Matthias F. Valverde Salzmann1, Klaus Scheffler1, and Rolf Pohmann1
1High-field Magnetic Resonance, Max Planck Institute for Biological Cybernetics, Tuebingen, Germany
Synopsis
A setup for concurrent functional MRI and intrinsic
optical imaging spectroscopy inside a 14.1 T animal scanner was developed,
based on a magnetic field proof camera and optics. fMRI and optical imaging
were simultaneously performed on rats with electrical forepaw stimulation,
resulting in excellent signals for both BOLD and optical reflectance in two
wavelengths (red and green). Only minor interactions between both modalities were
observed. The combination of these two techniques can be used to investigate
the origins of the BOLD effect and to open up novel ways of exploring brain
function.Introduction
Functional
magnetic resonance imaging (fMRI) has become the most important technique to monitor blood
flow responses that follow neural activity. However, the spatial resolution of
most MR scanners is restricted to voxel sizes larger than
the size of cortical columns (~200 µm), which makes investigations of
neurovascular coupling at submillimeter scale difficult. In contrast, optical
imaging of intrinsic signals (IOI) has been used for more than 20 years to
record hemodynamic responses at high spatial and temporal resolutions, allowing
to map columnar structures like individual barrels in rodent cortices or
orientation columns in the primary visual cortex of primates and other species.
However, it lacks the third dimension that fMRI is able to provide. In order to
get deeper insights into the origin of the BOLD signal we have created a setup
that allows us to combine the benefits of both techniques.
Methods
Setup: An optical imaging
setup was designed that is completely
capable of functioning inside our 14.1 T MR scanner (Fig. 1), based on a
custom-made 5.5 megapixel (2560 x 2160 pixel) board-level camera equipped with
a scientific, highly sensitive CMOS sensor, capable of recording
images at framerates of up to 120Hz. A tandem macroscope was assembled of two
objectives (Nikon Nikkor 50mm F1.2 and Zeiss Sonnar 135mm F1.8) with an effective
magnification of 2.7. Both objectives were stripped of all mechanical elements,
leaving only the lenses and the lens mounting (mainly aluminum), which was replaced
by plastic in the regions close to the rat brain to avoid artifacts. The cortical
surface was illuminated by red or green light (LEDs peak wavelengths: 530nm,
630nm) that was guided to the cortical surface by eight 1mm diameter PMMA
fibers.
Animal preparation: Rats were anesthetized with urethane. The
skull was removed to form a cranial window of about 6x6 mm2 above
the somatosensory forepaw region. The dura was left unharmed. Neuronal activity
inside S1 was triggered by forepaw stimulation, applying 9 mA currents with 9
Hz for four seconds through two electrodes inserted in the forepaw.
Optical Imaging: Reflectance images from the cortical surface were recorded at green and
red light illumination in consecutive stimulus blocks, each consisting of 15 stimulus
trials. 800 frames were recorded per single trial at 29 Hz, 30 ms exposure /frame
and 2560x2160 pixel resolution. The signal-to-noise ratio was enhanced by averaging all 15 trials of a
single block and additional 2x2 pixel binning. To calculate single condition maps we used a frame-0-subtraction: Twenty
camera frames preceding stimulus onset were
averaged to form the frame zero. Each frame following stimulus
onset and its ten nearest neighbours
were averaged and used to calculate percentage signal changes. For topographic localization of functional domains,
reflectance maps were further filtered for high and low frequencies in the
spatial domain.
fMRI: A
single loop surface coil around the cranial window served to transmit and
receive MRI signals. Functional images were acquired from four 0.5 mm slices parallel
to the brain surface with EPI with a spatial resolution of (0.31 mm)2, a matrix
size of 642, and a TR of 1 s. To investigate the effect of the rapid
gradient switching in EPI, additional functional scans were performed using a FLASH
sequence with long TE. The data were processed with home-written Matlab
routines.
Results
Intrinsic optical signals
were of excellent quality and allowed for clear identification of activated
cortex regions (Fig. 2) in both red and green light, indicating changes in oxygenation
and CBV, respectively. Reflectances up to 0.15% were observed. RF-transmission
during the MRI scans had no effect on the images, while the rapidly switched
EPI gradients cause slight vibrations in the optical images, which get stronger
for increasing spatial resolution of the fMRI scans, but disappear when using a
FLASH sequence. fMRI signals were not significantly affected by the presence
and operation of the camera. BOLD signal changes of up to 15% were observed in
all slices.
Discussion
Concurrent fMRI and intrinsic optical imaging with high spatial
resolution is possible even in the magnetic field of an ultra-high field animal
scanner. In contrast to previous approaches, which rely on optical fibers to
guide the signal to a camera outside the magnetic field [1], our setup uses a
magnetic field proof camera and optics, allowing for higher sensitivity and
spatial resolution. The excellent quality of both optical and BOLD signals will
allow for a detailed investigation of the spatial and temporal formation of the
BOLD signal and open up novel possibilities to explore brain function by a
combination of those two modalities.
Acknowledgements
No acknowledgement found.References
[1] A. J. Kennerley, J. Berwick, J. Martindale, D. Johnston,N. Papadakis, J. E. Mayhew: Concurrent fMRI and Optical Measures for theInvestigation of the Hemodynamic Response Function. Magn. Reson. Med. 54, 354-365 (2005)