Hindmarsh J L, Rose R M
School of Mathematics, University of Wales College of Cardiff, U.K.
Philos Trans R Soc Lond B Biol Sci. 1994 Oct 29;346(1316):165-83. doi: 10.1098/rstb.1994.0139.
We add a slow hyperpolarization-activated inward current IH = gHmH (v-vH) to our previous model of rebound bursting (Hindmarsh & Rose Phil. Trans. R. Soc. Lond. B 346, 129-150 (1994a)) to give a four-dimensional physiological model, and a corresponding four-dimensional model of the model. The physiological model generates periodic 'bursts of bursts' or 'spindles' resembling those recorded experimentally in thalamocortical (TC) neurons. The model of the model is simplified to a two-dimensional system having a limit cycle which corresponds to the slow spindle oscillation of the physiological model. Analysis of the stability of this two-dimensional model allows us to divide the parameter space of the slope (gamma mH) and shift (theta mH) parameters of mH infinity (v) into regions in which the model generates spindles or continuous bursting. This enables us to determine the parameter values required for spindling in the physiological model and to explain the experimentally observed effects of noradrenaline. Next we examine whether a cell at a stable equilibrium point can be driven into spindling by applying a sinusoidal input at the resonant frequency. This is done by averaging the equations for the driven model of the model. Analysis of the stability of these averaged equations shows how the regions of the (theta mH, gamma mH) parameter space change when the system is driven by a sinusoidal input. This enables us to choose parameter values for a physiological model of a driven spindle. We show that if the physiological model is modified to include a voltage-dependent time constant for mH, spindles, similar to those of TC cells, can be obtained with a small Ca(2+)-activated K+ current. Finally our knowledge of the form of the bifurcation diagram and the conditions for resonance leads to a new suggestion for the roles of GABAA and GABAB inhibitory postsynaptic potentials when TC cells are driven into spindling by neurons of the nucleus reticularis thalami.
我们在之前的反弹爆发模型(Hindmarsh和Rose,《英国皇家学会会刊B》346卷,129 - 150页(1994a))中加入一个缓慢的超极化激活内向电流(I_H = g_Hm_H (v - v_H)),得到一个四维生理模型以及该模型对应的四维模型。生理模型产生周期性的“爆发簇”或“纺锤波”,类似于在丘脑皮质(TC)神经元中实验记录到的情况。该模型的模型被简化为一个二维系统,具有一个极限环,它对应于生理模型的缓慢纺锤波振荡。对这个二维模型稳定性的分析使我们能够将(m_H)无穷大((v))的斜率((\gamma m_H))和偏移((\theta m_H))参数的参数空间划分为模型产生纺锤波或持续爆发的区域。这使我们能够确定生理模型中产生纺锤波所需的参数值,并解释去甲肾上腺素的实验观察效应。接下来,我们研究处于稳定平衡点的细胞是否能通过在共振频率施加正弦输入而被驱动进入纺锤波状态。这是通过对模型的受驱模型方程进行平均来完成的。对这些平均方程稳定性的分析表明,当系统由正弦输入驱动时,((\theta m_H),(\gamma m_H))参数空间的区域如何变化。这使我们能够为受驱纺锤波的生理模型选择参数值。我们表明,如果生理模型被修改为包括(m_H)的电压依赖性时间常数,那么通过一个小的钙激活钾电流就可以获得类似于TC细胞的纺锤波。最后,我们对分岔图形式和共振条件的了解为丘脑网状核神经元驱动TC细胞进入纺锤波状态时GABAA和GABAB抑制性突触后电位的作用提出了一个新的建议。