint to the electromagnetic inverse problem necessitates
the assumption that the areas that appear active with different
methods are to some extent the same. The spatial correspondence
has been mostly investigated in the context of motor and
somatosensory evoked activity. In the localization of the
primary sensory and motor areas using equivalent current
dipole modeling, typical spatial differences between the
dipole location and the center of fMRI activation have been
between 10 to 16 millimeters [Beisteiner R et al 1995, Beisteiner
et al 1997, Sanders JA et al 1996, Stippich C et al 1998].
In light of the current limited knowledge, the localization
results seem to agree reasonably well when locating responses
from primary sensory areas. Extending comparison to more
complex cortical networks has indicated mostly converging
activation patterns [Ahlfors SP et al 1999, Korvenoja A
et al 1998]. The activation patterns converged better on
group level, thus suggesting that improvements in the sensitivities
of respective techniques would further increase the convergence
of the results.
There are occasions where disagreement in spatial activation
patterns could exist. It is not clear, for example, whether
very short-lasting synchronous firing, which can be detected
in EEG and MEG, will produce a detectable hemodynamic change.
Event-related synchronization and resynchronization are
phenomena that possibly remain undetected by observing hemodynamic
changes. For example, in the study by Ahlfors et al. [Ahlfors
SP et al 1999], MEG indicated activity over the frontal
cortex bilaterally while fMRI did not demonstrate any activity
in similar areas. Using fMRI activation pattern as a strict
spatial constraint or guidance in the model construction
would obviously lead to incomplete and erroneous source
models in these situations. Liu et al. [Liu AK et al 1998investigated
the effect of the spatial constraint weighting to inverse
solutions. In Monte Carlo simulations they found 90% weighting
of the minimum-norm solution as the best compromise, providing
good differentiation of the activity between sources localized
correctly by fMRI and minimization of the errors caused
by missing source areas in fMRI.
3. Applications of fMRI in Multi-Dipole Modeling of MEG
Data
Multi-dipole models and continuous current distribution
models (18) based on minimum-norm estimates have been applied
in efforts to combine electrophysiological data with spatial
information from hemodynamic responses. In two studies,
we have attempted to model complex cortical networks with
interaction from multiple brain areas using multiple ECDs.
Somatosensory evoked responses. We used an eight-dipole
model constrained with fMRI data to model median nerve somatosensory
evoked fields (SEFs) [Korvenoja A et al 1999]. Five normal
subjects were studied. Somatosensory evoked fields were
recorded with a Neuromag-122 magnetometer. In MEG, the interstimulus
interval (ISI) was 5 s, while in fMRI an ISI of 0.25 s was
chosen. The goal was to maximize the response amplitude
in both imaging modalities, in order to achieve the best
possible signal-to-noise ratio. The SEFs were first modeled
independently of fMRI results. Thereafter a multi-dipole
model was constructed by placing ECDs to fMRI activation
centroids. If MEG data indicated activity in some of the
eight source areas but no fMRI activation was seen, then
ECD location from independent MEG data analysis was used.
The eight dipoles were spatially fixed, but were allowed
to change their orientation and amplitude to explain the
data (rotating dipoles). The ECD orientations were remarkably
stable over the whole analysis period (0 to 400 ms poststimulus).
The time-courses of activation in the model were found to
agree with data, that have been obtained with invasive electrophysiological
methods (Table I) [Allison T et al 1989, Allison T et al
1989, Allison T et al 1996, Lüders H et al 1985].
TABLE I. Time of onset of activity in cortical areas
participating in the processing of somatosensory information.
Comparison between mean values obtained from fMRI
constrained multi-dipole model and results of invasive
recordings found in literature(20-23). SMI: primary
sensorimotor cortex, PoCS: postcentral sulcus, AO:
Anterior operculum, PO: posterior operculum, SMA:
supplementary motor area.
