We analyze the structure of physiological noise in the $$$k$$$-space of BOLD fMRI. We use DRIFTER which is an algorithm based on optimal Bayesian smoothing techniques for separation of the fMRI signal to a BOLD signal component and physiological noises. DRIFTER is run independently for each spatial frequency and it is shown that the physiological noise lies in the $$$k$$$-space points with low spatial frequency and that its amplitude is proportional to the BOLD signal. This result suggests that we can lower the computational burden without losing estimation accuracy by running DRIFTER only on a subset of $$$k$$$-space points.
Structured non-white noise resulting from cardiac and respiratory activity can account for over a third of the total standard deviation in BOLD fMRI1, making proper treatment of these noise sources an essential part in enhancing the signal-to-noise ratio2. Removal of the structural noise is typically done retrospectively from the reconstructed images3,4, but it has been demonstrated5 that working directly with the raw $$$k$$$-space data is possible and can result to more accurate noise estimates. In this work, we investigate the $$$k$$$-space structure of the physiological noise, as estimated by the DRIFTER algorithm3. Knowing this spatial distribution is important as such, but it can also be used for reducing the computational burden of the DRIFTER algorithm—as the DRIFTER processes each spatial frequency independently and most of the energy is concentrated to low frequencies, we can save computations by only processing a subset of the $$$k$$$-space.
The DRIFTER algorithm is a retrospective estimation scheme for identification and removal of physiological noise in fMRI data. It is based on Bayesian optimal filtering and smoothing methods from signal processing. The algorithm decomposes the data into different noise components and the “cleaned” BOLD signal. In this work we apply DRIFTER to raw $$$k$$$-space data. After this we select spatial frequencies that contain most of the energy and process only these. This kind of subset processing is only possible in $$$k$$$-space whereas processing only some of the image space voxels would make little sense. Specifically, we use DRIFTER to compute the overall physiological noise distribution in the $$$k$$$-space and then investigate how the reconstructed images are affected if only the those spatial frequencies containing 90% or 50% of the total physiological noise energy are processed further. The actual image reconstruction is done with Kaiser–Bessel regridding6 and by weighting by the complete coil images when summing over the coil channels.
The test data consists of a 27-run set of raw resting state fMRI data and accompanying anatomical images of one volunteer. The data was obtained at Aalto AMI Centre of Aalto NeuroImaging, part of Aalto University School of Science, with a 3 T Siemens Skyra scanner using a 32-channel receive-only head-coil array. Parameters of the EPI sequence were TR: 77 ms; TE: 21 ms; FA: 60 degrees; FOV: 224 mm; matrix size: 64$$$\times$$$64; voxel size: 3.5$$$\times$$$3.5$$$\times$$$6 mm, and those of the EPI trajectory were ramp times: 140 $$$\mu$$$s; flat-top: 220 $$$\mu$$$s; ADC readout time: 409.6 $$$\mu$$$s. Each run had a length of approximately 30 seconds and consisted of a fixed reference slice and a second slice with the gap size between them advancing on each run. The reference cardiac and respiration signals were time-locked to the fMRI data with a peripheral (BIOPAC) pulse measure and a respiratory belt, respectively. The physiological signals were sampled with a frequency of 1 kHz. For the DRIFTER algorithm, two harmonic resonators were used with their frequencies for each run estimated from external cardiac and respiration signals.
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7. DRIFTER TOOLBOX: An SPM toolbox for removing periodic noise in fMRI data. http://becs.aalto.fi/en/research/bayes/drifter/. Accessed November 4, 2016.