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confirmed Einstein's prediction of gravitational light deflection (see Doc. 151).
By employing finite-difference time-domain (FDTD) simulation, the light deflection phenomenon is realized.
For planar premixed flames, the relationship between light deflection and flame structure has been resolved analytically.
In this review the influence of temperature, natural convection and light deflection on the accuracy of the diffusion measurements is also discussed.
The location of the peak light deflection, and hence of the Schlieren image, depends on whether the flame front curvature is concave or convex toward the hot products.
By assigning the light deflection angle to each freeform surface, multiple surfaces can be obtained simultaneously by solving the corresponding equations, meanwhile the restricted angle on CF-LCoS is guaranteed.
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Palima, D. et al. Optical forces through guided light deflections.
An optically geometrical superposition of light deflections from the running crack and blasting waves is proposed, considering concave and convex lens effects of waviness of initially flat plane under blasting waves.
It is shown that use of holographic interferometry in the place of more traditional methods eliminates one type of error induced by light-deflection effects.
Experimental methods based on light beam deflection for the determination of surface stress change of electrodes are critically revisited.
To know some light actions (deflection, diffraction, and absorption) around this area, DIC observation was performed: when the background was darken by adjusting a DIC prism, the eye-spot area readily appeared as a bright spot, and removal of the DIC analyzer enhanced the brightness of the spot, indicating polarization of the transmitted light (see Results for details).
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