Area mean value | Model value | Invasive study | Invasive recording |
| SMI contralateral | 17-22 | Allison et al.1989 | 22 |
| PoCS contralateral | 21-25 | Allison et al.1989 | 25 |
| PO contralateral | 19-32 | Lüders et al. 1995 | 24 |
| AO contralateral | 22-51 | | |
| SMA | 24-48 | Allison et al.1996 | 40-50 |
| SMI ipsilateral | 30-70 | | |
| Allison et al.1989 | 40-50 | | |
| PO ipsilateral | 42-92 | | |
| AO ipsilateral | 32-112 | | |
Visual motion processing. We have also studied temporal
dynamics of visual motion areas, combining fMRI and MEG
data [Ahlfors SP et al 1999]. In this study, the cortical
network processing visual motion was modeled with nine ECDs.
The stimulus was a set of concentric contracting and expanding
rings. The direction of motion changed with 3 s intervals.
Four normal subjects were studied. Magnetic evoked responses
measured with a Neuromag-122 magnetometer were averaged
relative to the time of motion reversal. In fMRI, activation
related to visual motion processing was studied by comparison
between similar contracting and expanding rings versus stationary
rings. The analysis of MEG data was first done independently
of fMRI results. Independent MEG analysis indicated activity
in occipital (V1, V3A), occipito-temporal (MT+) and parieto-temporal
(posterior superior temporal sulcus) areas as well. The
occipito-temporal and frontal sources were found in both
hemispheres in all subjects. The field patterns indicated
the existence of a frontal source at the latency of 170-190
ms. FMRI indicated activity in similar areas bilaterally,
with the exception of frontal activation. A multi-dipole
model with ECDs placed to fMRI activation foci centroids
was constructed. Figure
1 illustrates that the measured fields are explained
unsatisfactorily if sources are constrained only to locations
shown by fMRI. This model apparently did not explain the
data well when frontal sources were active. A clearly better
goodness-of-fit was obtained with a model augmented with
frontal ECDs, whose locations were found independently from
MEG data (Figure 1).
Figure 1.
Visual evoked magnetic fields at 170 ms
after visual motion direction reversal. The recorded magnetic
fields are not modeled sufficiently when the dipoles are
fixed only at the centroids of fMRI activations. Adding
a frontal dipole, whose location is obtained by dipole fitting
independently of fMRI data, results in a better goodness-of-fit
(modified from Ahlfors et al. 1999).
Both of the above mentioned studies indicated that while
complete overlap of activation patterns determined independently
from MEG and fMRI did not exist on individual level, the
activation patterns did converge at the group level.
Figure 2. Somatosensory
evoked activity in opercular areas is usually modeled with
one dipole in each hemisphere. Functional MRI data indicate,
however, that activity is distributed in two clusters in
each hemisphere: one in parietal operculum and one in frontal
operculum and the insula. Using two dipoles bilaterally
in the operculum (8-dipole model) clearly improves the model
goodness-of-fit in opercular areas.
When sources are located close to each other, it might
prove difficult to separate them into distinct source areas,
even though shifts in the dipole location might indicate
that multiple generators exist in an area. This is the case,
for example, with opercular sources (Figure
2) of SEFs. The source area in postcentral sulcus for
somatosensory evoked fields is very close to primary sensorimotor
areas. Functional MRI, however, indicates separate areas
of activation.
The results from these studies suggest that while fMRI
cannot be used as a strict constraint in modeling MEG data,
it will be useful in giving further validation for the source
configuration used in a model.
4. Conclusion
Current results indicate that while it may not be possible
to simply restrict the source model solutions to areas where
fMRI shows activation, it still seems to be a valuable aid
in the validation of the source model. Even when the experimental
setups in fMRI and MEG were slightly different, a similar
activation pattern could be seen with both methods in our
studies. Converging lines of evidence from multiple methods
will increase the likelihood of correct solution. The ultimate
way to validate the inverse solution will be invasive recordings.
Data from cortical surface recordings and depth electrode
measurements are scarce for obvious reasons. Our experience
from somatosensory evoked fields modeled with fMRI guided
multi-dipole model shows that the time-course of activation
shown by the model agrees with invasive data at least in
those areas where reported data are available in the literature.
Acknowledgements
This work has been financially supported by grants from
the Helsinki University Central Hospital (TYH-0313), the
European Commission 5th framework program (QLK3-CT-1999-00894),
the Academy of Finland, Sigrid Juselius Foundation, Cancer
Organizations of Finland, and the Helsinki University Central
Hospital Clinical research institute. The authors thank
Dr. Seppo Ahlfors for providing an image used in this publication.
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