Type, Ul (x, y) is definitely the amplitude from the lth la u = (cos )/, v = (cos )/ (8) the distance in between the lth layer along with the holographic plane, would be the wavelengt where FT represents frequencies, and and y) will be the amplitude with the lth the incident w v are the spatial the Fourier transform, Ul (x, are the angles among layer, zl will be the distance involving the lth layer and the holographic plane, is the wavelength, u the x- and y-directions, respectively. As this study uses a phase-only spatial ligh and v are the spatial frequencies, and and would be the angles amongst the incident wave lator (SLM), y-directions, respectively. As this (x, y) really should be extracted from as well as the x- along with the phase-only distribution Epstudy utilizes a phase-only spatial lightEcom (x, y modulator (SLM), the phase-only distribution Ep (x, y) need to be extracted from Ecom (x, y) tion (7)).(Equation (7)).3.2. MCC950 Technical Information reconstruction of CGHs3.two. Reconstruction the effectiveness To verify of CGHsof the 2D-to-3D rendering strategy in practicalTo we constructed a phase-only 2D-to-3D rendering approach in sensible applications, tions, confirm the effectiveness of theholographic Decanoyl-L-carnitine Autophagy display technique, as shown in Figure three. we built a phase-only holographic display technique, as shown in Figure 3. The illumination mination laser beam was filtered by a pinhole and collimated by a lens. The CGH laser beam was filtered by a pinhole and collimated by a lens. The CGH of was uploaded uploaded on a phase-only SLM. The SLM employed within the program was a on a phase-only SLM. The SLM employed in the method was a Holoeye Gaea-2 VIS. AfterHoloey VIS. Soon after being modulated SLM, the reconstructed SLM, the reconstructed becoming modulated by the CGH on theby the CGH on the wavefront was captured by a wavefr Canon 60D digitalCanon 60D digital camera. captured by a camera.Figure three. The phase-only holographic show Figure 3. The phase-only holographic show system.technique.In the experimental technique, the illumination wavelength, pixel pitch, and resolution in the CGH are 532 nm, 3.74 and 2000 2000, respectively. Throughout the experiments, the camera is placed at shooting distances of 155, 160, 165, and 170 mm, respectively. The captured outcomes are shown in Figure 4. When the shooting distance is 155 mm, the a part of the reconstruction that may be nearest to the camera is clear, although the distant component is blurred. Because the shooting distance varies, the focus position of your reconstruction also modifications. Therefore, a 3D effect may be obtained employing CGDMs within this 2D-to-3D rendering method.Appl. Sci. 2021, 11,In the experimental system, the illumination wavelength, pixel pitch, and resolution of the CGH are 532 nm, 3.74 m and 2000 2000, respectively. During the experiments, the camera is placed at shooting distances of 155, 160, 165, and 170 mm, respectively. The captured benefits are shown in Figure 4. When the shooting distance is 155 mm, the part of the reconstruction which is nearest for the camera is clear, though the distant component is blurred. 6 of 9 As the shooting distance varies, the concentrate position in the reconstruction also changes. Therefore, a 3D impact may be obtained applying CGDMs in this 2D-to-3D rendering approach.Figure 4. Reconstructions of 3D scenes by 2D-to-3D rendering technique at depths of 155 mm, 160 mm, Figure 4. Reconstructions of 3D scenes by 2D-to-3D rendering method at depths of 155mm, 160mm, 165 mm and 170 mm, respectively. 165mm and 170mm, respectively.Appl. Sci. 2021, 11,4. Discussion four. Discussion In Figure 5a, objects A and B ar.
