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The Journal of Neurophysiology Vol. 87 No. 6 June 2002, pp. 2778-2789
Copyright ©2002 by the American Physiological Society
Departments of 1Bioengineering and Physiology and 2Biophysics and 3Regional Primate Research Center, University of Washington, Seattle, Washington 98195
Soetedjo, Robijanto,
Chris R. S. Kaneko, and
Albert F. Fuchs.
Evidence Against a Moving Hill in the Superior Colliculus During
Saccadic Eye Movements in the Monkey. J. Neurophysiol. 87: 2778-2789, 2002. Saccadic eye movements of
different sizes and directions are represented in an orderly
topographic map across the intermediate and deep layers of the superior
colliculus (SC), where large saccades are encoded caudally and small
saccades rostrally. Based on experiments in the cat, it has been
suggested that saccades are initiated by a hill of activity at the
caudal site appropriate for a particular saccade. As the saccade
evolves and the remaining distance to the target, the motor error,
decreases, the hill moves rostrally across successive SC sites
responsible for saccades of increasingly smaller amplitudes. When the
hill reaches the "fixation zone" in the rostral SC, the saccade is
terminated. A moving hill of activity has also been posited for the
monkey, in which it is supposed to be transported via so-called
build-up neurons (BUNs), which have a prelude of activity that
culminates in a burst for saccades. However, several studies using a
variety of approaches have yet to provide conclusive evidence for or
against a moving hill. The moving hill scenario predicts that during a
large saccade the burst of a BUN in the rostral SC will be delayed
until the motor error remaining in the evolving saccade is equal to the saccadic amplitude for which that BUN discharges best, i.e., its optimal amplitude. Therefore a plot of the burst lead preceding the
"optimal" motor error against the time of occurrence of the optimal
motor error should have a slope of zero. A slope of
1 indicates no
moving hill. For our 20 BUNs, we used three measures of burst timing:
the leads to the onset, peak, and center of the burst. The average
slopes of these relations were
1.09,
0.79, and
0.58,
respectively. For individual BUNs, the slopes of all three relations
always differed significantly from zero. Although the peak and center
leads fall between
1 and 0, a hill of activity moving rostrally at a
rate indicated by either of these slopes would arrive at the fixation
zone much too late to terminate the saccade at the appropriate time.
Calculating our same three timing measures from averaged data leads us
to the same conclusion. Thus our data do not support the moving hill
model. However, we argue in the DISCUSSION that the
constant lead of the burst onset relative to saccade onset (~27 ms)
suggests that the BUNs may help to trigger the saccade.
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