Synopsis
Keywords: Data Analysis, Brain, Quantitative Susceptiblity Mapping, fQSM, fMRI
Functional QSM (fQSM) detects changes in blood
oxygenation in response to neuronal activation, providing complementary
information to conventional magnitude-based fMRI. For standard structural
gradient-echo QSM, multi-echo (ME) acquisitions are more accurate than
single-echoes. Preliminary work suggests this holds for ME-EPI. Previous fQSM
studies used single-echo EPI with physiological noise correction but with ME-EPI,
we observed fQSM activations in the visual cortex with a visual stimulus without
physiological noise correction. ME and single-echo EPI fQSM
were compared, showing that ME-EPI might be preferable. fQSM activations were
weaker (maximum T-score=4 compared to 10 in fMRI) and more localised than fMRI,
as expected.
Introduction
Functional quantitative
susceptibility mapping (fQSM) provides complementary information to
conventional magnitude-based BOLD fMRI, showing potential to improve spatial
localisation of neuronal activity1,2. This is because QSM reveals the blood susceptibility changes that
underlie magnitude signal changes in the BOLD model of functional activation.
fQSM is also based on the linear dependence of susceptibility on blood
oxygenation3 rather than the non-linear dependence of the T2*-weighted signal
magnitude on blood oxygenation4.
Using multiple echoes provides more
accurate QSM than single echo acquisitions for conventional 3D gradient-echo
acquisitions5–7. Preliminary work suggests this holds for multi-echo EPI8. Further, there is increasing evidence that combining images from
multiple echoes recovers signal drop-out and considerably increases fMRI
sensitivity compared to conventional single-echo EPI9–11. Therefore, in this preliminary study, we investigated multi-echo
EPI for fQSM and compared it to fQSM at each echo as all published fQSM
studies, e.g.1,2,12,13, have used single-echo EPI. We also investigated the effect of the
size of the smoothing kernel on fQSM activations.Methods
Image acquisition: 70 volumes of multi-echo GRE EPI were
acquired in a healthy male volunteer (30 years old) on a 3T Siemens-Prisma
using a 64-channel head coil with the parameters shown in Figure 1. Structural T1-weighted images were acquired for anatomical reference.
fMRI stimulus: A standard visual stimulation paradigm was used to
maximise the BOLD signal with a conventional block design shown in Figure 1.
Data
processing: For all multi-echo processing brain
masks were calculated using FSL BET14 on the magnitude images from the second echo. For single-echo
fQSM, BET masks were calculated on the magnitude image at each echo. For all
analyses, transformations from the combined-magnitude timeseries registrations (1,
below) were applied to the masks at each volume. All masks were eroded by a
single voxel.
For the magnitude-based fMRI analysis,
the multi-echo magnitude images were combined using T2*-weighted
echo summation15. Quantitative susceptibility maps (QSM) were calculated from the
phase images at each timepoint of the fMRI time-series: the total field map was
calculated using a non-linear fit of the complex data16 plus Laplacian unwrapping17; intra-slice background fields were removed with 2D V-SHARP18 followed by 3D-PDF19 to remove inter-slice fields20 and susceptibility maps were calculated using non-linear total
variation regularisation (FANSI, a = 2x10-4)21.
SPM1222,23 was used for fMRI and fQSM processing. Spatial pre-processing
performed on both the combined magnitude images and the QSM included: (1) rigid-body
realignment of the magnitude images to the first image in the time-series to
correct for motion. The resulting transformations were then applied to the
corresponding susceptibility maps (and masks). (2) spatial smoothing with an 8
mm FWHM Gaussian kernel to improve SNR and increase statistical power24. We investigated the effect of the FWHM (0, 2, 4, 6, 8 mm) of this
kernel on the fQSM activation maps.
Note that, unlike previous fQSM
studies, e.g.1,2, no additional physiological noise correction was performed. A
general-linear model (GLM) was reconstructed with a regressor for the visual
stimuli. Statistically significant changes were detected by voxel-wise t-tests.
