Laura Bortolotti1, James Antony Smith1, Penny Gowland1, and Richard William Bowtell1
1SPMIC, University of Nottingham, Nottingham, United Kingdom
Synopsis
The
extra-cranial magnetic field changes due to changes in head position have been measured
in a 7T scanner using a 16-channel field camera and used to estimate the head
movements. A partial least squares regression was used to identify the
relationship between field changes and head position data that was
simultaneously measured using an optical camera. By applying spherical harmonic
spatial filtering to the field measurements it was possible to reduce the
unwanted effect of chest movement in respiration, and to then predict head
position changes with good accuracy. This provides a step forward towards a
non-contact motion monitoring technique.
Introduction
Head
movement during MRI produces image artefacts resulting from errors in spatial
encoding and distortions related to position-dependent field perturbations. A
variety of methods for monitoring head position inside the scanner and then
using this information to correct image data, prospectively or retrospectively,
have been developed1.
Some of these methods require the rigid attachment of markers to the head (e.g.
Moire Phase Tracking [MPT] marker(s) or NMR probes), while others require
modification of the imaging sequence to allow rapid acquisition of navigator
information. Here, we evaluate the potential for using measurements of the
magnetic field perturbations produced outside the head for monitoring head
position inside a 7T MR scanner. This approach could allow contactless motion
monitoring without the need for modification of imaging sequences. In
experiments on four subjects we used a 16-channel field camera in conjunction
with a MPT camera system to simultaneously monitor external field changes and
head position and to test the possibility of calculating head position from
field measurements.Methods
Figure 1 shows the experimental
set-up2. 16
field probes were mounted in a set of rings placed inside the head RF coil,
while the MPT marker was attached to a dental mould using a small extension so
that it was visible to a camera mounted within the scanner bore. Data were
recorded from each subject for 60s periods corresponding to four different
conditions: rest, head nodding, head shaking and wiggling the feet. During each
recording, respiratory and cardiac cycles were also monitored using the
scanner’s physiological logging system (peripheral pulse unit and respiratory
belt). Data were temporally aligned3 and resampled at a common frequency of 10Hz
(the field camera data was acquired at 10 Hz, while the MPT camera and
physiological signals have higher acquisition frequencies). Figure 2 shows example
data recorded from one subject during 35s-segments of the rest and head shaking
conditions. The data from the rest condition show that, as expected, there are
fluctuations of the field measurements of order 10-7 T in magnitude
which are correlated with the respiratory belt signal. These variations are not
evident in the head position parameters reported by the MPT camera as they
arise from chest movement. To eliminate these effects, we fitted the field
probe measurements at each time point to a series of spherical harmonics up to
3rd order and then reconstituted the signals using only the 2nd
and 3rd order harmonics: the field variation due to chest movement
is represented by the lower order harmonics and so largely eliminated, while
the field variation due to head movement is mainly represented by higher order
harmonics (see Fig. 3).
We used a partial least squares (PLS) regression
to relate the filtered field camera measurements to the changes in head
position measured using the MPT camera system. For each data set the PLS
coefficients were derived using 75% of the data and the measured coefficients
were then used to predict the position changes from the remaining 25% of field
camera measurements. The accuracy of the predicted value was evaluated by calculating
the Root Mean Squared Error (RMSE) with respect to the MPT-measured parameters,
and the ratio of the RMSE with respect to the standard deviation (STD) of the actual
position changes.Results
Figure
4 shows the movement parameters predicted by applying the PLS regression method
to the field camera measurements in comparison to the actual parameters
measured using the MPT camera on one subject for the feet wiggling, shaking and
nodding conditions. The RMSE and
RMSE/STD values are also reported for each movement parameter (translation in
mm and rotation degrees). Figure 5 reports these measures for the three conditions
for all four subjects.Discussion
Elimination
of the field variations that result from sources other than head movement by
spatial filtering improved the predictions of head position using the field
camera. The PLS method can identify the relationship between changes in head
position and the pattern of field variation from measurements acquired over
45s. The accuracy of prediction of movement parameters is better for the larger
movements, and for the dominant movement parameters for each type of motion.Conclusion
Measurements
of the changes in the field generated outside the head can be used to estimate
head movement parameters with reasonable accuracy. For practical use it would
be necessary to learn the relationship between the field variation and head
positions, which requires access to simultaneous measures of head position made
using another approach (e.g. optical camera or navigators) during the learning
phase.Acknowledgements
No acknowledgement found.References
1. Aranovitch A., Haeberlin M., Gross S. et al.
Prospective Motion Correction With NMR Markers Using Only Native Sequence
Elements. Magn Reson Med. 2018; 79:2046–2056.
2. Bischof L., Smith J., Mougin O. et al. Relating
external magnetic field changes to head movement using motion and field
cameras. Hawaii,USA ISMRM; 0303. 2017
3. Bortolotti L., Smith J., Spancer G. et al .Test
of multiple sensor set-up for head motion characterization during MRI
acquisition. Master Thesis, University of Bologna, Italy, 2017