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A model of high-frequency oscillatory potentials in retinal ganglion cells

Published online by Cambridge University Press:  22 January 2004

GARRETT T. KENYON
Affiliation:
P-21, Biophysics, Los Alamos National Laboratory, Los Alamos
BARTLETT MOORE
Affiliation:
P-21, Biophysics, Los Alamos National Laboratory, Los Alamos Department of Neurobiology and Anatomy, University of Texas Medical School, Houston
JANELLE JEFFS
Affiliation:
P-21, Biophysics, Los Alamos National Laboratory, Los Alamos Department of Bioengineering, University of Utah, Salt Lake City
KATE S. DENNING
Affiliation:
P-21, Biophysics, Los Alamos National Laboratory, Los Alamos
GREG J. STEPHENS
Affiliation:
P-21, Biophysics, Los Alamos National Laboratory, Los Alamos
BRYAN J. TRAVIS
Affiliation:
EES-6, Hydrology, Geochemistry, and Geology, Los Alamos National Laboratory, Los Alamos
JOHN S. GEORGE
Affiliation:
P-21, Biophysics, Los Alamos National Laboratory, Los Alamos
JAMES THEILER
Affiliation:
NIS-2, Space and Remote Sensing Sciences, Los Alamos National Laboratory, Los Alamos
DAVID W. MARSHAK
Affiliation:
Department of Neurobiology and Anatomy, University of Texas Medical School, Houston

Abstract

High-frequency oscillatory potentials (HFOPs) have been recorded from ganglion cells in cat, rabbit, frog, and mudpuppy retina and in electroretinograms (ERGs) from humans and other primates. However, the origin of HFOPs is unknown. Based on patterns of tracer coupling, we hypothesized that HFOPs could be generated, in part, by negative feedback from axon-bearing amacrine cells excited via electrical synapses with neighboring ganglion cells. Computer simulations were used to determine whether such axon-mediated feedback was consistent with the experimentally observed properties of HFOPs. (1) Periodic signals are typically absent from ganglion cell PSTHs, in part because the phases of retinal HFOPs vary randomly over time and are only weakly stimulus locked. In the retinal model, this phase variability resulted from the nonlinear properties of axon-mediated feedback in combination with synaptic noise. (2) HFOPs increase as a function of stimulus size up to several times the receptive-field center diameter. In the model, axon-mediated feedback pooled signals over a large retinal area, producing HFOPs that were similarly size dependent. (3) HFOPs are stimulus specific. In the model, gap junctions between neighboring neurons caused contiguous regions to become phase locked, but did not synchronize separate regions. Model-generated HFOPs were consistent with the receptive-field center dynamics and spatial organization of cat alpha cells. HFOPs did not depend qualitatively on the exact value of any model parameter or on the numerical precision of the integration method. We conclude that HFOPs could be mediated, in part, by circuitry consistent with known retinal anatomy.

Type
Research Article
Copyright
2003 Cambridge University Press

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