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The Journal of Neurophysiology Vol. 82 No. 2 August 1999, pp. 829-840
Copyright ©1999 by the American Physiological Society
1Department of Physiology, University of Adelaide, South Australia 5005, Australia; and 2Department of Physiology and Biophysics, School of Medicine, University of Washington, Seattle, Washington 98195
Türker, K. S. and
R. K. Powers.
Effects of Large Excitatory and Inhibitory Inputs on Motoneuron
Discharge Rate and Probability. J. Neurophysiol. 82: 829-840, 1999. We elicited repetitive
discharge in hypoglossal motoneurons recorded in slices of rat brain
stem using a combination of a suprathreshold injected current step with
superimposed noise to mimic the synaptic drive likely to occur during
physiological activation. The effects of repetitive en mass stimulation
of afferent nerves were simulated by the further addition of trains of
injected current transients of varying shapes and sizes. The effects of a given current transient on motoneuron discharge timing and discharge rate were measured by calculating a peristimulus time histogram (PSTH)
and a peristimulus frequencygram (PSF). The amplitude and time course
of the simulated postsynaptic potentials (PSPs) produced by the current
transients were calculated by convolving the current transient with an
estimate of the passive impulse response of the motoneuron. We then
compared the shape of the injected current transient and the simulated
PSP to the profiles of the PSTH and the PSF records. The PSTHs produced
by excitatory PSPs (EPSPs) were characterized by a large, short-latency
increase in firing probability that lasted slightly longer than the
rising phase of the EPSP, followed by a reduced discharge probability
during the falling phase of the EPSP. In contrast, the PSF analysis
revealed a proportionate increase in discharge rate over the entire
profile of the EPSP, even though relatively few spikes occurred during the falling phase. The PSTHs associated with inhibitory PSPs (IPSPs) indicated a reduction in discharge probability during the initial, hyperpolarizing phase of the IPSP, followed by an increase in the
discharge probability during its subsequent repolarizing phase. Using
the PSF analysis, the initial phase of the IPSP appeared as a large
hole in the record where a very small number or no discharges occurred.
The subsequent phase of the IPSP was associated with frequency values
that were lower than the background values. The primary features of
both PSTHs and PSFs can be used to estimate the relative amplitudes of
the underlying EPSPs and IPSPs. However, PSTHs contain secondary peaks
and troughs that are not directly related to the underlying PSP but
instead reflect the regular recurrence of spikes following those
affected by the PSP. The PSF analysis is more useful for indicating the
total duration and the profile of the underlying PSP. The shape of the
underlying PSP can be obtained directly from the PSF records because
the discharge frequency of the spikes follow the PSPs very closely, especially for EPSPs.
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