Qian Kun, Yu Na, Tucker Kristal R, Levitan Edwin S, Canavier Carmen C
Department of Cell Biology and Anatomy, Louisiana State University School of Medicine, New Orleans, Louisiana; Neuroscience Center of Excellence, Louisiana State University School of Medicine, New Orleans, Louisiana; and.
Department of Cell Biology and Anatomy, Louisiana State University School of Medicine, New Orleans, Louisiana;
J Neurophysiol. 2014 Dec 1;112(11):2779-90. doi: 10.1152/jn.00578.2014. Epub 2014 Sep 3.
Dopamine neurons in freely moving rats often fire behaviorally relevant high-frequency bursts, but depolarization block limits the maximum steady firing rate of dopamine neurons in vitro to ∼10 Hz. Using a reduced model that faithfully reproduces the sodium current measured in these neurons, we show that adding an additional slow component of sodium channel inactivation, recently observed in these neurons, qualitatively changes in two different ways how the model enters into depolarization block. First, the slow time course of inactivation allows multiple spikes to be elicited during a strong depolarization prior to entry into depolarization block. Second, depolarization block occurs near or below the spike threshold, which ranges from -45 to -30 mV in vitro, because the additional slow component of inactivation negates the sodium window current. In the absence of the additional slow component of inactivation, this window current produces an N-shaped steady-state current-voltage (I-V) curve that prevents depolarization block in the experimentally observed voltage range near -40 mV. The time constant of recovery from slow inactivation during the interspike interval limits the maximum steady firing rate observed prior to entry into depolarization block. These qualitative features of the entry into depolarization block can be reversed experimentally by replacing the native sodium conductance with a virtual conductance lacking the slow component of inactivation. We show that the activation of NMDA and AMPA receptors can affect bursting and depolarization block in different ways, depending upon their relative contributions to depolarization versus to the total linear/nonlinear conductance.
自由活动大鼠的多巴胺神经元通常会产生与行为相关的高频爆发式放电,但去极化阻滞将体外多巴胺神经元的最大稳定放电频率限制在约10赫兹。我们使用一个能忠实地再现这些神经元中测量到的钠电流的简化模型,发现添加最近在这些神经元中观察到的钠通道失活的另一个慢成分,会以两种不同方式定性地改变模型进入去极化阻滞的方式。首先,失活的慢时间进程允许在进入去极化阻滞之前的强去极化期间引发多个动作电位。其次,去极化阻滞发生在动作电位阈值附近或以下(体外阈值范围为-45至-30毫伏),因为额外的失活慢成分抵消了钠窗电流。在没有额外的失活慢成分时,这种窗电流产生一个N形的稳态电流-电压(I-V)曲线,从而在实验观察到的接近-40毫伏的电压范围内防止去极化阻滞。动作电位间隔期间从慢失活恢复的时间常数限制了进入去极化阻滞之前观察到的最大稳定放电频率。通过用缺乏失活慢成分的虚拟电导替代天然钠电导,实验上可以逆转进入去极化阻滞的这些定性特征。我们表明,NMDA和AMPA受体的激活可以以不同方式影响爆发式放电和去极化阻滞,这取决于它们对去极化与总线性/非线性电导的相对贡献。