ABSTRACT
Synaptic plasticity is usually considered as the main form of activity-dependent functional plasticity in the mammalian brain. Short- and long-term regulation of synaptic transmission have been shown in various types of excitatory synapses including cortical and hippocampal synapses. In this review, we discuss a novel form of non-synaptic plasticity that involves voltage-gated K+ conductances in CA3 pyramidal cell axons. With experimental and theoretical arguments, we show that axons cannot only be considered as a simple structure that transmit reliably the action potential (AP) from the cell body to the nerve terminals. The axon is also able to express conduction failures in specific axonal pathways. We discuss possible physiological conditions in which these axonal plasticity may occur and its incidence on hippocampal network properties.
Subject(s)
Action Potentials/physiology , Axons/physiology , Hippocampus/physiology , Ion Channel Gating/physiology , Neural Conduction/physiology , Neuronal Plasticity/physiology , Potassium Channels/physiology , Animals , Humans , Models, NeurologicalABSTRACT
A model of CA3 pyramidal cell axons was used to study a new mode of gating of action potential (AP) propagation along the axon that depends on the activation of A-type K+ current (Debanne et al., 1997). The axonal membrane contained voltage-dependent Na+ channels, K+ channels, and A-type K+ channels. The density of axonal A-channels was first determined so that (1) at the resting membrane potential an AP elicited by a somatic depolarization was propagated into all axon collaterals and (2) propagation failures occurred when a brief somatic hyperpolarization preceded the AP induction. Both conditions were fulfilled only when A-channels were distributed in clusters but not when they were homogeneously distributed along the axon. Failure occurs in the proximal part of the axon. Conduction failure could be determined by a single cluster of A-channels, local decrease of axon diameter, or axonal elongation. We estimated the amplitude and temporal parameters of the hyperpolarization required for induction of a conduction block. Transient and small somatic hyperpolarizations, such as simulated GABAA inhibitory postsynaptic potentials, were able to block the AP propagation. It was shown that AP induction had to occur with a short delay (<30 msec) after the hyperpolarization. We discuss the possible conditions in which such local variations of the axon geometry and A-channel density may occur and the incidence of AP propagation failures on hippocampal network properties.
Subject(s)
Axons/physiology , Computer Simulation , Ion Channel Gating/physiology , Models, Neurological , Potassium Channels/physiology , Pyramidal Cells/physiology , Action Potentials/physiology , Animals , Axons/chemistry , Excitatory Postsynaptic Potentials/physiology , Hippocampus/cytology , Kinetics , Neural Conduction/physiology , Neural Inhibition/physiology , Neuronal Plasticity/physiology , Pyramidal Cells/chemistry , Pyramidal Cells/ultrastructure , Receptors, GABA-A/physiology , Sodium Channels/physiologyABSTRACT
Intracellular recording of abducens motoneurons in vivo has shown that ionophoretic applications of N-methyl-D-aspartate produced long-lasting membrane potential oscillations including a slow depolarization plateau with a burst of fast action potentials. This complex N-methyl-D-aspartate pattern was reproduced in the model of abducens motoneuron in vivo identified, intracellularly stained with horseradish peroxidase and reconstructed at high spatial resolution. The excitable soma of the simulated cell contained voltage-gated Ca, Na and K conductances, N-methyl-D-aspartate-gated voltage-sensitive Ca-Na-K conductance and Ca-dependent K conductance. The dendrite was passive either completely or with the exception of branching nodes containing N-methyl-D-aspartate conductances of the same slow kinetics but of lower values than at the soma. In the completely passive case, the N-methyl-D-aspartate pattern decayed with different rates along different dendritic paths depending on the geometry and topology of the reconstructed dendrite. The branches formed four clusters discriminated in somatofugal attenuations of steady voltages, and were correspondingly discriminated in attenuation of the complex N-methyl-D-aspartate pattern. Fast spikes decayed more than the slow depolarization plateau so that the prevalence of slow over fast components in the transformed pattern increased with somatofugal path distance. As a consequence, the lower the electrotonic effectiveness of a branch in the cluster or in the whole arborization, the lower both the voltage level and the frequency range of its voltage modulation by N-methyl-D-aspartate oscillations. In the case of active branching points, the somatic pattern changed depending on the level of activation of dendritic N-methyl-D-aspartate conductances with slow kinetics of voltage sensitivity. The higher this level, the longer the plateau and burst, and the greater the discharge rate; and the spikes in the burst were smaller. When the pattern spread in the dendrite, the fast spikes decayed and the slow plateau was boosted, with a greater effect along the somatofugal path containing more branching points. These results show how the somatofugal back-invasion along the dendrites by activity patterns generated at the soma can tune voltage-sensitive dendritic conductances. The dendritic back-invasion is geometry- and topology-dependent. It is proposed as a subtle feedback mechanism for the neuron to control its own synaptic inputs.