fMRI and fQSM activation maps were calculated using a threshold of p<0.001
and no FWE correction without restriction of minimum cluster size to allow
individual supra-threshold voxels to be apparent.Results and Discussion
Figure 2 shows a
representative susceptibility map. Figure 3 shows fMRI and fQSM activation maps,
in which activations appeared in the primary visual cortex as expected. Similar
to previous fQSM studies1,2,12, the magnitude fMRI response was stronger (larger t-values) and more
widespread (more activated voxels) than in the fQSM, with less noise in the
timecourse (Figure 3). Despite the lack of physiological noise correction, voxels
in the visual cortex show significant activation in the ME-EPI fQSM, similar to
previous fQSM studies with a visual paradigm1,2. The results of fQSM for separate single echoes (Figure 4) show that the
second echo (TE=33.71 ms) gave more statistically significant activations than
the first echo (TE=12.8 ms), which showed no activations, and the third echo
(TE=54.63 ms), which gave only one cluster. This might be because the second
echo time is closest to the tissue T2* at which susceptibility
contrast is maximized6. The activations in the ME-EPI fQSM (Figure 3) had fewer clusters more
localized to the visual cortex than the fQSM at the second echo, suggesting
that ME-EPI may provide more accurate fQSM than single-echo EPI. Figure
5 shows the effect of smoothing kernel size on fQSM activations. The FWHM=8 mm kernel
was chosen as it gave the fewest clusters of activated voxels.Conclusions
Here, we showed that fQSM is feasible using multi-echo EPI, in contrast
to previous fQSM studies which have used single-echo EPI. We observed fQSM
activations in the visual cortex in response to a visual stimulus even without
physiological noise correction that was essential in previous fQSM studies.
This suggests that ME-EPI shows promise for fQSM although future work is needed
to optimise physiological noise correction techniques for ME-EPI fQSM. As
expected, activations in fQSM were weaker and more localised than in
conventional BOLD-fMRI. It is not clear from this preliminary study whether
this is due to improved spatial localisation of neuronal activity in fQSM or
reflects its greater sensitivity to physiological noise.Acknowledgements
All authors except for Oliver Kiersnowski were supported by European Research Council Consolidator Grant DiSCo MRI SFN 770939.
Oliver Kiersnowski was supported by the EPSRC-funded UCL Centre for Doctoral Training in Intelligent, Integrated Imaging in Healthcare (i4health)(EP/S021930/1).References
[1] P. S. Özbay et
al., “Probing neuronal activation by functional quantitative susceptibility
mapping under a visual paradigm: A group level comparison with BOLD fMRI and
PET,” NeuroImage, vol. 137, pp. 52–60, Aug. 2016, doi:
10.1016/j.neuroimage.2016.05.013.
[2] D.
Z. Balla et al., “Functional quantitative susceptibility mapping
(fQSM),” NeuroImage, vol. 100, pp. 112–124, Oct. 2014, doi:
10.1016/j.neuroimage.2014.06.011.
[3] V.
Jain, O. Abdulmalik, K. J. Propert, and F. W. Wehrli, “Investigating the
magnetic susceptibility properties of fresh human blood for noninvasive oxygen
saturation quantification,” Magn. Reson. Med., vol. 68, no. 3, pp.
863–867, 2012, doi: 10.1002/mrm.23282.
[4] J.
R. Reichenbach, R. Venkatesan, D. A. Yablonskiy, M. R. Thompson, S. Lai, and E.
M. Haacke, “Theory and application of static field inhomogeneity effects in
gradient-echo imaging,” J. Magn. Reson. Imaging, vol. 7, no. 2, pp.
266–279, 1997, doi: 10.1002/jmri.1880070203.
[5] G.
Gilbert, G. Savard, C. Bard, and G. Beaudoin, “Quantitative comparison between
a multiecho sequence and a single-echo sequence for susceptibility-weighted
phase imaging.,” Magn. Reson. Imaging, 2012, doi:
10.1016/j.mri.2012.02.008.
[6] B.
Wu, W. Li, A. V. Avram, S.-M. Gho, and C. Liu, “Fast and tissue-optimized mapping
of magnetic susceptibility and T2* with multi-echo and multi-shot spirals,” NeuroImage,
vol. 59, no. 1, pp. 297–305, Jan. 2012, doi: 10.1016/j.neuroimage.2011.07.019.
[7] E.
Biondetti, A. Karsa, D. L. Thomas, and K. Shmueli, “Investigating the accuracy
and precision of TE-dependent versus multi-echo QSM using Laplacian-based
methods at 3 T,” Magn. Reson. Med., vol. 84, no. 6, pp. 3040–3053, 2020,
doi: 10.1002/mrm.28331.
[8] O.
Kiersnowski, P. Fuchs, S. Wastling, M. Elgwely, J. Thornton, and K. Shmueli,
“Optimising Multi-Echo and Single-Echo 2D EPI for Rapid QSM: What is the
Maximum TE?,” QMR Lucca: Joint Workshop on MR phase, magnetic susceptibility and electrical properties mapping, Italy, 2022.
