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In particular, it is shown that in some cases large input to the photoemission efficiency arises from collection of photoelectrons by backward surface of the satellite.
Then, random lasers with linear polarization from both the forward and backward surface of the DDNLC cells were observed.
In contrast, Parkinsonian subjects coactivate proximal muscles on the ventral side of the body (QUAD-ABD) with backward surface translation, and on dorsal side of the body (PSP and HAM) with forward surface translation.
A later study aimed to evaluate the effects of parkinsonism and of dopamine replacement therapy on the scaling of automatic postural responses based on peripheral sensory information and on central set, compared measures of surface reactive torques and EMG activity in response to backward surface translations in Parkinsonian patients and elderly controls [ 44].
The ability to quickly change the postural set was inferred by comparing leg muscle activity under two conditions of support (free stance versus grasping a frame, or sitting) during backward surface translations, during toes up surface rotations, and during voluntary rise to toes.
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By using different rubbing methods on the light-emitting sides, random laser with different polarization directions can be obtained from both forward and backward surfaces of one cell at the same time.
Random lasers with linear polarization can be obtained from both forward and backward surfaces of the DDNLC cells and the polarization direction is along the rubbing direction of the light-emitting side.
Here, the A and B models are used to identify the vertical adsorption of N2O gas from the O side and N side on the outer surface of nanotube, respectively, whereas the C and D models are used to show the horizontal adsorption of N2O gas on the forward and backward surfaces of nanotube, respectively.
Through constructing cells with different rubbing methods on the forward and backward surfaces of light-emitting sides, we can get two random laser beams with different polarization directions from one DDNLC cell at the same time, and the polarization direction is along the rubbing direction of the light-emitting sides.
So, it can be concluded that the polarization direction of random lasers from DDNLC cells is influenced by the rubbing methods and is always along the rubbing direction of the light-emitting side for both forward and backward surfaces of the cells.
The compensation of the desired coordinate is carried through a nested backward sliding surface design, which compensates some of the non-actuated state components, while the remaining states are maintained to be bounded.
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