Download A numerical simulation model to facilitate the understanding by Eduardo E Zurek Affiliation: Departamento de Ingeniería de PDF
By Eduardo E Zurek Affiliation: Departamento de Ingeniería de Sistemas, Universidad del Norte, Km. 5 Vía a Puerto Colombia, Barranquilla, Colombia; Wilfrido A Moreno Affiliation: Electrical Engineering Department, University of South Florida, Tampa, FL 336
This paper introduces a brand new device to method the results of a diffraction grating and its interplay with different optical and digital parts in a mild wavelength research approach. The model's theoretical heritage is defined. This version is meant for tutorial reasons and it's mentioned a miniaturized spectrophotometer. © 2011 Wiley Periodicals, Inc. Comput Appl Eng Educ 22:187-194, 2014; View this article on-line at wileyonlinelibrary.com/journal/cae; DOI 10.1002/cae.20544 Read more...
summary: This paper introduces a brand new instrument to strategy the results of a diffraction grating and its interplay with different optical and digital elements in a gentle wavelength research procedure. The model's theoretical historical past is defined. This version is meant for academic reasons and it really is observed a miniaturized spectrophotometer. © 2011 Wiley Periodicals, Inc. Comput Appl Eng Educ 22:187-194, 2014; View this text on-line at wileyonlinelibrary.com/journal/cae; DOI 10.1002/cae.20544
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Additional resources for A numerical simulation model to facilitate the understanding of the properties of a diffraction grating
Since the two rays are orthogonally polarized, another polarizer P2 is used to make them interfere. The interference pattern consists of equally spaced straight fringes localized at infinity. The object is placed in the beam, and its refractive index and thickness variations introduce phase variations, which distort the fringes. A Savart plate introduces linear shear in a collimated beam. Usually, the incident beam has a small divergence. Savart plates can be modified to accept wider fields. However, with a spherical beam, linear shear can be introduced by a Wollaston prism.
Allen, Light with a twist in its tail, Contemp. , 41, 275–285, 2000. 9. P. Muys and E. Vandamme, Direct generation of Bessel beams, Appl. , 41, 6375–6379, 2002. 10. V. Garcés-Chávez, D. McGloin, H. Melville, W. Sibbett, and K. Dholakia, Simultaneous micromanipulation in multiple planes using a self-reconstructing light beam, Nature 419, 145–147, 2002. 11. Miguel A. Bandres, Julio C. Gutiérrez-Vega, and S. Chávez-Cerda, Parabolic nondiffracting optical wavefields, Opt. , 29, 44–46, 2004. 12. Carlos López-Mariscal, Julio C.
It also has a “healing” property in that it exhibits selfreconstruction after encountering an obstacle. A true Bessel beam, being unbounded, cannot be created. However, there are several practical ways to create a beam that is a close approximation to a true Bessel beam, including diffraction at an annular aperture, focusing by an axicon, and the use of diffractive elements (holograms). 4 shows a schematic for producing Bessel beam using an axicon. A Gaussian beam is incident on the axicon, which produces two plane waves in conical geometry.