Although this rearrangement was observed both along the dorsomedial-ventrolateral and outer-inner axes in the dLGN, it occurred more rapidly along the outer-inner axis.
Interestingly, we found that the rearrangement along the outer-inner axis (O-I axis), which is the axis perpendicular to the surface of the dLGN [21], [22], occurred more quickly than that along the dorsomedial-ventrolateral axis (DM-VL axis), the axis roughly in parallel to the surface of the dLGN [23].
Finally, comparable experiments are carried out to verify the application of the proposed approach to an inner-axis driven by a direct current (DC) torque motor through extra-low speed servo for a high precision flight simulator, and the axis works under deteriorating conditions such as periodically fluctuating torques of motor, nonlinear friction, and time-varying model parameters.
The polyaxial bushing can be laterally rotated up to 5°, which together with the 10° eccentric angle of its inner thread axis can increase angular regulation amplitude for the locking screw up to 30°.
This observation led Al-Awqati and Schwartz to propose a "kidney-inner ear axis" model to highlight the strikingly conserved mechanism of foxi1 for kidney and inner ear differentiation [2].
In the following Myr, the system circularizes and the semimajor-axis decreases by a factor 2. After synchronisation and circularisation has been reached, the inner semimajor-axis increases due to the ejection of stellar winds.
The evolution of the inner semimajor-axis on the same timescale as Figure 9 and 10.
The inner semimajor-axis even increases from 6.0 to 7.3 AU.
However, polymerization produced decreases in deuteration mainly localized to the "inner", filament-axis side as predicted by the Holmes model.
In the first Myr, the evolution of the system is dominated by the Lidov-Kozai mechanism and the inner semimajor-axis remains more or less constant.
