| Literature DB >> 34310719 |
M Edalati1,2, M Mahmoudzadeh1,3, J Safaie2, F Wallois1,3, S Moghimi1,2,3.
Abstract
Rhythm processing involves building expectations according to the hierarchical temporal structure of auditory events. Although rhythm processing has been addressed in the context of predictive coding, the properties of the oscillatory response in different cortical areas are still not clear. We explored the oscillatory properties of the neural response to rhythmic incongruence and the cross-frequency coupling between multiple frequencies to further investigate the mechanisms underlying rhythm perception. We designed an experiment to investigate the neural response to rhythmic deviations in which the tone either arrived earlier than expected or the tone in the same metrical position was omitted. These two manipulations modulate the rhythmic structure differently, with the former creating a larger violation of the general structure of the musical stimulus than the latter. Both deviations resulted in an MMN response, whereas only the rhythmic deviant resulted in a subsequent P3a. Rhythmic deviants due to the early occurrence of a tone, but not omission deviants, seemed to elicit a late high gamma response (60-80 Hz) at the end of the P3a over the left frontal region, which, interestingly, correlated with the P3a amplitude over the same region and was also nested in theta oscillations. The timing of the elicited high-frequency gamma oscillations related to rhythmic deviation suggests that it might be related to the update of the predictive neural model, corresponding to the temporal structure of the events in higher-level cortical areas.Entities:
Keywords: event-related potential; mismatch negativity; phase-amplitude coupling; prediction error; predictive coding
Mesh:
Year: 2021 PMID: 34310719 PMCID: PMC9285090 DOI: 10.1111/psyp.13909
Source DB: PubMed Journal: Psychophysiology ISSN: 0048-5772 Impact factor: 4.348
FIGURE 1(a) The Experimental protocol. (b) The standard and deviant stimuli
FIGURE 2Event‐locked analysis of rhythm and omission conditions. The onset of the deviant chord was set to zero and the next trial started at 450 and 300 ms for the rhythm and omission conditions, respectively. For both conditions, the baseline was set to 250 to 450 ms from the onset of the first chord. (a) Grand average of ERP (‐SE) for the rhythm deviant condition, the control condition, and their difference over frontal and parietal clusters. (b) Same as (a) for the omission condition. Both rhythm and omission deviants elicited an MMN. However, a P3a followed the MMN for only the rhythm deviants. The black bars over the ERP figures represent the time intervals of significant difference between the deviant and control conditions (p < .05, corrected, marked according to cluster‐based permutation analysis). The topography of each significant time window is shown in the boxes: above for the MMN corresponding to the rhythm and omission deviant conditions and below for the P3a in the rhythm and omission (not significant) deviant condition
FIGURE 3Event‐locked analysis of the rhythm and omission deviant conditions. The average TFR locked to the beginning of the rhythm deviant (a) and omission deviant (b) trials. The corresponding ERP of the ROI is superimposed on each TFR to better illustrate the results. The statistically significant changes from the control condition are indicated by a white contour. Rhythm deviant: low‐frequency cluster: 90 to 228 ms, p = .0008, corrected; high‐frequency cluster: 260 to 289 ms p = .0142, corrected. Omission deviant: low‐frequency cluster: 140 to 283 ms, p = .0002, corrected; high‐frequency cluster: 307 to 330 ms, p = .048, corrected. The figures below the high‐frequency TFRs show the uncorrected p values corresponding to the comparison between the deviant and control conditions (paired‐sample t test). The topographical distributions of the electrodes belonging to the significant low‐ and high‐frequency clusters are specified on the head map on top. The topographical distribution of the average power over the frequency and time window corresponding to each cluster is presented in the boxes (above for the low‐frequency and below for the high‐frequency TFR). (c) Comodulograms of phase‐amplitude coupling analysis over the 450‐ms window corresponding to the rhythm deviant condition. Comparison of the rhythm deviant condition with the control condition showed a single cluster with significant MI (p = .0318, corrected). (d) The difference between the rhythm deviant and control conditions in low‐frequency TFR, high‐frequency TFR, and time‐varying PAC over the time course of the rhythm deviant condition is shown. The significant cluster observed when comparing the two conditions is marked in all the three figures. The time‐varying PAC is presented as the mean ± SE