Subject(s)
Dendrites/physiology , Models, Neurological , Motor Neurons/physiology , Muscle, Skeletal/innervation , N-Methylaspartate/pharmacology , Action Potentials/drug effects , Animals , Computer Simulation , Dendrites/drug effects , Ion Channel Gating , Ion Channels/physiology , Membrane Potentials/drug effects , Motor Neurons/drug effects , Oscillometry , Time FactorsABSTRACT
1. In vivo experiments have shown that extracellular microelectrophoretic application of N-methyl-D-aspartate (NMDA) induced oscillatory plateau potentials with bursts of action potentials in rat abducens motoneurons. The period of these slow NMDA oscillations could be altered by single trigeminal non-NMDA excitatory input delivered at low frequency during the NMDA oscillations. 2. A resetting of the oscillations was observed depending on the phase of slow oscillatory cycle during which the trigeminal excitation occurred. 3. We investigated local mechanisms responsible for the phase-dependent modifications of NMDA oscillations, including contributions of voltage and concentration transients, in the mathematical model of the isopotential membrane compartment equipped with voltage-gated Na+, K+, and Ca2+ channels, with Ca2+-dependent K+ channels, and with ligand-gated NMDA and alpha-amino-3-hydroxy-5-methyl-4-isoxazolepropionic acid (AMPA) receptor channels. The faithful model was constructed with the use of models described earlier, which were modified by increasing time constants of kinetic variables of all voltage-gated conductances and by including coupled dynamics of voltages and ion concentrations. The changes in ion concentrations were produced near the membrane by transmembrane currents and removal mechanisms (pumps, diffusion). 4. This work focuses on local arrangement of voltage- and ligand-gated conductances and on local ion concentration changes in two separate pools: the postsynaptic pool of AMPA receptors and the extrasynaptic pool. In terms of the electrotonic and diffusional length constants, these pools were electrotonically close but diffusionally remote. 5. It was found that the effect of resetting can be produced by a local interaction between plateau and spike-generating conductances and glutamate receptors. 6. In vivo phase-dependent interactions between NMDA oscillations and AMPA synaptic input were reproduced by the local model only when changes in intracellular sodium and extracellular potassium concentrations were taken into account and the mechanisms of ion removal from postsynaptic pools had slower kinetics than the fast pump system operating in the extracellular pool. 7. Postsynaptic changes in ion concentrations of Na+ and K+ in intra- and extracellular layers near the membrane shift of Nernst equilibrium potentials for these ions depending on the phase of activation of synaptic input. Thus Na+ and k+ components of all transmembrane currents involved in the pattern generation are differently affected by synaptic action during the oscillations. We conclude that slow postsynaptic changes in ion concentrations near the membrane play a key role in the resetting of the NMDA oscillations.
Subject(s)
Abducens Nerve/physiology , Motor Neurons/physiology , N-Methylaspartate/physiology , Synapses/physiology , Abducens Nerve/cytology , Abducens Nerve/drug effects , Action Potentials/drug effects , Action Potentials/physiology , Animals , Excitatory Postsynaptic Potentials/drug effects , Excitatory Postsynaptic Potentials/physiology , Ion Channel Gating , Ion Channels/physiology , Male , Models, Neurological , Motor Neurons/drug effects , N-Methylaspartate/pharmacology , Potassium/metabolism , Rats , Rats, Wistar , Receptors, AMPA/physiology , Receptors, N-Methyl-D-Aspartate/physiology , Sodium/metabolism , Synapses/drug effects , Trigeminal Nerve/physiologyABSTRACT
A region of possible location of potassium-conducting synapses responsible for generation of "slow", or "long-term" IPSPs has been determined in computer experiments with the use of neuroscience-oriented software program CRONA on the basis of data of measurement of reversal potential of such IPSPs under natural experiments. Such geometrical parameters as dimensions of neuronal dendritic branches and intracellular potassium concentration have been studied for their effect on determination of the above-mentioned region using the results of natural experimental studies of interaction of long-term IPSPs with polarizing currents. It is shown that synaptic inputs under investigation have non-somatic location and the region of their location on apical dendrites is between 110 and 460 microns from the soma.