Stationary optical wave fields with arbitrary longitudinal shape by superposing equal frequency Bessel beams: Frozen Waves

dc.creatorZamboni-Rached, M
dc.date2004
dc.dateAUG 23
dc.date2014-11-14T07:13:34Z
dc.date2015-11-26T16:05:12Z
dc.date2014-11-14T07:13:34Z
dc.date2015-11-26T16:05:12Z
dc.date.accessioned2018-03-28T22:54:11Z
dc.date.available2018-03-28T22:54:11Z
dc.identifierOptics Express. Optical Soc Amer, v. 12, n. 17, n. 4001, n. 4006, 2004.
dc.identifier1094-4087
dc.identifierWOS:000223469000016
dc.identifier10.1364/OPEX.12.004001
dc.identifierhttp://www.repositorio.unicamp.br/jspui/handle/REPOSIP/74572
dc.identifierhttp://www.repositorio.unicamp.br/handle/REPOSIP/74572
dc.identifierhttp://repositorio.unicamp.br/jspui/handle/REPOSIP/74572
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/1265644
dc.descriptionIn this paper it is shown how one can use Bessel beams to obtain a stationary localized wave field with high transverse localization, and whose longitudinal intensity pattern can assume any desired shape within a chosen interval 0 less than or equal to z less than or equal to L of the propagation axis. This intensity envelope remains static, i.e., with velocity v = 0; and because of this we call "Frozen Waves" the new solutions to the wave equations (and, in particular, to the Maxwell equations). These solutions can be used in many different and interesting applications, such as optical tweezers, atom guides, optical or acoustic bistouries, various important medical purposes, etc. (C) 2004 Optical Society of America.
dc.description12
dc.description17
dc.description4001
dc.description4006
dc.languageen
dc.publisherOptical Soc Amer
dc.publisherWashington
dc.publisherEUA
dc.relationOptics Express
dc.relationOpt. Express
dc.rightsaberto
dc.sourceWeb of Science
dc.titleStationary optical wave fields with arbitrary longitudinal shape by superposing equal frequency Bessel beams: Frozen Waves
dc.typeArtículos de revistas


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