IISc Mathematics Initiative, Department of Mathematics, Indian Institute of Science, C V Raman road, Bangalore 560012, Karnataka, India.
Centre for Neuroscience, Indian Institute of Science, C V Raman road, Bangalore 560012, Karnataka, India.
Cereb Cortex. 2023 Sep 9;33(18):10108-10121. doi: 10.1093/cercor/bhad270.
Gamma rhythm refers to oscillatory neural activity between 30 and 80 Hz, induced in visual cortex by stimuli such as iso-luminant hues or gratings. The power and peak frequency of gamma depend on the properties of the stimulus such as size and contrast. Gamma waveform is typically arch-shaped, with narrow troughs and broad peaks, and can be replicated in a self-oscillating Wilson-Cowan (WC) model operating in an appropriate regime. However, oscillations in this model are infinitely long, unlike physiological gamma that occurs in short bursts. Further, unlike the model, gamma is faster after stimulus onset and slows down over time. Here, we first characterized gamma burst duration in local field potential data recorded from two monkeys as they viewed full screen iso-luminant hues. We then added different types of noise in the inputs to the WC model and tested how that affected duration and temporal dynamics of gamma. While the model failed with the often-used Poisson noise, Ornstein-Uhlenbeck noise applied to both the excitatory and the inhibitory populations replicated the duration and slowing of gamma and replicated the shape and stimulus dependencies. Thus, the temporal dynamics of gamma oscillations put constraints on the type and properties of underlying neural noise.
伽马节律是指视觉皮层中由等亮度色调或光栅等刺激引起的 30 至 80 Hz 的振荡神经活动。伽马的功率和峰值频率取决于刺激的特性,如大小和对比度。伽马波通常呈拱形,有狭窄的波谷和宽阔的波峰,可以在适当的条件下在自激威尔逊-考恩(WC)模型中复制。然而,与生理伽马不同,这种模型中的振荡是无限长的,而生理伽马是在短时间内爆发的。此外,与模型不同的是,伽马在刺激开始后会更快,并随着时间的推移而减慢。在这里,我们首先在两只猴子观看全屏幕等亮度色调时记录的局部场电位数据中描述了伽马爆发持续时间。然后,我们在 WC 模型的输入中添加了不同类型的噪声,并测试了这如何影响伽马的持续时间和时间动态。虽然模型在经常使用的泊松噪声下失败了,但应用于兴奋性和抑制性群体的奥恩斯坦-乌伦贝克噪声复制了伽马的持续时间和减缓,并复制了形状和刺激依赖性。因此,伽马振荡的时间动态对潜在神经噪声的类型和特性施加了限制。