Neural Comp. NEW Faster Access
HOME HELP FEEDBACK SUBSCRIPTIONS ARCHIVE SEARCH TABLE OF CONTENTS
 QUICK SEARCH:   [advanced]


     


This Article
Right arrow Full Text
Right arrow Full Text (PDF)
Right arrow Alert me when this article is cited
Right arrow Alert me if a correction is posted
Services
Right arrow Similar articles in this journal
Right arrow Similar articles in PubMed
Right arrow Alert me to new issues of the journal
Right arrow Download to citation manager
Right arrow reprints & permissions
Citing Articles
Right arrow Citing Articles via HighWire
Right arrow Citing Articles via Google Scholar
Google Scholar
Right arrow Articles by Mo, C.-H.
Right arrow Articles by Koch, C.
Right arrow Search for Related Content
PubMed
Right arrow PubMed Citation
Right arrow Articles by Mo, C.-H.
Right arrow Articles by Koch, C.
(Neural Computation. 2003;15:735-759.)
© 2003 The MIT Press

Modeling Reverse-Phi Motion-Selective Neurons in Cortex: Double Synaptic-Veto Mechanism

Chun-Hui Mo

mo{at}klab.caltech.edu, Division of Biology, and Division of Chemistry, California Institute of Technology, Pasadena, CA 91125, U.S.A.

Christof Koch

koch{at}klab.caltech.edu, Division of Biology, Division of Engineering and Applied Science, California Institute of Technology, Pasadena, CA 91125, U.S.A.

Reverse-phi motion is the illusory reversal of perceived direction of movement when the stimulus contrast is reversed in successive frames. Livingstone, Tsao, and Conway (2000) showed that direction-selective cells in striate cortex of the alert macaque monkey showed reversed excitatory and inhibitory regions when two different contrast bars were flashed sequentially during a two-bar interaction analysis. While correlation or motion energy models predict the reverse-phi response, it is unclear how neurons can accomplish this. We carried out detailed biophysical simulations of a direction-selective cell model implementing a synaptic shunting scheme. Our results suggest that a simple synaptic-veto mechanism with strong direction selectivity for normal motion cannot account for the observed reverse-phi motion effect. Given the nature of reverse-phi motion, a direct interaction between the ON and OFF pathway, missing in the original shunting-inhibition model, it is essential to account for the reversal of response. We here propose a double synaptic-veto mechanism in which ON excitatory synapses are gated by both delayed ON inhibition at their null side and delayed OFF inhibition at their preferred side. The converse applies to OFF excitatory synapses. Mapping this scheme onto the dendrites of a direction-selective neuron permits the model to respond best to normal motion in its preferred direction and to reverse-phi motion in its null direction. Two-bar interaction maps showed reversed excitation and inhibition regions when two different contrast bars are presented.




This article has been cited by other articles:


Home page
J. Neurophysiol.Home page
B. Krekelberg and T. D. Albright
Motion Mechanisms in Macaque MT
J Neurophysiol, May 1, 2005; 93(5): 2908 - 2921.
[Abstract] [Full Text] [PDF]


Home page
Neural Comput.Home page
C.-H. Mo, M. Gu, and C. Koch
A Learning Rule for Local Synaptic Interactions Between Excitation and Shunting Inhibition
Neural Comput., December 1, 2004; 16(12): 2507 - 2532.
[Abstract] [Full Text] [PDF]




HOME HELP FEEDBACK SUBSCRIPTIONS ARCHIVE SEARCH TABLE OF CONTENTS
J COGNITIVE NEUROSCIENCE NEURAL COMPUTATION MIT PRESS JOURNALS
Copyright © 2003 by The MIT Press.