S. A. Korol’kov, Yu. S. Kuz'minov, A. V. Mamaev, V. Shkunov, A. Zozulya
{"title":"Spatial Structure of Scattered Radiation in a Self-Pumped Photorefractive Passive Ring Mirror","authors":"S. A. Korol’kov, Yu. S. Kuz'minov, A. V. Mamaev, V. Shkunov, A. Zozulya","doi":"10.1364/JOSAB.9.000664","DOIUrl":null,"url":null,"abstract":"We present detailed experimental investigation of scattered radiation spatial structure in the geometry of a transmission grating photorefractive passive ring mirror (Fig. 1) and compare our results with the predictions of Ref.[1]. According to the theory, behaviour of a ring mirror in the limit of large Fresnel numbers is determined by two scale variation coefficients: α// and α⊥. Scale variation coefficient α// is the ratio of the width of the pumping beam 4 in the plane of intersection to that of the pumping beam 2 (see Fig. 1). For | α// | <1 beam 4 is narrower and for | α// | >1 wider, than beam 2. The same with the scale variation coefficient α⊥, but for the direction, perpendicular to the intersection plane.","PeriodicalId":355924,"journal":{"name":"Photorefractive Materials, Effects, and Devices","volume":"78 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1992-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"14","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Photorefractive Materials, Effects, and Devices","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/JOSAB.9.000664","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 14
Abstract
We present detailed experimental investigation of scattered radiation spatial structure in the geometry of a transmission grating photorefractive passive ring mirror (Fig. 1) and compare our results with the predictions of Ref.[1]. According to the theory, behaviour of a ring mirror in the limit of large Fresnel numbers is determined by two scale variation coefficients: α// and α⊥. Scale variation coefficient α// is the ratio of the width of the pumping beam 4 in the plane of intersection to that of the pumping beam 2 (see Fig. 1). For | α// | <1 beam 4 is narrower and for | α// | >1 wider, than beam 2. The same with the scale variation coefficient α⊥, but for the direction, perpendicular to the intersection plane.