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Then, random lasers with linear polarization from both the forward and backward surface of the DDNLC cells were observed.
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.
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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.
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.
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.
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.
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.
The needle is moved forward and backward, sliding on the surface of the supraspinatus muscle-tendon fascia along the subacromial space and under the acromioclavicular joint until no resistance is felt at the tip of the needle.
In the case of a spherical obstacle, the point at which the boundary layer separates from the rear surface of the sphere shifts backward when the boundary layer becomes turbulent, away from the equator Q in Figure 15 and toward P′, and the eddies attached to the sphere therefore become smaller.
The extreme surface expansion and pressures observed during the backward cup extrusion process can adversely affect the surface of the work-piece and diminish the life of the punches.
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