Komendantov Alexander O, Canavier Carmen C
Department of Psychology, University of New Orleans, New Orleans, LA 70148, USA.
J Neurophysiol. 2002 Mar;87(3):1526-41. doi: 10.1152/jn.00255.2001.
The role of gap junctions between midbrain dopamine (DA) neurons in mechanisms of firing pattern generation and synchronization has not been well characterized experimentally. We modified a multi-compartment model of DA neuron by adding a spike-generating mechanism and electrically coupling the dendrites of two such neurons through gap junctions. The burst-generating mechanism in the model neuron results from the interaction of a N-methyl-D-aspartate (NMDA)-induced current and the sodium pump. The firing patterns exhibited by the two model neurons included low frequency (2-7 Hz) spiking, high-frequency (13-20 Hz) spiking, irregular spiking, regular bursting, irregular bursting, and leader/follower bursting, depending on the parameter values used for the permeability for NMDA-induced current and the conductance for electrical coupling. All of these firing patterns have been observed in physiological neurons, but a systematic dependence of the firing pattern on the covariation of these two parameters has not been established experimentally. Our simulations indicate that electrical coupling facilitates NMDA-induced burst firing via two mechanisms. The first can be observed in a pair of identical cells. At low frequencies (low NMDA), as coupling strength was increased, only a transition from asynchronous to synchronous single-spike firing was observed. At high frequencies (high NMDA), increasing the strength of the electrical coupling in an identical pair resulted in a transition from high-frequency single-spike firing to burst firing, and further increases led to synchronous high-frequency spiking. Weak electrical coupling destabilizes the synchronous solution of the fast spiking subsystems, and in the presence of a slowly varying sodium concentration, the desynchronized spiking solution leads to bursts that are approximately in phase with spikes that are not in phase. Thus this transitional mechanism depends critically on action potential dynamics. The second mechanism for the induction of burst firing requires a heterogeneous pair that is, respectively, too depolarized and too hyperpolarized to burst. The net effect of the coupling is to bias at least one cell into an endogenously burst firing regime. In this case, action potential dynamics are not critical to the transitional mechanism. If electrical coupling is indeed more prominent in vivo due to basal level of modulation of gap junctions in vivo, these results may indicate why NMDA-induced burst firing is easier to observe in vivo as compared in vitro.
中脑多巴胺(DA)神经元之间的缝隙连接在放电模式产生和同步机制中的作用尚未通过实验得到充分表征。我们通过添加一个产生动作电位的机制,并通过缝隙连接将两个这样的神经元的树突进行电耦合,对DA神经元的多房室模型进行了修改。模型神经元中的爆发产生机制源于N-甲基-D-天冬氨酸(NMDA)诱导电流与钠泵的相互作用。两个模型神经元表现出的放电模式包括低频(2 - 7赫兹)放电、高频(13 - 20赫兹)放电、不规则放电、规则爆发、不规则爆发以及主/从爆发,这取决于用于NMDA诱导电流的通透性和电耦合电导的参数值。所有这些放电模式在生理神经元中都已被观察到,但放电模式对这两个参数协变的系统依赖性尚未通过实验确定。我们的模拟表明,电耦合通过两种机制促进NMDA诱导的爆发式放电。第一种机制可以在一对相同的细胞中观察到。在低频(低NMDA)时,随着耦合强度增加,仅观察到从异步单峰放电到同步单峰放电的转变。在高频(高NMDA)时,增加相同细胞对中的电耦合强度会导致从高频单峰放电到爆发式放电的转变,进一步增加会导致同步高频放电。弱电耦合会使快速放电子系统的同步解变得不稳定,并且在存在缓慢变化的钠浓度的情况下,去同步化的放电解会导致与不同步的峰电位大致同相的爆发。因此,这种转变机制关键取决于动作电位动力学。诱导爆发式放电的第二种机制需要一对异质性细胞,即一个细胞过度去极化而另一个过度超极化以至于无法爆发。耦合的净效应是使至少一个细胞偏向内源性爆发式放电脑。在这种情况下,动作电位动力学对转变机制并不关键。如果由于体内缝隙连接的基础调节水平,电耦合在体内确实更为显著,那么这些结果可能表明为什么与体外相比,NMDA诱导的爆发式放电在体内更容易被观察到。