The hidden heart rate in the slice-wise BOLD-fMRI global signal.
Michael Hütel1,2, Andrew Melbourne1, David L Thomas1,2, Jonathan Rohrer2, and Sebastien Ourselin1,2

1Translational Imaging Group, University College London, London, United Kingdom, 2Dementia Research Centre, University College London, London, United Kingdom

Synopsis

Previous studies have shown that slow variations in the cardiac cycle are coupled with signal changes in the blood-oxygen level dependent (BOLD) contrast. The detection of neurophysiological hemodynamic changes, driven by neuronal activity, is hampered by such physiological noise. It is therefore of great importance to model and remove these physiological artefacts. The cardiac cycle causes pulsatile arterial blood flow. This pulsation is translated into brain tissue and fluids bounded by the cranial cavity. We exploit this pulsality effect and provide evidence that the heart rate is inherent in BOLD fMRI images.

PURPOSE

Studies$$$^{1,2,3}$$$ have shown that a significant amount of BOLD signal variance is explained by the heart rate. This is further underpinned by the fact that cardiac regressors share variance with the global signal.$$$^2$$$However, it is still unclear how the heart rate exactly impacts BOLD fluctuations. For the first time, we provide evidence that the heart rate is inherent in BOLD-fMRI images.

METHODS

The cardiac cycle causes pulsatile arterial blood flow. This pulsation is translated into brain tissue and fluids bounded by the cranial cavity. We exploit this pulsality effect to obtain the heart rate hidden in the slice-wise global signal. To recover the heart rate, we rearrange all acquired BOLD slices depending on their acquisition time. We then average across all voxels that lie within the brain mask of a slice to obtain a signal sampled every slice rather than every volume. A short-window Fourier transform is applied to this slice-wise global signal to obtain the time-frequency spectrogram. We obtain the heart rate from this spectrogram by walking along frequency trajectories. A frequency trajectory is defined as a trajectory through the spectrogram that comprises exactly one frequency for each time point. The frequency trajectory that maximises the energy while traveling from time $$$t_1$$$ to $$$t_n$$$ is the wanted heart rate as depicted in Figure 1. To reduce the noise in the spectrogram, we apply a 1d-Gaussian filter ($$$\sigma^2=0.1$$$) and fit a Gaussian frequency mixture model to the power spectrum at each time point $$$t_i$$$. Examples of the resulting spectrograms are depicted in Figure 3, 4 and 5.

RESULTS

We tested our proposed heart rate extraction from the slice-wise global signal by comparing the obtained heart rate with pulse oximetry recordings in three resting-state fMRI cohorts. Cohort 1 comprises 108 subjects comparing term vs preterm individuals, average age 19 years, scanned on a Philips 3T Achieva (TR 3000ms, TE 30ms, flip angle 80$$$^{\circ}$$$, voxel size 2.5x2.5x3 mm, field of view (FoV) 240 mm$$$^2$$$, 50 oblique transverse slices, slice-order descending). Cohort 2 is a previously published open source data set$$$^4$$$ of 22 subjects, 4 scans per subject, average age 23 years, acquired on a Siemens MAGNETOM 7T (TR 3000ms, TE 17 ms, flip angle 70$$$^{\circ}$$$, voxel size 1.5mm isotropic, field of view (FoV) 192mm$$$^2$$$, 70 oblique transverse slices, slice-order interleaved). We excluded 5 scans because of a corrupted physiological recording or acquisition error.$$$^4$$$ Cohort 3 consists of 21 subjects that are part of a study looking at lifelong health and ageing, average age 69, acquired on a Siemens MAGNETOM 3T (TR 2020ms, TE 30ms, flip angle 75$$$^{\circ}$$$, voxel size 3x3x4 mm, field of view (FoV) 192 mm$$$^2$$$, 36 oblique transverse slices, slice-order interleaved). We projected motion realignment parameters, linear and quadratic trends out of all fMRI scans before obtaining the slice-wise global signal. We then bandpass-filtered (0.6-2Hz) the slice-wise global signal. First, we manually compared the spectrogram of the pulse oximetry recording with the spectrogram of the slice-wise global signal. We found traces of the heart rate in the slice-wise global signal in 98.15% (106/108) of cohort 1, in 100% (83/83) of cohort 2 and in 95.24% (20/21) of cohort 3. Our heuristic heart rate extraction algorithm achieved a median error (difference between extracted heart rate and heart rate from physiological recording) below 0.05Hz in 82.86% of cohort 1, 71.08% of cohort 2 and 47.63% of cohort 3 depicted in Figure 2. The identification of the heart rate in the slice-wise global signal by our algorithm was mainly compromised by artefacts due to large or periodic motion.

