Due to weak amplitude and fast oscillation, it is still controversial whether neuronal activities can be directly detected through MR imaging. In this study, we propose a novel method, multiple‑TR approach, which utilized 1) multi-phase acquisition and 2) frequency spectrum multiplication for detecting weak and fast oscillating magnetic fields. We demonstrated with phantom experiments that SNR at the stimulation frequency on the spectrum was remarkably enhanced with the higher number of TRs under almost the same scan time, amplifying oscillation frequency component while suppressing systematic noises. This proposed approach will increase possibility of directly detecting neural oscillations in vivo.
All experiments were performed on a 3 Tesla MRS 3000 scanner (MR solutions) and data were analyzed with MATLAB (The Mathworks, USA). The single-shot gradient-echo echo-planar imaging (GE-EPI) sequence was used for fast imaging and the scan parameters were as follows: FOV= 50×50 mm2, matrix= 64×64, flip angle= 10°, TE= 20ms, TR= 90, 91, 92, 93, 94, 95, 96, and 97 ms (total 8 TRs). A 26-gauge copper wire was wound around a phantom tube filled with distilled water and electrical stimulation was given with specific frequencies to form the oscillating magnetic field within the current loop (Fig. 2a,b). Phantom experiments were conducted with two different amplitudes of magnetic field calculated by Biot-Savart law (1nT/5nT) and two different stimulation frequencies (3Hz/25Hz). For multiple-TR analysis, the data acquired with eight different TRs were resampled with new sampling periods(Tsamp) which can be calculated by difference between the period of stimulation frequency(Tstim) and MRI temporal resolution (Tsamp=TR-n×Tstim, n is interger). The resampled data could be pixel-by-pixel 1-D Fourier transformed along dynamic scans with the range of [-1/(2Tsamp), 1/(2Tsamp)]. The linear interpolations were performed on the remaining seven frequency spectra based on the longest Tsamp spectrum to match the position of stimulation frequencies. By multiplying these eight frequency spectra, the amplitude of stimulation components is strengthened while the amplitudes of systematic noise components are suppressed so that pronounced peak can be obtained at the stimulation frequency (Fig. 1). For an obvious comparison between the two-TR analysis and the proposed multiple TR analysis, the total number of dynamic scans (i.e., total scan time) remained the same (Fig. 4a). The signal-to-noise ratio (SNR) was calculated from ROI-average absolute frequency spectrum formed by each multiple TR multiplication data. It was also analyzed by different number of dynamic scans and various frequencies (7Hz, 17Hz, 25Hz) on eight-TR analysis.
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