Berger Sandra D, Crook Sharon M
School of Life Sciences, Arizona State University Tempe, AZ, USA.
School of Life Sciences, Arizona State University Tempe, AZ, USA ; School of Mathematical and Statistical Sciences, Arizona State University Tempe, AZ, USA.
Front Comput Neurosci. 2015 Nov 18;9:139. doi: 10.3389/fncom.2015.00139. eCollection 2015.
Voltage gated ion channels play a major role in determining a neuron's firing behavior, resulting in the specific processing of synaptic input patterns. Drosophila and other invertebrates provide valuable model systems for investigating ion channel kinetics and their impact on firing properties. Despite the increasing importance of Drosophila as a model system, few computational models of its ion channel kinetics have been developed. In this study, experimentally observed biophysical properties of voltage gated ion channels from the fruitfly Drosophila melanogaster are used to develop a minimal, conductance based neuron model. We investigate the impact of the densities of these channels on the excitability of the model neuron. Changing the channel densities reproduces different in situ observed firing patterns and induces a switch from integrator to resonator properties. Further, we analyze the preference to input frequency and how it depends on the channel densities and the resulting bifurcation type the system undergoes. An extension to a three dimensional model demonstrates that the inactivation kinetics of the sodium channels play an important role, allowing for firing patterns with a delayed first spike and subsequent high frequency firing as often observed in invertebrates, without altering the kinetics of the delayed rectifier current.
电压门控离子通道在决定神经元的放电行为中起主要作用,从而导致突触输入模式的特定处理。果蝇和其他无脊椎动物为研究离子通道动力学及其对放电特性的影响提供了有价值的模型系统。尽管果蝇作为模型系统的重要性日益增加,但针对其离子通道动力学的计算模型却很少被开发出来。在本研究中,利用从果蝇黑腹果蝇实验观察到的电压门控离子通道的生物物理特性,开发了一个基于电导的最小神经元模型。我们研究了这些通道的密度对模型神经元兴奋性的影响。改变通道密度可重现不同的原位观察到的放电模式,并诱导从积分器特性到谐振器特性的转变。此外,我们分析了对输入频率的偏好以及它如何依赖于通道密度和系统所经历的分叉类型。扩展到三维模型表明,钠通道的失活动力学起着重要作用,允许出现如在无脊椎动物中经常观察到的具有延迟的第一个尖峰和随后高频放电的放电模式,而无需改变延迟整流电流的动力学。