Phase Response Curves to Measure Ion Channel Effects on Neurons

In this chapter, we explore how different common ionic currents change the shape of the PRC using several well-known conductance-based models. By also studying the simplest possible network – two pulse coupled neural oscillators – we can use the shape of the PRC to quantify the degree of synchrony in such a pair. We find a number of qualitative effects that include changing the sign of the PRC during certain phases and altering the skew of the PRC. Using bifurcation theory, we trace these effects back to the underlying dynamics that govern the onset of repetitive firing as the neuron is depolarized by a constant current. The key bifurcation involves the so-called Takens-Bogdanov bifurcation. We show that many of the shape changes of the PRC can be understood by examining the dynamics of the neuron near this bifurcation.

[1]  V. Crunelli,et al.  A TASK3 channel (KCNK9) mutation in a genetic model of absence epilepsy , 2007, Journal of Molecular Neuroscience.

[2]  K. Lehnertz,et al.  Synchronization phenomena in human epileptic brain networks , 2009, Journal of Neuroscience Methods.

[3]  Ivan Soltesz,et al.  Persistently modified h-channels after complex febrile seizures convert the seizure-induced enhancement of inhibition to hyperexcitability , 2001, Nature Medicine.

[4]  Charles J. Wilson,et al.  Response properties and synchronization of rhythmically firing dendritic neurons. , 2007, Journal of neurophysiology.

[5]  S. Schiff,et al.  Decreased Neuronal Synchronization during Experimental Seizures , 2002, The Journal of Neuroscience.

[6]  W. Singer,et al.  Neural Synchrony in Brain Disorders: Relevance for Cognitive Dysfunctions and Pathophysiology , 2006, Neuron.

[7]  Charles M. Gray,et al.  Synchronous oscillations in neuronal systems: Mechanisms and functions , 1994, Journal of Computational Neuroscience.

[8]  D. McCormick,et al.  On the cellular and network bases of epileptic seizures. , 2001, Annual review of physiology.

[9]  Germán Mato,et al.  Electrical Synapses and Synchrony: The Role of Intrinsic Currents , 2003, The Journal of Neuroscience.

[10]  G. Ermentrout,et al.  Phase-response curves give the responses of neurons to transient inputs. , 2005, Journal of neurophysiology.

[11]  B. Hille,et al.  Ionic channels of excitable membranes , 2001 .

[12]  Eric Shea-Brown,et al.  On the Phase Reduction and Response Dynamics of Neural Oscillator Populations , 2004, Neural Computation.

[13]  J. Dostrovsky,et al.  Neuronal Oscillations in the Basal Ganglia and Movement Disorders: Evidence from Whole Animal and Human Recordings , 2004, The Journal of Neuroscience.

[14]  G. Buzsáki,et al.  High-Frequency Oscillations in the Output Networks of the Hippocampal–Entorhinal Axis of the Freely Behaving Rat , 1996, The Journal of Neuroscience.

[15]  Eugene M. Izhikevich,et al.  Dynamical Systems in Neuroscience: The Geometry of Excitability and Bursting , 2006 .

[16]  L. Annunziato,et al.  Atypical Gating Of M-Type Potassium Channels Conferred by Mutations in Uncharged Residues in the S4 Region of KCNQ2 Causing Benign Familial Neonatal Convulsions , 2007, The Journal of Neuroscience.

[17]  Boris S. Gutkin,et al.  The effects of cholinergic neuromodulation on neuronal phase-response curves of modeled cortical neurons , 2009, Journal of Computational Neuroscience.

[18]  B. McNaughton,et al.  Theta phase precession in hippocampal neuronal populations and the compression of temporal sequences , 1996, Hippocampus.

[19]  Boris S. Gutkin,et al.  The Effects of Spike Frequency Adaptation and Negative Feedback on the Synchronization of Neural Oscillators , 2001, Neural Computation.

[20]  G. Ermentrout,et al.  Synchrony, stability, and firing patterns in pulse-coupled oscillators , 2002 .

[21]  John Rinzel,et al.  Analysis of bursting in a thalamic neuron model , 1994, Biological Cybernetics.

[22]  M. Lazdunski,et al.  Inhalational anesthetics activate two-pore-domain background K+ channels , 1999, Nature Neuroscience.

[23]  G. Buzsáki,et al.  Gamma Oscillations in the Entorhinal Cortex of the Freely Behaving Rat , 1998, The Journal of Neuroscience.

[24]  A. Reyes,et al.  Effects of transient depolarizing potentials on the firing rate of cat neocortical neurons. , 1993, Journal of neurophysiology.

[25]  Haim Sompolinsky,et al.  Chaos and synchrony in a model of a hypercolumn in visual cortex , 1996, Journal of Computational Neuroscience.

[26]  T. Sejnowski,et al.  Cholinergic Neuromodulation Changes Phase Response Curve Shape and Type in Cortical Pyramidal Neurons , 2008, PloS one.

[27]  G. Ermentrout,et al.  Analysis of neural excitability and oscillations , 1989 .

[28]  D. Johnston,et al.  Seizure-Induced Plasticity of h Channels in Entorhinal Cortical Layer III Pyramidal Neurons , 2004, Neuron.

[29]  G Bard Ermentrout,et al.  Class-II neurons display a higher degree of stochastic synchronization than class-I neurons. , 2008, Physical review. E, Statistical, nonlinear, and soft matter physics.

[30]  Bard Ermentrout,et al.  Type-II phase resetting curve is optimal for stochastic synchrony. , 2009, Physical review. E, Statistical, nonlinear, and soft matter physics.

[31]  John R. Huguenard,et al.  Thalamic synchrony and dynamic regulation of global forebrain oscillations , 2007, Trends in Neurosciences.

[32]  M. Avoli,et al.  Physiology and pharmacology of epileptiform activity induced by 4-aminopyridine in rat hippocampal slices. , 1991, Journal of neurophysiology.

[33]  Y. Amitai,et al.  Propagating neuronal discharges in neocortical slices: computational and experimental study. , 1997, Journal of neurophysiology.

[34]  Michael A. Rogawski,et al.  Molecular targets for antiepileptic drug development , 2011, Neurotherapeutics.