DISCUSSION

There is an ongoing debate about wether to use a global signal in resting-state fMRI preprocessing.$$$^{5,6}$$$ Projecting a global signal out of BOLD time series aims to remove non-neural effects that affect large numbers of voxels. However, since the global signal is an unknown mixture of neural and non-neural fluctuations, its removal will ultimately change inter-regional correlations and hamper their interpretation.$$$^2$$$

CONCLUSION

We have proven for the first time that the heart rate is inherent in the slice-wise global signal. We identified heart rate traces in BOLD-fMRI images across different scanners, sequences and population cohorts, and provide thus a way to circumvent the undesirable use of the global signal as noise regressor when physiological recordings are not available. Our finding proves that the heart rate affects many voxels, showing the importance of physiological monitoring in BOLD-fMRI. In future studies, we will investigate new physiological noise models that incorporate joint information from physiological recordings and the slice-wise global signal.

Acknowledgements

MH gratefully acknowledges the support of the UCL Leonard Wolfson Experimental Neurology Centre. We would also like to acknowledge the MRC (MR/J01107X/1), the National Institute for Health Research (NIHR), the EPSRC (EP/H046410/1) and the National Institute for Health Research University College London Hospitals Biomedical Research Centre (NIHR BRC UCLH/UCL High Impact Initiative- BW.mn.BRC10269). This work is supported by the EPSRC-funded UCL Centre for Doctoral Training in Medical Imaging (EP/L016478/1). The Dementia Research Centre is supported by Alzheimer’s Research UK, Brain Research Trust, and The Wolfson Foundation.

References

1. Shmueli, K., van Gelderen, P., de Zwart, J. A., Horovitz, S. G., Fukunaga, M., Jansma, J. M., & Duyn, J. H. (2007). Low-frequency fluctuations in the cardiac rate as a source of variance in the resting-state fMRI BOLD signal.Neuroimage, 38(2), 306-320.

2. Chang, C., & Glover, G. H. (2009). Effects of model-based physiological noise correction on default mode network anti-correlations and correlations.Neuroimage, 47(4), 1448-1459.

3. Chang, C., Cunningham, J. P., & Glover, G. H. (2009). Influence of heart rate on the BOLD signal: the cardiac response function. Neuroimage, 44(3), 857-869.

4. Gorgolewski, K. J., Mendes, N., Wilfling, D., Wladimirow, E., Gauthier, C. J., Bonnen, T., ... & Margulies, D. S. (2015). A high resolution 7-Tesla resting-state fMRI test-retest dataset with cognitive and physiological measures. Scientific data, 2.

5. Murphy, K., Birn, R. M., & Bandettini, P. A. (2013). Resting-state fMRI confounds and cleanup. Neuroimage, 80, 349-359.

6. Murphy, K., Birn, R. M., Handwerker, D. A., Jones, T. B., & Bandettini, P. A. (2009). The impact of global signal regression on resting state correlations: are anti-correlated networks introduced?. Neuroimage, 44(3), 893-905.

Figures

Fig. 1: Subjects acquired on a Siemens 7T, Siemens 3T and Philips 3T (TR 3s, 2.02s and 3s, respectively). The pulse oximetry signal was acquired at the individual physiological monitoring units (A,C,E). A short-time window (60s) Fourier transform was used to compute the time-frequency spectrogram of individual pulse ox. signals. The slice-wise time-frequency spectrogram (B,D,F) from the respective BOLD fMRI scans resembles the change in heart rate seen in (A,C,E).

Fig. 2: The summary statistic of the difference between the extracted heart rate from the slice-wise global signal and the heart rate from pulse oximetry (sorted by median error).

Fig. 3: Comparison of two Siemens 7T scans. The first row depicts a scan in which the heart rate in the slice-wise global signal almost perfectly matches with the heart rate of the pulse ox. recording. The second row shows a scan in which the identification of the heart rate is hindered by periodic motion.

Fig. 4: Comparison of two Philips 3T scans. The heart rate can be determined by examining the slice-wise global signal in first scan (first row), whereas periodic motion corrupts the heart rate in the slice-wise signal of the second scan (second row).

Fig. 5: Comparison of two Siemens 3T scans. Both heart rate signals show high correlation in the first scan (first row). The identification of the heart rate is again hampered by spontaneous occurring motion in the second scan (second row).



Proc. Intl. Soc. Mag. Reson. Med. 24 (2016)
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