Influence of Plate Mode Structure and Gaussian Beam Profile Characteristics on Ultrasonic Reflection and Transmission

1982 ◽  
Vol 29 (2) ◽  
pp. 112-114 ◽  
Author(s):  
T.D.K. Ngoc ◽  
W.G. Mayer
1974 ◽  
Vol 52 (11) ◽  
pp. 962-972 ◽  
Author(s):  
Yahia M. Antar ◽  
Wolfgang M. Boerner

The problem of electromagnetic Gaussian beam scattering from a planar interface separating two lossless dielectric media is considered. Employing a modal plane wave expansion and the continuity of the fields across the boundary, the reflected and transmitted beams are obtained using the Fresnel approximation, and a Taylor series expansion of the reflection and transmission coefficients, for both polarizations. Particular emphasis is given to the beam shift of both the reflected and refracted beams, the change in width of the transmitted beam, and the behavior at polarizing incidence.


2001 ◽  
Author(s):  
Alexander A. Serafetinides ◽  
Giorgos Chourdakis ◽  
Dimitris N. Papadopoulos ◽  
Kenneth R. Rickwood

2021 ◽  
Vol 0 (0) ◽  
Author(s):  
Shwetabh Verma ◽  
Juergen Hesser ◽  
Samuel Arba-Mosquera

Abstract Smoother surfaces after laser vision correction have been widely accepted as a factor for improving visual recovery regardless of the used technique (PRK, LASIK, or even SMILE). We tested the impact of laser beam truncation, dithering (expressing a continuous profile on a basis of lower resolution causing pixels to round up/down the number of pulses to be placed), and jitter (a controlled random noise (up to ±20 µm in either direction) added to the theoretical scanner positions) on residual smoothness after Poly(methyl methacrylate) (PMMA) ablations, using a close-to-Gaussian beam profile. A modified SCHWIND AMARIS system has been used providing a beam profile with the following characteristics: close-to-Gaussian beam profile with full width at half maximum (FWHM) of 540 µm, 1050 Hz. Laser parameters have been optimized following Invest. Ophthalmol. Vis. Sci., vol. 58, no. 4, pp. 2021–2037, 2017, the pulse energy has been optimized following Biomed. Opt. Express vol. 4, pp. 1422–1433, 2013. For the PMMA ablations, two configurations (with a 0.7 mm pinhole and 0.75 mJ and without pinhole and 0.9 mJ (for fluences of 329 mJ/cm2 and 317 mJ/cm2 and corneal spot volumes of 174 and 188 pl)) were considered, along with two types of lattices (with and without ordered dithering to select the optimum pulse positions), and two types of spot placement (with and without jitter). Real ablations on PMMA (ranging from −12D to +6D with and without astigmatism of up to 3D) completed the study setup. The effect of the 2 × 2 × 2 different configurations was analyzed based on the roughness in ablation estimated from the root mean square error in ablation. Truncation of the beam is negatively associated to a higher level of residual roughness; ordered dithering to select the optimum pulse positions is positively associated to a lower level of residual roughness; jitter is negatively associated to a higher level of residual roughness. The effect of dithering was the largest, followed by truncation, and jitter had the lowest impact on results. So that: Dithering approaches help to further minimize residual roughness after ablation; minimum (or no) truncation of the beam is essential to minimize residual roughness after ablation; and jitter shall be avoided to minimize residual roughness after ablation. The proposed model can be used for optimization of laser systems used for ablation processes at relatively low cost and would directly improve the quality of results. Minimum (or no) truncation of the beam is essential to minimize residual roughness after ablation. Ordered dithering without jitter helps to further minimize residual roughness after ablation. Other more complex dithering approaches may further contribute to minimize residual roughness after ablation.


Author(s):  
Matthias Wohlmuth ◽  
Konrad Altmann ◽  
Michaël Hemmer ◽  
Mario Goehre ◽  
Christoph Pflaum ◽  
...  

2000 ◽  
Vol 9 (1) ◽  
pp. 65-68 ◽  
Author(s):  
Yao Xin-cheng ◽  
Li Zhao-lin ◽  
Cheng Bing-ying ◽  
Han Xue-hai ◽  
Zhang Dao-zhong

2000 ◽  
Author(s):  
Loic M. A. Plouzennec ◽  
Laurence J. Sargent ◽  
Richard V. Penty ◽  
Ian H. White ◽  
Peter J. Heard ◽  
...  

2014 ◽  
Vol 22 (3) ◽  
pp. 3705 ◽  
Author(s):  
Mingjun Wang ◽  
Huayong Zhang ◽  
Guosheng Liu ◽  
Yingle Li ◽  
Qunfeng Dong

2013 ◽  
Vol 291 ◽  
pp. 31-37 ◽  
Author(s):  
Wei Wen ◽  
Gaofeng Wu ◽  
Kehui Song ◽  
Yiming Dong
Keyword(s):  

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