The variable gain element of the vestibulo-ocular reflex is common to the optokinetic system of the cat.
The variable gain element of the vestibulo-ocular reflex is common to the optokinetic system of the cat.
复制标题
前庭眼反射的可变增益元件是猫的视动系统所共有的。
DOI:
10.1016/0006-8993(81)90740-x
复制
发表时间:
1981
期刊:
影响因子:
2.9
通讯作者:
Demer,JL
中科院分区:
文献类型:
--
作者:
Demer,JL
The gain (slow-phase eye velocity/head velocity) of the vestibulo-ocular reflex (VOR) of 6 alert cats was sequentially adapted to values between 0.2 and 1.66 by the chronic wearing of visual reversing or 2 X magnifying spectacles, combined with forced rotation in the light. Gain was measured during sinusoidal oscillation in darkness at 0.05 Hz at a peak velocity of about 30°/s. In each state of VOR gain adaptation, optokinetic nystagmus (OKN) and optokinetic afternystagmus (OKAN) were measured in a full-field optokinetic drum at velocities of 20-80°/s. Steady-state, slow-phase, optokinetic eye velocity nearly equaled low drum velocities, but saturated at higher velocities and declined when drum velocity further increased. The saturation velocity varied in relation to VOR gain, ranging from 20-20°/s at a VOR gain of 0.2–0.4, to 65°/s at a VOR gain of 1.66. This means that the variable gain element of the VOR is shared by the optokinetic system (OKS).OKAN, measured in darkness, had a roughly exponential decay. The time constant of OKAN (Tokan) also varied with VOR gain, ranging from about 2 s at a VOR gain of 0.2, to 10 s at a VOR gain of 1.66. This is a novel finding which suggests that the velocity-storage mechanism was also affected by gain changes. A model is proposed in which a neural, variable-gain element is located in a positive-feedback, velocity-storage loop common to both the VOR and the OKS. Computer simulation showed that this hypothesis could account for most of the observed changes in OKN saturation and TOKANwith changes in VOR gain. The model also predicts that low frequency VOR phase lead in darkness should increase with decreasing VOR gain. Experimental VOR phase lead at 0.05 Hz varied from about 10° for VOR gains above 1.1, to about 50° for VOR gains below 0.3. Such phase-lead data agree with the trend predicted by the model.