[9] B.
A. Poser and D. G. Norris, “Investigating the benefits of multi-echo EPI for
fMRI at 7 T,” NeuroImage, vol. 45, no. 4, pp. 1162–1172, May 2009, doi:
10.1016/j.neuroimage.2009.01.007.
[10] S.
Posse, “Multi-echo acquisition,” NeuroImage, vol. 62, no. 2, pp.
665–671, Aug. 2012, doi: 10.1016/j.neuroimage.2011.10.057.
[11] P.
Kundu et al., “Integrated strategy for improving functional connectivity
mapping using multiecho fMRI,” Proc. Natl. Acad. Sci. U. S. A., vol.
110, no. 40, pp. 16187–16192, Oct. 2013, doi: 10.1073/pnas.1301725110.
[12] H.
Sun, P. Seres, and A. h. Wilman, “Structural and functional quantitative
susceptibility mapping from standard fMRI studies,” NMR Biomed., vol.
30, no. 4, p. e3619, 2017, doi: 10.1002/nbm.3619.
[13] Z.
Chen and V. D. Calhoun, “Task-evoked brain functional magnetic susceptibility
mapping by independent component analysis (ϿICA),” J. Neurosci. Methods,
vol. 261, pp. 161–171, Mar. 2016, doi: 10.1016/j.jneumeth.2016.01.007.
[14] S.
M. Smith, “Fast robust automated brain extraction,” Hum. Brain Mapp.,
vol. 17, no. 3, pp. 143–155, Nov. 2002, doi: 10.1002/hbm.10062.
[15] B.
A. Poser, M. J. Versluis, J. M. Hoogduin, and D. G. Norris, “BOLD contrast
sensitivity enhancement and artifact reduction with multiecho EPI:
Parallel-acquired inhomogeneity-desensitized fMRI,” Magn. Reson. Med.,
vol. 55, no. 6, pp. 1227–1235, 2006, doi: 10.1002/mrm.20900.
[16] T.
Liu, C. Wisnieff, M. Lou, W. Chen, P. Spincemaille, and Y. Wang, “Nonlinear
formulation of the magnetic field to source relationship for robust
quantitative susceptibility mapping,” Magn. Reson. Med., 2013, doi:
10.1002/mrm.24272.
[17] M.
A. Schofield and Y. Zhu, “Fast phase unwrapping algorithm for interferometric
applications,” Opt. Lett., vol. 28, no. 14, pp. 1194–1196, Jul. 2003,
doi: 10.1364/ol.28.001194.
[18] W.
Li, B. Wu, and C. Liu, “Quantitative susceptibility mapping of human brain
reflects spatial variation in tissue composition,” NeuroImage, vol. 55,
no. 4, pp. 1645–1656, Apr. 2011, doi: 10.1016/j.neuroimage.2010.11.088.
[19] T.
Liu et al., “A novel background field removal method for MRI using
projection onto dipole fields (PDF),” NMR Biomed., vol. 24, no. 9, pp.
1129–1136, Nov. 2011, doi: 10.1002/nbm.1670.
[20] H.
Wei, Y. Zhang, E. Gibbs, N. K. Chen, N. Wang, and C. Liu, “Joint 2D and 3D
phase processing for quantitative susceptibility mapping: application to 2D
echo-planar imaging,” NMR Biomed., vol. 30, no. 4, Apr. 2017, doi:
10.1002/nbm.3501.
[21] “Fast
nonlinear susceptibility inversion with variational regularization - Milovic -
2018 - Magnetic Resonance in Medicine - Wiley Online Library.” https://onlinelibrary.wiley.com/doi/10.1002/mrm.27073
(accessed Nov. 07, 2022).
[22] K.
J. Friston, A. P. Holmes, K. J. Worsley, J.-P. Poline, C. D. Frith, and R. S.
J. Frackowiak, “Statistical parametric maps in functional imaging: A general
linear approach,” Hum. Brain Mapp., vol. 2, no. 4, pp. 189–210, 1994,
doi: 10.1002/hbm.460020402.
[23] J.
Ashburner, “SPM: A history,” NeuroImage, vol. 62, no. 2, pp. 791–800,
Aug. 2012, doi: 10.1016/j.neuroimage.2011.10.025.
[24] M.
K. Chung, “Gaussian kernel smoothing.” arXiv, Nov. 29, 2021. doi:
10.48550/arXiv.2007.09539.