{"title":"SELF-IMAGING OF THREE-DIMENSIONAL PHASE GRATINGS","authors":"M. Carbon, N. Lauinger, J. Schwab","doi":"10.1088/0963-9659/7/5/017","DOIUrl":null,"url":null,"abstract":"We present a general solution of the wave equation, obtained by the four-dimensional spectral method, for diffraction of a plane monochromatic light wave by a three-dimensional (3D) phase grating layer of finite thickness. As an example, we consider spherical particles in 3D phase gratings with orthogonal and hexagonal geometry. Conditions for the strong self-imaging of a 3D grating layer and for the weak self-imaging of a two-dimensional (2D) grating are formulated and investigated. Intensity distributions for diffracted light in planes of positive and negative self-imaging and in a plane of lowest contrast are computed and compared for 2D and 3D gratings. Some aspects of the Talbot and Lau effects for 2D and 3D phase gratings are discussed.","PeriodicalId":20787,"journal":{"name":"Pure and Applied Optics: Journal of The European Optical Society Part A","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"1998-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Pure and Applied Optics: Journal of The European Optical Society Part A","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1088/0963-9659/7/5/017","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
We present a general solution of the wave equation, obtained by the four-dimensional spectral method, for diffraction of a plane monochromatic light wave by a three-dimensional (3D) phase grating layer of finite thickness. As an example, we consider spherical particles in 3D phase gratings with orthogonal and hexagonal geometry. Conditions for the strong self-imaging of a 3D grating layer and for the weak self-imaging of a two-dimensional (2D) grating are formulated and investigated. Intensity distributions for diffracted light in planes of positive and negative self-imaging and in a plane of lowest contrast are computed and compared for 2D and 3D gratings. Some aspects of the Talbot and Lau effects for 2D and 3D phase gratings are discussed.