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Based on minimization of radiant power of light, we found that, by utilizing the spontaneous shear effect, a liquid crystalline orientation with a tilted angle to the beam axis can be energetically more favorable than the most studied planar alignment.
Stretching of the GUV along the beam axis can be clearly observed.
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Scanning the sample beam along a transverse axis can be performed to create a B-scan image and obtain two-, three-, and four-dimensional data arrays.
Beam rotation around its wave propagation axis can be achieved by varying ϕ0.
In reinforced concrete beams, less stressed concrete near neutral axis can be replaced by some light weight material like bricks to reduce the weight of the structure and also achieve the economy.
The typical shape of the RPO beam with the null electrical field at the axis can be visualized clearly in Fig. 1(a) (calculated at λ = 532 nm).
The extension of the usable light sheet along the illumination axis can be defined by twice the Rayleigh length of the Gaussian beam, so that the field of view for optimal contrast was approximately 84 µm×20 µm.
The separation of the axis label from the axis can be changed, as in Figure 17.
The axis can be turned via an externally positioned crank.
As shown in Fig. 3d, the deflection angle information of the incident light beams along the x-axis and the y-axis can be calculated by the distance between of light spot on the x-axis and the y-axis based on the related model between the angle and the change of the spot.
While higher on axis beam density can be achieved (better beam collimation), the beam temperatures are usually higher too (~10°K).
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